morphology and surface properties of carbonizates (c/sic...

14
Composite Interfaces, Vol. 12, No. 5, pp. 459–472 (2005) VSP 2005. Also available online - www.vsppub.com Morphology and surface properties of carbonizates (C/SiC nanocomposites) obtained via pyrolysis of a coal tar pitch modified with selected silicon-bearing precursors CEZARY CZOSNEK, MARIUSZ DRYGA ´ S and JERZY F. JANIK AGH University of Science and Technology, Faculty of Fuels and Energy, Al. Mickiewicza 30, 30-059 Kraków, Poland Received 8 February 2005; accepted 1 March 2005 Abstract—Morphology of carbon-based composite materials obtained from pyrolysis of a coal tar pitch admixed with selected silicon-bearing additives is discussed based on SEM/EDX observations, mercury porosimetry, BET surface area determinations, and helium density data. The silicon precursors used in the study included elemental silicon Si, silica SiO 2 , poly(carbomethylsilane) { CH 2 SiH(CH 3 ) } n , and commercial SiC. Each individual binary mixture, i.e. pitch/silicon additive, was first repeatedly homogenized at 160 C in the liquid medium of the molten pitch followed by carbonization at 500 C. In all cases, one part of the initial 500 C solid carbonizate was further pyrolyzed at 1300 C and another part at 1650 C under an argon flow resulting in nanocomposite products C/SiC. Differences in properties and morphology of the products were linked to specific chemical changes taking place in the reaction systems. Keywords: Pitch; carbon materials; nanomaterials; silicon carbide; SiC; composites. 1. INTRODUCTION Because of its robust chemical, thermal and mechanical properties, silicon carbide SiC has found numerous technological applications. For example, in electronics many of the compound’s uses rely on its semiconducting properties while, simul- taneously, exploiting advantageous thermal and chemical resistance at high tem- peratures [1, 2]. By the same token, SiC has been introduced as a modifier to a group of carbon/graphite materials where its significant resistance to oxidation and thermal shocks coupled with a low thermal expansion coefficient are utilized to improve the performance and lifetime of blast-furnace carbon/graphite linings in metallurgy [3, 4]. To whom correspondence should be addressed. E-mail: [email protected]

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Composite Interfaces Vol 12 No 5 pp 459ndash472 (2005) VSP 2005Also available online - wwwvsppubcom

Morphology and surface properties of carbonizates (CSiCnanocomposites) obtained via pyrolysis of a coal tar pitchmodified with selected silicon-bearing precursors

CEZARY CZOSNEK MARIUSZ DRYGAS and JERZY F JANIK lowast

AGH University of Science and Technology Faculty of Fuels and Energy Al Mickiewicza 3030-059 Krakoacutew Poland

Received 8 February 2005 accepted 1 March 2005

AbstractmdashMorphology of carbon-based composite materials obtained from pyrolysis of a coal tarpitch admixed with selected silicon-bearing additives is discussed based on SEMEDX observationsmercury porosimetry BET surface area determinations and helium density data The siliconprecursors used in the study included elemental silicon Si silica SiO2 poly(carbomethylsilane) CH2 SiH(CH3) n and commercial SiC Each individual binary mixture ie pitchsiliconadditive was first repeatedly homogenized at 160C in the liquid medium of the molten pitch followedby carbonization at 500C In all cases one part of the initial 500C solid carbonizate was furtherpyrolyzed at 1300C and another part at 1650C under an argon flow resulting in nanocompositeproducts CSiC Differences in properties and morphology of the products were linked to specificchemical changes taking place in the reaction systems

Keywords Pitch carbon materials nanomaterials silicon carbide SiC composites

1 INTRODUCTION

Because of its robust chemical thermal and mechanical properties silicon carbideSiC has found numerous technological applications For example in electronicsmany of the compoundrsquos uses rely on its semiconducting properties while simul-taneously exploiting advantageous thermal and chemical resistance at high tem-peratures [1 2] By the same token SiC has been introduced as a modifier to agroup of carbongraphite materials where its significant resistance to oxidation andthermal shocks coupled with a low thermal expansion coefficient are utilized toimprove the performance and lifetime of blast-furnace carbongraphite linings inmetallurgy [3 4]

lowastTo whom correspondence should be addressed E-mail janikjuciaghedupl

460 C Czosnek et al

Depending on the mode of SiC incorporation into a materialrsquos structure and onthe type of applied silicon precursor polycrystalline SiC with a range of crystallitesizes can be formed in the pores of carbon matrix [3] or a thin protective SiC layercan be produced on carbon grain surfaces [5] It is worth pointing out also thatnanosized SiC may improve properties of such CSiC composite materials [6ndash8]That is mostly why significant research efforts have recently been undertaken inthe area of utilization of various silicon-bearing precursors as modifiers for carbonmaterials [9ndash19] that supplement the known method of using elemental silicon asa molten saturating agent for making SiC in porous carbons [11ndash13] similarlyCVD methods of preparing SiC films have also shown to be promising in somecases [5 15]

In order to achieve highly homogeneous distribution of SiC nanocrystallites ina modified carbon matrix special and usually troublesome procedures alreadyduring initial preparation of precursors are required In this regard all methodsfor manufacturing carbongraphite materials that employ mixtures of solid carbonprecursors and low melting coal tar or petroleum pitch binders are especiallywell suited for efficient mixinghomogenization since one can utilize potentiallyadvantageous pre-modifications of the pitch with a silicon precursor in the liquidphase

The authors of this study have recently reported the investigations of various pitchsilicon precursors that provided an insight into thermally promoted conversion of theprecursors in the matrix of simultaneously carbonized pitch toward nanocompositesCSiC [20ndash22] In the current report major applicable properties of the CSiC com-posites and particularly morphology and surface development are discussed

2 EXPERIMENTAL

The target products included carbon materials prepared by thermal treatment (car-bonization pyrolysis) under an argon atmosphere at final temperatures of 1300Cor 1650C of a typical coal tar pitch binder (softening point by Mettler 1015Ctoluene insolubles 209) that was individually pre-modifiedmixed with selectedsilicon-bearing precursors The following powdered silicon precursors were used(Aldrich) elemental Si (lt325 mesh) silica SiO2 (lt325 mesh) commercial SiC(lt400 mesh) and poly(carbomethylsilane) CH2 SiH(CH3) n (av molecu-lar weight 800 mp 79C) Comparable reference carbonizates were also pre-pared from a pure non-modified pitch After repeated mixinghomogenization ofthe components at 160C in the liquid medium of the molten pitch the substratemixtures were pyrolyzed at 500C under an argon atmosphere to afford initial solidcarbonizates for further pyrolysis at the final temperature of 1300C or 1650C Adetailed description of the preparation and materials spectroscopic characterizationis provided elsewhere [20 21 23]

The composite CSiC materials were characterized with (i) BET surface areasderived from standard low temperature nitrogen adsorption measured with Mi-

