5 nm 10.333 m (b) what is carbon nano-onion experiment set-up controllable growth of carbon...

1
-0.3 0.0 0.3 -400 -200 0 200 400 C ap acitan ce (F /g ) 10 m v/s 50 m v/s 100 m v/s 500 m v/s 1000 m v/s P oten tial(V ) 5 nm 5 nm 10.333 m (b ) 800 1600 In ten sity (a.u) R am an sh ift (cm -1 ) What is carbon nano-onion Experiment set-up Controllable Growth of Carbon Nano-Onions for Developing Controllable Growth of Carbon Nano-Onions for Developing High-Performance Supercapacitors High-Performance Supercapacitors Y. Gao, Y. S. Zhou, J. Hudgins, Y. Gao, Y. S. Zhou, J. Hudgins, and Y. F. Lu* and Y. F. Lu* Department of Electrical Engineering, University of Nebraska, Lincoln Department of Electrical Engineering, University of Nebraska, Lincoln E-mail: E-mail: [email protected] website: website: http://lane.unl.edu http://lane.unl.edu Fresh Onion: edible Carbon Nano-Onion: non- edible Carbon nano-onions (CNOs) are concentric multilayer giant fullerenes, which consist of multiple concentric graphitic shells to form encapsulated structures Motivations High specific surface area High electrochemical stability High electronic conductivity Emergency doors on jet Emergency doors on jet planes planes Hybrid auto Hybrid auto Backup power supply Backup power supply Wind energy storage Wind energy storage Battleship Battleship ignition ignition Experiments and results Synthesis of CNOs Capacitive properties of CNOs Capacitive properties of MnO 2 /CNO hybrid structure Illustration of the experimental setup for CNO growth with resonant excitation by a wavelength-tunable CO 2 laser. 10.532 m 10.333 m Without laser Photographs of ethylene-oxygen flames under laser excitation (The images below show molecular vibration under the excitation conditions). A laser-assisted combustion process for growing CNO in open air was developed by using laser irradiations to achieve resonant excitation of precursor molecules. The laser energy was much more effectively coupled into the flame through the resonant excitation of ethylene molecules at 10.532 µm than other non-resonant wavelength. Without laser 10.333 m 10.532 m 2D CNOs FWHM of G-band (cm -1 ) R3=I D3 /( I D3 +I D2 +I G ) Without laser 71.4 0.24 10.333 m 64.6 0.23 10.532 m 59.5 0.19 D G 10.532 m 5 nm 5 nm Experiment results 1500 2000 2500 3000 2400 2700 3000 In te n s ity (a .u .) R am an sh ift (cm -1 ) 5 nm 5 nm 5 nm 5 nm 10.532 µm-400 W 10.532 µm-600 W TEM images of CNOs grown (a) without laser excitation and with laser excitations at (b) 10.333 and (c) 10.532 µm. (d) Raman spectra of CNOs grown without laser excitation and with laser excitations at 10.333 and 10.532 µm . (e) Typical curve fitting of a first-order Raman spectrum. 5 nm 5 nm Without laser (a ) (c ) 1500 2000 2500 3000 In ten s ity (a .u .) R am an sh ift (cm -1 ) (d ) Summary of G-band FWHM and R3 for CNOs grown without laser excitation and with excitation at wavelengths of 10.333 and 10.532 µm at 1000 W. TEM images of CNOs grown (a) without laser excitation and with different laser powers of (b) 400, (c) 600, and (d) 1000 W at 10.532 µm. (e) Raman spectra of CNOs grown with different laser powers. Without laser (a ) (b ) (c ) (d ) (e ) A simple method was used to activate the primitive CNOs by using KOH solution to achieve the increased specific surface areas of CNOs. In brief, (1) CNOs was firstly impregnated in KOH solution for 24 h; (2) The solution was filtered to get the impregnated CNOs. (3) The obtained CNOs was dried in an oven for 12 h at ~90 ℃; (4) At last, the CNOs were annealed at ~800 ℃ in N 2 atmosphere for 1 h. Capacitive properties of CNOs before KOH activation -0.4 -0.2 0.0 0.2 0.4 -30 -20 -10 0 10 20 30 C ap acitan ce (F /g ) P oten tial(V ) -0.4 -0.2 0.0 0.2 0.4 -45 -30 -15 0 15 30 P o tential(V ) C ap acitan ce (F /g ) -0.4 -0.2 0.0 0.2 0.4 -60 -40 -20 0 20 40 P oten tial(V ) C ap acitan ce (F /g ) (a) Specific surface areas (SSAs) of CNOs grown at different laser powers. (b - d) Cyclic voltammograms of CNO electrodes. (a ) (b ) (c ) (d ) 400 W: 16 F/g 800 W: 25 F/g 1000 W: 30 F/g Capacitive properties of CNOs after KOH activation The SSAs increase with the increase in laser power. Consequently, the capacitance of CNOs increases. However, CNOs with much larger SSAs are needed to achieve improved capacitances. 1 10 100 0.00 0.02 0.04 0.06 0.08 0.10 0.12 W ith o u t activatio n 4M K O H activatio n 5M K O H activatio n 6M K O H activatio n 7M K O H activatio n P o re vo lu m e (cm 3 /g/nm ) P o re size (n m ) 0 2 4 6 8 400 500 600 700 800 K O H co n cen tratio n fo r activatio n (m ol/L) S p ecific su rface area (m 2 /g ) (a) SSAs and (b) Pore size distributions of CNOs activated at different KOH concentrations. The SSAs increase with the increase of KOH concentration. After activation, pores (<= 5 nm) contribute significantly to the total pore volume of CNOs. It is suggested that the activation of carbon with KOH proceeds as 6KOH + C ↔ 2K +3H 2 + 2K 2 CO 3 Then it followed by decomposition of K 2 CO 3 and/or reaction of K/K 2 CO 3 /CO 2 , with carbon. 5nm 5nm 5nm 5nm (b ) (a ) TEM images of CNOs (c) before activation (d) after 6M activation. Before activation After activation (c ) (d ) -0.4 -0.2 0.0 0.2 0.4 -150 -100 -50 0 50 100 150 P o tential(V ) C ap acitan c e (F /g) 0 50 100 -0.4 -0.2 0.0 0.2 0.4 Tim e (S ec) P o ten tial(V ) 6 M activation: 108 F/g Before activation: 25 F/g 6 M activation Before activation 0 2 4 6 8 20 40 60 80 100 120 K O H co n cen tratio n fo r activatio n (m ol/L) C ap acitan c e (F /g) (a) Capacitance of CNOs after KOH activation. (b) Galvanostatic charge/discharge curves of CNOs before and after 6 M KOH activation. (c) Cyclic voltammograms of CNOs before and after 6