Properties of carbonizates 461

cromeritics Gemini 2360 (ii) helium density measurements with Micromeritics Ac-cuPyc (fivefold helium purging) and (iii) mercury intrusion porosimetry carried outwith Porosimeter 2000 by Carlo Erba Instruments (pressures from 1 atm to 2000 atmcorresponding to approx 15 000 nm to 75 nm pore diameter range respectively)additionally (iv) SEM images were acquired with JSM 5400 Jeol scanning electronmicroscope (20 kV accelerating voltage samples coated with Au) equipped withmicroprobe Link Isis 300 for intentionally preserved chunks of the materials ofapprox 10 mm in size

3 RESULTS AND DISCUSSION

Table 1 includes the results of helium density and BET surface area determinationsfor all composites The density data indicate basically similar values for samples A(pitchSi) B (pitchSiO2) and C (pitchcommercial SiC) with the higher densitiesobserved for the 1650C carbonizates (237ndash243 gcm3) relative to the respective1300C carbonizates (215ndash228 gcm3) These values have to be compared withthe literature density data for graphite 226 gcm3 and SiC 321 gcm3 and theyall are higher than the densities measured for both carbonizates from the purepitch ie 204ndash209 gcm3 (sample E) The latter observation can be explainedby virtue of the composites containing either (i) yet unreacted or partially reactedheavy silicon precursors in the presumed Si O C assemblages in relevant systemsafter pyrolysis at 1300C or (ii) prevailing regular β-SiC formed upon the 1650Ctreatment in all systems The various structural forms of transient and final siliconspecies evolving in the pyrolyzed carbon matrix were previously described for thesesystems [20]

Compared with the above the densities for sample D (pitchpoly(carbomethylsi-lane)) 176ndash183 gcm3 appear to be outstandingly lower even in relation to therespective values for the carbonizates from the pure pitch (sample E) Such low

Table 1Helium densities dHe and BET surface areas SBET of composites obtained from the systems Apitchelemental Si B pitchSiO2 C pitchcommercial SiC D pitchpoly(carbomethylsilane) E purenonmodified pitch

Sample dHe (gcm3) SBET (m2g)

1300C 1650C 1300C 1650C

A 215 243 14 20B 218 244 40 83C 228 237 04 12D 183 176 13 19E 204 209 14 07

462 C Czosnek et al

densities coupled with the established presence of nano-SiC in the composites [20]strongly imply the presence of abundant closed pores and make this material uniqueamong the samples

The low temperature nitrogen adsorption measurements indicate that all compos-ites are characterized by rather small and basically comparable BET surface areasin the range 04ndash83 m2g Among them the composites from the pitchSiO2 sys-tem show the highest values of 40 m2g (1300C) and 83 m2g (1650C) Hereinthe higher value detected in material after the 1650C pyrolysis is thought to resultmainly from the carbothermal reduction of silica to SiC taking place in this temper-ature range and this is accompanied by consumption of carbon from the C-matrixand concurrent release of volatiles such as CO andor CO2 [24]

SiO2 (s) + C (s) rarr SiO (g) + CO (g) (1)

SiO2 (s) + CO (g) rarr SiO (g) + CO2 (g) (2)

SiO (g) + 2C (s) rarr SiC (s) + CO (g) (3)

SiO (g) + 3CO (g) rarr SiC (s) + 2CO2 (g) (4)

CO2 (g) + C (s) rarr 2CO (g) (5)

Such surface-type reactions at temperatures required for the carbothermal reduc-tion of silica can result in opening of closed pores and extension of existing onesthus producing materials with increased surface areas after the 1650C treatmentHowever some surface area increases are noticed also for other precursor systemseven including the pitchcommercial SiC In the latter case our SEM study con-firmed the existence of numerous cracks along CSiC grains boundaries These het-erogeneities on the one hand could result from differences in thermal expansioncoefficients of the two components of CSiC On the other hand the microcrackscould also evolve from secondary carbothermal reduction of the passivating SiO2

layers as supported by FT-IR spectroscopic studies of the system [23] Eventuallyin all cases where carbon in the matrix is consumed in reactions with the precur-sors one could envision increased surface areas of the composites mostly in theform of meso- and macropore contributions Figure 1 shows low magnification im-ages of two composites obtained at different pyrolysis temperatures from the samepitchSiO2 system that support the discussed morphologicalsurface area changesat least on the surfaces of the material grains

Figure 2 represents typical results on porosity for the materials of interestcollected from mercury porosimetry including the carbonizates made from the purenon-modified pitch Figure 2A shows the cumulative pore volumes as a functionof pore diameters for the 1300C carbonizates while Fig 2B shows similar resultsafter the 1650C pyrolysis It is apparent from Fig 2A that the visibly highestporosity is evident for the 1300C non-modified carbonizate and that a similaralas lower porosity is observed for the carbonizate from the pitchelemental Sisystem At this stage of precursors conversion ie after 1300C treatmentone can expect either unreacted (pitchSiO2) or partially reacted (pitchelemental

Properties of carbonizates 463

Figure 1 SEM images illustrating surface development for CSiC composites obtained from thepitchSiO2 system at applied carbonization temperatures (A) 1300C (B) 1650C

464 C Czosnek et al

Figure 2 Cumulative pore volumes from mercury porosimetry for carbonizates from the indicatedreaction systems (A) 1300C (B) 1650C PCS is an abbreviation for poly(carbomethylsilane)

Properties of carbonizates 465

Si pitchpoly(carbomethylsilane)) precursor species contributing their own lowporosities to the overall sample porosity and therefore showing overall lowerporosities compared with the nonmodified carbonizate

The results in Fig 2B for the 1650C carbonizates clearly indicate a dramaticallydifferent sequence of the porosity curves than discussed above The highest porosityis now found for the composite from the pitchSiO2 system a ten-fold increasecompared with the relevant product from the 1300C stage This observationcan likely be linked to the major chemical reaction at the higher temperatureie carbothermal reduction of silica and the evolution of new pores and possibleexpansion of the existing ones as previously mentioned when discussing the BETdata

For the pitchSiC system an increase in porosity after the 1650C pyrolysiscan also be linked to volume-related effects due to the carbothermal reductionof passivating SiO2 layers and formation of secondary SiC Additionally for thissystem differences in thermal expansion coefficients between the carbon phase andSiC grains at phase boundaries may contribute to unfavourable mechanical strainand evolution of microcracks on cooling

Some typical SEM images for the 1300C composite systems are displayed inFig 3 The pictures were taken for bigger samples of materials approx 10 mmin size that were preserved (not ground) after the 500C initial carbonizationso to enable microscopic observations of evolving macro-morphological featuresThese specimens were further pyrolyzed at increased temperatures together with theparent bulk powder to yield the actual samples for SEM examination Forexample Fig 3A shows an image for the system pitchSi with abundant macroporesdeveloped in the massive body of the compositersquos solid matrix Figures 3B and 3Crepresent images for the pitchSiO2 and pitchcommercial SiC systems respectivelythat are characteristic of generally fewer macropores than observed in the previouspitchSi system This likely results from the lack of significant chemical changesin the former systems wherein the silicon precursors are mostly inert while inthe latter one the elemental silicon is shown to react toward detectable nano-SiCunder the applied conditions [20] On the other hand the respective material fromthe pitchpoly(carbomethylsilane) system (Fig 3D) appears to contain even moremacropores forming a foam-like structure of the matrix In conclusion the imagessupport qualitatively the conclusions from the porosimetry and BET studies aboutthe prevailing meso- and macroporous nature of these solids

Typical SEM images and the matching maps of element distribution (C carbonO oxygen Si silicon) obtained for the 1650C carbonizates from the pitchelementalSi and pitchcommercial SiC systems are included in Fig 4 part A and part Brespectively A characteristic feature of the images for the pitchSi system is auniform distribution of all the mapped elements supporting first a very efficientmixing of components and second an advantageous uniform distribution of theresultant nano-SiC in the carbon matrix evolved from the pitch (Fig 4A) This isalso true for the pitchSiO2 and pitchpoly(carbomethylsilane) systems (not shown)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

460 C Czosnek et al

Depending on the mode of SiC incorporation into a materialrsquos structure and onthe type of applied silicon precursor polycrystalline SiC with a range of crystallitesizes can be formed in the pores of carbon matrix [3] or a thin protective SiC layercan be produced on carbon grain surfaces [5] It is worth pointing out also thatnanosized SiC may improve properties of such CSiC composite materials [6ndash8]That is mostly why significant research efforts have recently been undertaken inthe area of utilization of various silicon-bearing precursors as modifiers for carbonmaterials [9ndash19] that supplement the known method of using elemental silicon asa molten saturating agent for making SiC in porous carbons [11ndash13] similarlyCVD methods of preparing SiC films have also shown to be promising in somecases [5 15]

In order to achieve highly homogeneous distribution of SiC nanocrystallites ina modified carbon matrix special and usually troublesome procedures alreadyduring initial preparation of precursors are required In this regard all methodsfor manufacturing carbongraphite materials that employ mixtures of solid carbonprecursors and low melting coal tar or petroleum pitch binders are especiallywell suited for efficient mixinghomogenization since one can utilize potentiallyadvantageous pre-modifications of the pitch with a silicon precursor in the liquidphase

The authors of this study have recently reported the investigations of various pitchsilicon precursors that provided an insight into thermally promoted conversion of theprecursors in the matrix of simultaneously carbonized pitch toward nanocompositesCSiC [20ndash22] In the current report major applicable properties of the CSiC com-posites and particularly morphology and surface development are discussed

2 EXPERIMENTAL

The target products included carbon materials prepared by thermal treatment (car-bonization pyrolysis) under an argon atmosphere at final temperatures of 1300Cor 1650C of a typical coal tar pitch binder (softening point by Mettler 1015Ctoluene insolubles 209) that was individually pre-modifiedmixed with selectedsilicon-bearing precursors The following powdered silicon precursors were used(Aldrich) elemental Si (lt325 mesh) silica SiO2 (lt325 mesh) commercial SiC(lt400 mesh) and poly(carbomethylsilane) CH2 SiH(CH3) n (av molecu-lar weight 800 mp 79C) Comparable reference carbonizates were also pre-pared from a pure non-modified pitch After repeated mixinghomogenization ofthe components at 160C in the liquid medium of the molten pitch the substratemixtures were pyrolyzed at 500C under an argon atmosphere to afford initial solidcarbonizates for further pyrolysis at the final temperature of 1300C or 1650C Adetailed description of the preparation and materials spectroscopic characterizationis provided elsewhere [20 21 23]

The composite CSiC materials were characterized with (i) BET surface areasderived from standard low temperature nitrogen adsorption measured with Mi-

Properties of carbonizates 461

cromeritics Gemini 2360 (ii) helium density measurements with Micromeritics Ac-cuPyc (fivefold helium purging) and (iii) mercury intrusion porosimetry carried outwith Porosimeter 2000 by Carlo Erba Instruments (pressures from 1 atm to 2000 atmcorresponding to approx 15 000 nm to 75 nm pore diameter range respectively)additionally (iv) SEM images were acquired with JSM 5400 Jeol scanning electronmicroscope (20 kV accelerating voltage samples coated with Au) equipped withmicroprobe Link Isis 300 for intentionally preserved chunks of the materials ofapprox 10 mm in size

3 RESULTS AND DISCUSSION

Table 1 includes the results of helium density and BET surface area determinationsfor all composites The density data indicate basically similar values for samples A(pitchSi) B (pitchSiO2) and C (pitchcommercial SiC) with the higher densitiesobserved for the 1650C carbonizates (237ndash243 gcm3) relative to the respective1300C carbonizates (215ndash228 gcm3) These values have to be compared withthe literature density data for graphite 226 gcm3 and SiC 321 gcm3 and theyall are higher than the densities measured for both carbonizates from the purepitch ie 204ndash209 gcm3 (sample E) The latter observation can be explainedby virtue of the composites containing either (i) yet unreacted or partially reactedheavy silicon precursors in the presumed Si O C assemblages in relevant systemsafter pyrolysis at 1300C or (ii) prevailing regular β-SiC formed upon the 1650Ctreatment in all systems The various structural forms of transient and final siliconspecies evolving in the pyrolyzed carbon matrix were previously described for thesesystems [20]

Compared with the above the densities for sample D (pitchpoly(carbomethylsi-lane)) 176ndash183 gcm3 appear to be outstandingly lower even in relation to therespective values for the carbonizates from the pure pitch (sample E) Such low

Table 1Helium densities dHe and BET surface areas SBET of composites obtained from the systems Apitchelemental Si B pitchSiO2 C pitchcommercial SiC D pitchpoly(carbomethylsilane) E purenonmodified pitch

Sample dHe (gcm3) SBET (m2g)

1300C 1650C 1300C 1650C

A 215 243 14 20B 218 244 40 83C 228 237 04 12D 183 176 13 19E 204 209 14 07

462 C Czosnek et al

densities coupled with the established presence of nano-SiC in the composites [20]strongly imply the presence of abundant closed pores and make this material uniqueamong the samples

The low temperature nitrogen adsorption measurements indicate that all compos-ites are characterized by rather small and basically comparable BET surface areasin the range 04ndash83 m2g Among them the composites from the pitchSiO2 sys-tem show the highest values of 40 m2g (1300C) and 83 m2g (1650C) Hereinthe higher value detected in material after the 1650C pyrolysis is thought to resultmainly from the carbothermal reduction of silica to SiC taking place in this temper-ature range and this is accompanied by consumption of carbon from the C-matrixand concurrent release of volatiles such as CO andor CO2 [24]

SiO2 (s) + C (s) rarr SiO (g) + CO (g) (1)

SiO2 (s) + CO (g) rarr SiO (g) + CO2 (g) (2)

SiO (g) + 2C (s) rarr SiC (s) + CO (g) (3)

SiO (g) + 3CO (g) rarr SiC (s) + 2CO2 (g) (4)

CO2 (g) + C (s) rarr 2CO (g) (5)

Such surface-type reactions at temperatures required for the carbothermal reduc-tion of silica can result in opening of closed pores and extension of existing onesthus producing materials with increased surface areas after the 1650C treatmentHowever some surface area increases are noticed also for other precursor systemseven including the pitchcommercial SiC In the latter case our SEM study con-firmed the existence of numerous cracks along CSiC grains boundaries These het-erogeneities on the one hand could result from differences in thermal expansioncoefficients of the two components of CSiC On the other hand the microcrackscould also evolve from secondary carbothermal reduction of the passivating SiO2

layers as supported by FT-IR spectroscopic studies of the system [23] Eventuallyin all cases where carbon in the matrix is consumed in reactions with the precur-sors one could envision increased surface areas of the composites mostly in theform of meso- and macropore contributions Figure 1 shows low magnification im-ages of two composites obtained at different pyrolysis temperatures from the samepitchSiO2 system that support the discussed morphologicalsurface area changesat least on the surfaces of the material grains

Figure 2 represents typical results on porosity for the materials of interestcollected from mercury porosimetry including the carbonizates made from the purenon-modified pitch Figure 2A shows the cumulative pore volumes as a functionof pore diameters for the 1300C carbonizates while Fig 2B shows similar resultsafter the 1650C pyrolysis It is apparent from Fig 2A that the visibly highestporosity is evident for the 1300C non-modified carbonizate and that a similaralas lower porosity is observed for the carbonizate from the pitchelemental Sisystem At this stage of precursors conversion ie after 1300C treatmentone can expect either unreacted (pitchSiO2) or partially reacted (pitchelemental

Properties of carbonizates 463

Figure 1 SEM images illustrating surface development for CSiC composites obtained from thepitchSiO2 system at applied carbonization temperatures (A) 1300C (B) 1650C

464 C Czosnek et al

Figure 2 Cumulative pore volumes from mercury porosimetry for carbonizates from the indicatedreaction systems (A) 1300C (B) 1650C PCS is an abbreviation for poly(carbomethylsilane)

Properties of carbonizates 465

Si pitchpoly(carbomethylsilane)) precursor species contributing their own lowporosities to the overall sample porosity and therefore showing overall lowerporosities compared with the nonmodified carbonizate

The results in Fig 2B for the 1650C carbonizates clearly indicate a dramaticallydifferent sequence of the porosity curves than discussed above The highest porosityis now found for the composite from the pitchSiO2 system a ten-fold increasecompared with the relevant product from the 1300C stage This observationcan likely be linked to the major chemical reaction at the higher temperatureie carbothermal reduction of silica and the evolution of new pores and possibleexpansion of the existing ones as previously mentioned when discussing the BETdata

For the pitchSiC system an increase in porosity after the 1650C pyrolysiscan also be linked to volume-related effects due to the carbothermal reductionof passivating SiO2 layers and formation of secondary SiC Additionally for thissystem differences in thermal expansion coefficients between the carbon phase andSiC grains at phase boundaries may contribute to unfavourable mechanical strainand evolution of microcracks on cooling

Some typical SEM images for the 1300C composite systems are displayed inFig 3 The pictures were taken for bigger samples of materials approx 10 mmin size that were preserved (not ground) after the 500C initial carbonizationso to enable microscopic observations of evolving macro-morphological featuresThese specimens were further pyrolyzed at increased temperatures together with theparent bulk powder to yield the actual samples for SEM examination Forexample Fig 3A shows an image for the system pitchSi with abundant macroporesdeveloped in the massive body of the compositersquos solid matrix Figures 3B and 3Crepresent images for the pitchSiO2 and pitchcommercial SiC systems respectivelythat are characteristic of generally fewer macropores than observed in the previouspitchSi system This likely results from the lack of significant chemical changesin the former systems wherein the silicon precursors are mostly inert while inthe latter one the elemental silicon is shown to react toward detectable nano-SiCunder the applied conditions [20] On the other hand the respective material fromthe pitchpoly(carbomethylsilane) system (Fig 3D) appears to contain even moremacropores forming a foam-like structure of the matrix In conclusion the imagessupport qualitatively the conclusions from the porosimetry and BET studies aboutthe prevailing meso- and macroporous nature of these solids

Typical SEM images and the matching maps of element distribution (C carbonO oxygen Si silicon) obtained for the 1650C carbonizates from the pitchelementalSi and pitchcommercial SiC systems are included in Fig 4 part A and part Brespectively A characteristic feature of the images for the pitchSi system is auniform distribution of all the mapped elements supporting first a very efficientmixing of components and second an advantageous uniform distribution of theresultant nano-SiC in the carbon matrix evolved from the pitch (Fig 4A) This isalso true for the pitchSiO2 and pitchpoly(carbomethylsilane) systems (not shown)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

Properties of carbonizates 461

cromeritics Gemini 2360 (ii) helium density measurements with Micromeritics Ac-cuPyc (fivefold helium purging) and (iii) mercury intrusion porosimetry carried outwith Porosimeter 2000 by Carlo Erba Instruments (pressures from 1 atm to 2000 atmcorresponding to approx 15 000 nm to 75 nm pore diameter range respectively)additionally (iv) SEM images were acquired with JSM 5400 Jeol scanning electronmicroscope (20 kV accelerating voltage samples coated with Au) equipped withmicroprobe Link Isis 300 for intentionally preserved chunks of the materials ofapprox 10 mm in size

3 RESULTS AND DISCUSSION

Table 1 includes the results of helium density and BET surface area determinationsfor all composites The density data indicate basically similar values for samples A(pitchSi) B (pitchSiO2) and C (pitchcommercial SiC) with the higher densitiesobserved for the 1650C carbonizates (237ndash243 gcm3) relative to the respective1300C carbonizates (215ndash228 gcm3) These values have to be compared withthe literature density data for graphite 226 gcm3 and SiC 321 gcm3 and theyall are higher than the densities measured for both carbonizates from the purepitch ie 204ndash209 gcm3 (sample E) The latter observation can be explainedby virtue of the composites containing either (i) yet unreacted or partially reactedheavy silicon precursors in the presumed Si O C assemblages in relevant systemsafter pyrolysis at 1300C or (ii) prevailing regular β-SiC formed upon the 1650Ctreatment in all systems The various structural forms of transient and final siliconspecies evolving in the pyrolyzed carbon matrix were previously described for thesesystems [20]

Compared with the above the densities for sample D (pitchpoly(carbomethylsi-lane)) 176ndash183 gcm3 appear to be outstandingly lower even in relation to therespective values for the carbonizates from the pure pitch (sample E) Such low

Table 1Helium densities dHe and BET surface areas SBET of composites obtained from the systems Apitchelemental Si B pitchSiO2 C pitchcommercial SiC D pitchpoly(carbomethylsilane) E purenonmodified pitch

Sample dHe (gcm3) SBET (m2g)

1300C 1650C 1300C 1650C

A 215 243 14 20B 218 244 40 83C 228 237 04 12D 183 176 13 19E 204 209 14 07

462 C Czosnek et al

densities coupled with the established presence of nano-SiC in the composites [20]strongly imply the presence of abundant closed pores and make this material uniqueamong the samples

The low temperature nitrogen adsorption measurements indicate that all compos-ites are characterized by rather small and basically comparable BET surface areasin the range 04ndash83 m2g Among them the composites from the pitchSiO2 sys-tem show the highest values of 40 m2g (1300C) and 83 m2g (1650C) Hereinthe higher value detected in material after the 1650C pyrolysis is thought to resultmainly from the carbothermal reduction of silica to SiC taking place in this temper-ature range and this is accompanied by consumption of carbon from the C-matrixand concurrent release of volatiles such as CO andor CO2 [24]

SiO2 (s) + C (s) rarr SiO (g) + CO (g) (1)

SiO2 (s) + CO (g) rarr SiO (g) + CO2 (g) (2)

SiO (g) + 2C (s) rarr SiC (s) + CO (g) (3)

SiO (g) + 3CO (g) rarr SiC (s) + 2CO2 (g) (4)

CO2 (g) + C (s) rarr 2CO (g) (5)

Such surface-type reactions at temperatures required for the carbothermal reduc-tion of silica can result in opening of closed pores and extension of existing onesthus producing materials with increased surface areas after the 1650C treatmentHowever some surface area increases are noticed also for other precursor systemseven including the pitchcommercial SiC In the latter case our SEM study con-firmed the existence of numerous cracks along CSiC grains boundaries These het-erogeneities on the one hand could result from differences in thermal expansioncoefficients of the two components of CSiC On the other hand the microcrackscould also evolve from secondary carbothermal reduction of the passivating SiO2

layers as supported by FT-IR spectroscopic studies of the system [23] Eventuallyin all cases where carbon in the matrix is consumed in reactions with the precur-sors one could envision increased surface areas of the composites mostly in theform of meso- and macropore contributions Figure 1 shows low magnification im-ages of two composites obtained at different pyrolysis temperatures from the samepitchSiO2 system that support the discussed morphologicalsurface area changesat least on the surfaces of the material grains

Figure 2 represents typical results on porosity for the materials of interestcollected from mercury porosimetry including the carbonizates made from the purenon-modified pitch Figure 2A shows the cumulative pore volumes as a functionof pore diameters for the 1300C carbonizates while Fig 2B shows similar resultsafter the 1650C pyrolysis It is apparent from Fig 2A that the visibly highestporosity is evident for the 1300C non-modified carbonizate and that a similaralas lower porosity is observed for the carbonizate from the pitchelemental Sisystem At this stage of precursors conversion ie after 1300C treatmentone can expect either unreacted (pitchSiO2) or partially reacted (pitchelemental

Properties of carbonizates 463

Figure 1 SEM images illustrating surface development for CSiC composites obtained from thepitchSiO2 system at applied carbonization temperatures (A) 1300C (B) 1650C

464 C Czosnek et al

Figure 2 Cumulative pore volumes from mercury porosimetry for carbonizates from the indicatedreaction systems (A) 1300C (B) 1650C PCS is an abbreviation for poly(carbomethylsilane)

Properties of carbonizates 465

Si pitchpoly(carbomethylsilane)) precursor species contributing their own lowporosities to the overall sample porosity and therefore showing overall lowerporosities compared with the nonmodified carbonizate

The results in Fig 2B for the 1650C carbonizates clearly indicate a dramaticallydifferent sequence of the porosity curves than discussed above The highest porosityis now found for the composite from the pitchSiO2 system a ten-fold increasecompared with the relevant product from the 1300C stage This observationcan likely be linked to the major chemical reaction at the higher temperatureie carbothermal reduction of silica and the evolution of new pores and possibleexpansion of the existing ones as previously mentioned when discussing the BETdata

For the pitchSiC system an increase in porosity after the 1650C pyrolysiscan also be linked to volume-related effects due to the carbothermal reductionof passivating SiO2 layers and formation of secondary SiC Additionally for thissystem differences in thermal expansion coefficients between the carbon phase andSiC grains at phase boundaries may contribute to unfavourable mechanical strainand evolution of microcracks on cooling

Some typical SEM images for the 1300C composite systems are displayed inFig 3 The pictures were taken for bigger samples of materials approx 10 mmin size that were preserved (not ground) after the 500C initial carbonizationso to enable microscopic observations of evolving macro-morphological featuresThese specimens were further pyrolyzed at increased temperatures together with theparent bulk powder to yield the actual samples for SEM examination Forexample Fig 3A shows an image for the system pitchSi with abundant macroporesdeveloped in the massive body of the compositersquos solid matrix Figures 3B and 3Crepresent images for the pitchSiO2 and pitchcommercial SiC systems respectivelythat are characteristic of generally fewer macropores than observed in the previouspitchSi system This likely results from the lack of significant chemical changesin the former systems wherein the silicon precursors are mostly inert while inthe latter one the elemental silicon is shown to react toward detectable nano-SiCunder the applied conditions [20] On the other hand the respective material fromthe pitchpoly(carbomethylsilane) system (Fig 3D) appears to contain even moremacropores forming a foam-like structure of the matrix In conclusion the imagessupport qualitatively the conclusions from the porosimetry and BET studies aboutthe prevailing meso- and macroporous nature of these solids

Typical SEM images and the matching maps of element distribution (C carbonO oxygen Si silicon) obtained for the 1650C carbonizates from the pitchelementalSi and pitchcommercial SiC systems are included in Fig 4 part A and part Brespectively A characteristic feature of the images for the pitchSi system is auniform distribution of all the mapped elements supporting first a very efficientmixing of components and second an advantageous uniform distribution of theresultant nano-SiC in the carbon matrix evolved from the pitch (Fig 4A) This isalso true for the pitchSiO2 and pitchpoly(carbomethylsilane) systems (not shown)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

462 C Czosnek et al

densities coupled with the established presence of nano-SiC in the composites [20]strongly imply the presence of abundant closed pores and make this material uniqueamong the samples

The low temperature nitrogen adsorption measurements indicate that all compos-ites are characterized by rather small and basically comparable BET surface areasin the range 04ndash83 m2g Among them the composites from the pitchSiO2 sys-tem show the highest values of 40 m2g (1300C) and 83 m2g (1650C) Hereinthe higher value detected in material after the 1650C pyrolysis is thought to resultmainly from the carbothermal reduction of silica to SiC taking place in this temper-ature range and this is accompanied by consumption of carbon from the C-matrixand concurrent release of volatiles such as CO andor CO2 [24]

SiO2 (s) + C (s) rarr SiO (g) + CO (g) (1)

SiO2 (s) + CO (g) rarr SiO (g) + CO2 (g) (2)

SiO (g) + 2C (s) rarr SiC (s) + CO (g) (3)

SiO (g) + 3CO (g) rarr SiC (s) + 2CO2 (g) (4)

CO2 (g) + C (s) rarr 2CO (g) (5)

Such surface-type reactions at temperatures required for the carbothermal reduc-tion of silica can result in opening of closed pores and extension of existing onesthus producing materials with increased surface areas after the 1650C treatmentHowever some surface area increases are noticed also for other precursor systemseven including the pitchcommercial SiC In the latter case our SEM study con-firmed the existence of numerous cracks along CSiC grains boundaries These het-erogeneities on the one hand could result from differences in thermal expansioncoefficients of the two components of CSiC On the other hand the microcrackscould also evolve from secondary carbothermal reduction of the passivating SiO2

layers as supported by FT-IR spectroscopic studies of the system [23] Eventuallyin all cases where carbon in the matrix is consumed in reactions with the precur-sors one could envision increased surface areas of the composites mostly in theform of meso- and macropore contributions Figure 1 shows low magnification im-ages of two composites obtained at different pyrolysis temperatures from the samepitchSiO2 system that support the discussed morphologicalsurface area changesat least on the surfaces of the material grains

Figure 2 represents typical results on porosity for the materials of interestcollected from mercury porosimetry including the carbonizates made from the purenon-modified pitch Figure 2A shows the cumulative pore volumes as a functionof pore diameters for the 1300C carbonizates while Fig 2B shows similar resultsafter the 1650C pyrolysis It is apparent from Fig 2A that the visibly highestporosity is evident for the 1300C non-modified carbonizate and that a similaralas lower porosity is observed for the carbonizate from the pitchelemental Sisystem At this stage of precursors conversion ie after 1300C treatmentone can expect either unreacted (pitchSiO2) or partially reacted (pitchelemental

Properties of carbonizates 463

Figure 1 SEM images illustrating surface development for CSiC composites obtained from thepitchSiO2 system at applied carbonization temperatures (A) 1300C (B) 1650C

464 C Czosnek et al

Figure 2 Cumulative pore volumes from mercury porosimetry for carbonizates from the indicatedreaction systems (A) 1300C (B) 1650C PCS is an abbreviation for poly(carbomethylsilane)

Properties of carbonizates 465

Si pitchpoly(carbomethylsilane)) precursor species contributing their own lowporosities to the overall sample porosity and therefore showing overall lowerporosities compared with the nonmodified carbonizate

The results in Fig 2B for the 1650C carbonizates clearly indicate a dramaticallydifferent sequence of the porosity curves than discussed above The highest porosityis now found for the composite from the pitchSiO2 system a ten-fold increasecompared with the relevant product from the 1300C stage This observationcan likely be linked to the major chemical reaction at the higher temperatureie carbothermal reduction of silica and the evolution of new pores and possibleexpansion of the existing ones as previously mentioned when discussing the BETdata

For the pitchSiC system an increase in porosity after the 1650C pyrolysiscan also be linked to volume-related effects due to the carbothermal reductionof passivating SiO2 layers and formation of secondary SiC Additionally for thissystem differences in thermal expansion coefficients between the carbon phase andSiC grains at phase boundaries may contribute to unfavourable mechanical strainand evolution of microcracks on cooling

Some typical SEM images for the 1300C composite systems are displayed inFig 3 The pictures were taken for bigger samples of materials approx 10 mmin size that were preserved (not ground) after the 500C initial carbonizationso to enable microscopic observations of evolving macro-morphological featuresThese specimens were further pyrolyzed at increased temperatures together with theparent bulk powder to yield the actual samples for SEM examination Forexample Fig 3A shows an image for the system pitchSi with abundant macroporesdeveloped in the massive body of the compositersquos solid matrix Figures 3B and 3Crepresent images for the pitchSiO2 and pitchcommercial SiC systems respectivelythat are characteristic of generally fewer macropores than observed in the previouspitchSi system This likely results from the lack of significant chemical changesin the former systems wherein the silicon precursors are mostly inert while inthe latter one the elemental silicon is shown to react toward detectable nano-SiCunder the applied conditions [20] On the other hand the respective material fromthe pitchpoly(carbomethylsilane) system (Fig 3D) appears to contain even moremacropores forming a foam-like structure of the matrix In conclusion the imagessupport qualitatively the conclusions from the porosimetry and BET studies aboutthe prevailing meso- and macroporous nature of these solids

Typical SEM images and the matching maps of element distribution (C carbonO oxygen Si silicon) obtained for the 1650C carbonizates from the pitchelementalSi and pitchcommercial SiC systems are included in Fig 4 part A and part Brespectively A characteristic feature of the images for the pitchSi system is auniform distribution of all the mapped elements supporting first a very efficientmixing of components and second an advantageous uniform distribution of theresultant nano-SiC in the carbon matrix evolved from the pitch (Fig 4A) This isalso true for the pitchSiO2 and pitchpoly(carbomethylsilane) systems (not shown)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

Properties of carbonizates 463

Figure 1 SEM images illustrating surface development for CSiC composites obtained from thepitchSiO2 system at applied carbonization temperatures (A) 1300C (B) 1650C

464 C Czosnek et al

Figure 2 Cumulative pore volumes from mercury porosimetry for carbonizates from the indicatedreaction systems (A) 1300C (B) 1650C PCS is an abbreviation for poly(carbomethylsilane)

Properties of carbonizates 465

Si pitchpoly(carbomethylsilane)) precursor species contributing their own lowporosities to the overall sample porosity and therefore showing overall lowerporosities compared with the nonmodified carbonizate

The results in Fig 2B for the 1650C carbonizates clearly indicate a dramaticallydifferent sequence of the porosity curves than discussed above The highest porosityis now found for the composite from the pitchSiO2 system a ten-fold increasecompared with the relevant product from the 1300C stage This observationcan likely be linked to the major chemical reaction at the higher temperatureie carbothermal reduction of silica and the evolution of new pores and possibleexpansion of the existing ones as previously mentioned when discussing the BETdata

For the pitchSiC system an increase in porosity after the 1650C pyrolysiscan also be linked to volume-related effects due to the carbothermal reductionof passivating SiO2 layers and formation of secondary SiC Additionally for thissystem differences in thermal expansion coefficients between the carbon phase andSiC grains at phase boundaries may contribute to unfavourable mechanical strainand evolution of microcracks on cooling

Some typical SEM images for the 1300C composite systems are displayed inFig 3 The pictures were taken for bigger samples of materials approx 10 mmin size that were preserved (not ground) after the 500C initial carbonizationso to enable microscopic observations of evolving macro-morphological featuresThese specimens were further pyrolyzed at increased temperatures together with theparent bulk powder to yield the actual samples for SEM examination Forexample Fig 3A shows an image for the system pitchSi with abundant macroporesdeveloped in the massive body of the compositersquos solid matrix Figures 3B and 3Crepresent images for the pitchSiO2 and pitchcommercial SiC systems respectivelythat are characteristic of generally fewer macropores than observed in the previouspitchSi system This likely results from the lack of significant chemical changesin the former systems wherein the silicon precursors are mostly inert while inthe latter one the elemental silicon is shown to react toward detectable nano-SiCunder the applied conditions [20] On the other hand the respective material fromthe pitchpoly(carbomethylsilane) system (Fig 3D) appears to contain even moremacropores forming a foam-like structure of the matrix In conclusion the imagessupport qualitatively the conclusions from the porosimetry and BET studies aboutthe prevailing meso- and macroporous nature of these solids

Typical SEM images and the matching maps of element distribution (C carbonO oxygen Si silicon) obtained for the 1650C carbonizates from the pitchelementalSi and pitchcommercial SiC systems are included in Fig 4 part A and part Brespectively A characteristic feature of the images for the pitchSi system is auniform distribution of all the mapped elements supporting first a very efficientmixing of components and second an advantageous uniform distribution of theresultant nano-SiC in the carbon matrix evolved from the pitch (Fig 4A) This isalso true for the pitchSiO2 and pitchpoly(carbomethylsilane) systems (not shown)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

464 C Czosnek et al

Figure 2 Cumulative pore volumes from mercury porosimetry for carbonizates from the indicatedreaction systems (A) 1300C (B) 1650C PCS is an abbreviation for poly(carbomethylsilane)

Properties of carbonizates 465

Si pitchpoly(carbomethylsilane)) precursor species contributing their own lowporosities to the overall sample porosity and therefore showing overall lowerporosities compared with the nonmodified carbonizate

The results in Fig 2B for the 1650C carbonizates clearly indicate a dramaticallydifferent sequence of the porosity curves than discussed above The highest porosityis now found for the composite from the pitchSiO2 system a ten-fold increasecompared with the relevant product from the 1300C stage This observationcan likely be linked to the major chemical reaction at the higher temperatureie carbothermal reduction of silica and the evolution of new pores and possibleexpansion of the existing ones as previously mentioned when discussing the BETdata

For the pitchSiC system an increase in porosity after the 1650C pyrolysiscan also be linked to volume-related effects due to the carbothermal reductionof passivating SiO2 layers and formation of secondary SiC Additionally for thissystem differences in thermal expansion coefficients between the carbon phase andSiC grains at phase boundaries may contribute to unfavourable mechanical strainand evolution of microcracks on cooling

Some typical SEM images for the 1300C composite systems are displayed inFig 3 The pictures were taken for bigger samples of materials approx 10 mmin size that were preserved (not ground) after the 500C initial carbonizationso to enable microscopic observations of evolving macro-morphological featuresThese specimens were further pyrolyzed at increased temperatures together with theparent bulk powder to yield the actual samples for SEM examination Forexample Fig 3A shows an image for the system pitchSi with abundant macroporesdeveloped in the massive body of the compositersquos solid matrix Figures 3B and 3Crepresent images for the pitchSiO2 and pitchcommercial SiC systems respectivelythat are characteristic of generally fewer macropores than observed in the previouspitchSi system This likely results from the lack of significant chemical changesin the former systems wherein the silicon precursors are mostly inert while inthe latter one the elemental silicon is shown to react toward detectable nano-SiCunder the applied conditions [20] On the other hand the respective material fromthe pitchpoly(carbomethylsilane) system (Fig 3D) appears to contain even moremacropores forming a foam-like structure of the matrix In conclusion the imagessupport qualitatively the conclusions from the porosimetry and BET studies aboutthe prevailing meso- and macroporous nature of these solids

Typical SEM images and the matching maps of element distribution (C carbonO oxygen Si silicon) obtained for the 1650C carbonizates from the pitchelementalSi and pitchcommercial SiC systems are included in Fig 4 part A and part Brespectively A characteristic feature of the images for the pitchSi system is auniform distribution of all the mapped elements supporting first a very efficientmixing of components and second an advantageous uniform distribution of theresultant nano-SiC in the carbon matrix evolved from the pitch (Fig 4A) This isalso true for the pitchSiO2 and pitchpoly(carbomethylsilane) systems (not shown)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

Properties of carbonizates 465

Si pitchpoly(carbomethylsilane)) precursor species contributing their own lowporosities to the overall sample porosity and therefore showing overall lowerporosities compared with the nonmodified carbonizate

The results in Fig 2B for the 1650C carbonizates clearly indicate a dramaticallydifferent sequence of the porosity curves than discussed above The highest porosityis now found for the composite from the pitchSiO2 system a ten-fold increasecompared with the relevant product from the 1300C stage This observationcan likely be linked to the major chemical reaction at the higher temperatureie carbothermal reduction of silica and the evolution of new pores and possibleexpansion of the existing ones as previously mentioned when discussing the BETdata

For the pitchSiC system an increase in porosity after the 1650C pyrolysiscan also be linked to volume-related effects due to the carbothermal reductionof passivating SiO2 layers and formation of secondary SiC Additionally for thissystem differences in thermal expansion coefficients between the carbon phase andSiC grains at phase boundaries may contribute to unfavourable mechanical strainand evolution of microcracks on cooling

Some typical SEM images for the 1300C composite systems are displayed inFig 3 The pictures were taken for bigger samples of materials approx 10 mmin size that were preserved (not ground) after the 500C initial carbonizationso to enable microscopic observations of evolving macro-morphological featuresThese specimens were further pyrolyzed at increased temperatures together with theparent bulk powder to yield the actual samples for SEM examination Forexample Fig 3A shows an image for the system pitchSi with abundant macroporesdeveloped in the massive body of the compositersquos solid matrix Figures 3B and 3Crepresent images for the pitchSiO2 and pitchcommercial SiC systems respectivelythat are characteristic of generally fewer macropores than observed in the previouspitchSi system This likely results from the lack of significant chemical changesin the former systems wherein the silicon precursors are mostly inert while inthe latter one the elemental silicon is shown to react toward detectable nano-SiCunder the applied conditions [20] On the other hand the respective material fromthe pitchpoly(carbomethylsilane) system (Fig 3D) appears to contain even moremacropores forming a foam-like structure of the matrix In conclusion the imagessupport qualitatively the conclusions from the porosimetry and BET studies aboutthe prevailing meso- and macroporous nature of these solids

Typical SEM images and the matching maps of element distribution (C carbonO oxygen Si silicon) obtained for the 1650C carbonizates from the pitchelementalSi and pitchcommercial SiC systems are included in Fig 4 part A and part Brespectively A characteristic feature of the images for the pitchSi system is auniform distribution of all the mapped elements supporting first a very efficientmixing of components and second an advantageous uniform distribution of theresultant nano-SiC in the carbon matrix evolved from the pitch (Fig 4A) This isalso true for the pitchSiO2 and pitchpoly(carbomethylsilane) systems (not shown)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

466 C Czosnek et al

Figure 3 SEM images for carbonizates obtained at 1300C under an argon atmosphere from thesystems (A) pitchelemental Si (B) pitchSiO2 (C) pitchcommercial SiC (D) pitchpoly(carbo-methylsilane)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

Properties of carbonizates 467

Figure 3 (Continued)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

468 C Czosnek et al

Figure 4 SEM images and corresponding maps of element distrubutions in carbonizates obtainedat 1650C under an argon flow from the systems (A) pitchelemental Si (B) pitchcommercial SiCSEM image mdash upper left corner C distribution mdash upper right corner O distribution mdash bottom leftcorner Si distribution mdash bottom right corner

On the other hand the maps collected for the reference pitchSiC system (Fig 4B)clearly support the existence of separate relatively large grains of SiC which dueto their overall chemical inertness during carbonization persisted throughout the

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

Properties of carbonizates 469

treatment seemingly unchanged in bulk In this regard it is worth recalling thata detailed insight into this system supported carbothermal reduction within thepassivating SiO2 layers of the componentrsquos grains and the formation of secondarynano-SiC [20]

An interesting microscopic feature was observed for all systems but the pitchcom-mercial SiC carbonized at 1300C namely the occurrence of numerous whiskersfound both on flat surfaces and in big open pores of the more massive samples(Fig 5) The whiskers were confirmed by EDX mapping to be forms of silicon car-bide materials The formation of SiC whiskers is generally thought to proceed viaparticipation of reactive volatile silicon species in the gas phase thus indicating yetanother reaction pathway operating in these systems [25 26] The extent of whiskerformation seemed to be connected with amounts of available oxygen and it was arather peripheral phenomenon under applied conditions In this regard no whiskerswere observed in the related bulk powdered samples supporting a view that theirformation is additionally governed by local mass transport and diffusion phenom-ena Finally abundant SiC whiskers were also seen in the pitchSiO2 system afterthe 1650C pyrolysis consistent with the efficient carbothermal reduction chemistrytaking place in this temperature range

Figure 5 SEM images of whisker features found in carbonizates obtained at 1300C under anargon atmosphere from the systems (A) pitchelemental Si (B) pitchSiO2 (C) pitchpoly(carbo-methylsilane)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

470 C Czosnek et al

Figure 5 (Continued)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

5 S Jonas S Kluska and E Walasek Ceramics mdash Polish Ceramic Bulletin 67 7 (2001) (in Polish)6 M Monthioux and O Delverdier J Eur Ceram Soc 16 721 (1996)7 H S Ahn and D J Choi Surf Coat Technol 154 276 (2002)8 X Bourrat K S Turner and A G Evans J Am Ceram Soc 78 3050 (1995)9 C Vix-Guterl and P Ehrburger Carbon 35 1587 (1997)

10 P P Paul and S T Schwab Carbon 34 89 (1996)11 L Korona in Tworzywa z wegla uszlachetnionego nasycone metalami Wydawnictwa

Naukowo-Techniczne Warszawa Poland (1980) (in Polish)

472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)

Properties of carbonizates 471

4 CONCLUSIONS

We successfully prepared homogeneously dispersed binary mixtures of a coal tarpitch with individual powdered silicon additives for stepwise carbonization of thesystems up to 1650C under an argon flow to yield nanocomposite products CSiC

Some specific reaction pathways were observed in the pitchelemental SipitchSiO2 and pitchpoly(carbomethylsilane) systems resulting in occasional SiCwhisker formation

All products were found to show relatively small BET surface areas determinedby low-temperature adsorption of nitrogen but with some differences that could betraced to specific chemical changes in the systems

The porosimetry results supported the prevailingly meso- and macroporous natureof the materials with strong temperature dependence of the size of porosity For in-stance in the pitchSiO2 system the overall porosity of the 1650C carbonizate wasten times larger than the respective value for the 1300C carbonizate Such vari-ations were linked to the mass transporttemperature specifics of the carbothermalreduction of silica taking place in this temperature range

The majority of the nanocomposites showed comparable helium densities exceptfor the pitchpoly(carbomethylsilane) system in which the densities of the productswere significantly lower suggesting abundant closed pores and resulting in a uniquecomposite material

Acknowledgements

This work was supported by AGH University of Science and Technology grantNo 111121062

REFERENCES

1 J B Casady A K Agarwal S Seshadri R R Siergiej L B Rowland M F MacMillanD C Sheridan P A Sanger and C D Brandt Solid-State Electron 42 2165 (1998)

2 R R Siergiej R C Clarke S Sriram A K Agarwal R J Bojko A W Morse V BalakrishnaM F MacMillan A A Burk and C D Brandt Mater Sci Eng B 61ndash62 9 (1999)

3 J Szpineter The influence of the Si-additive on the structure and properties of carbon materialsPhD Dissertation Silesian Technical University Katowice Poland (1999) (in Polish)

4 K Skoczkowski in Wykładziny weglowo-grafitowe Wydawnictwo Fundacji im WojciechaSwietosławskiego na Rzecz Wspierania Nauki i Potencjału Naukowego w Polsce GliwicePoland (1998) (in Polish)

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pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

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472 C Czosnek et al

12 D W Shin S S Park Y H Choa and K Niihara J Am Ceram Soc 82 3251 (1999)13 F H Gern and R Kochendoumlrfer Composites Part A 28A 355 (1997)14 Q Zhu X Qiu and C Ma Carbon 37 1475 (1999)15 T Kingetsu M Takehara T Yarii K Ito and H Masumoto Thin Solid Films 315 139 (1998)16 L M Manocha S Manocha K B Patel and P Glogar Carbon 38 1481 (2000)17 L A Harris C R Kennedy G C T Wei and F P Jeffers J Am Ceram Soc Commun 67

C-0121 (1984)18 C Vix-Guterl J Lahaye and P Ehrburger Carbon 31 629 (1993)19 G B Zheng H Sano Y Uchiyama K Kobayaschi and H M Cheng J Mater Sci 34 827

(1999)20 C Czosnek W Ratuszek J F Janik and Z Olejniczak Fuel Process Technol 79 199 (2002)21 C Czosnek J F Janik and Z Olejniczak J Cluster Sci 13 487 (2002)22 C Czosnek J Wolszczak M Drygas M Goacutera and J F Janik J Phys Chem Solids 65 647

(2004)23 C Czosnek Conversions of elemental silicon and its compounds during co-pyrolysis with a

pitch from the point of view of product characteristics modifications PhD Dissertation AGHUniversity of Science and Technology Krakoacutew Poland (2003) (in Polish)

24 P C Silva and J L Figueiredo Mater Chem Phys 72 326 (2001)25 C Dai X Zhang J Zhang Y Yang L Cao and F Xia J Am Ceram Soc 80 1274 (1997)26 W-S Seo K Koumoto and S Aria J Am Ceram Soc 83 2584 (2000)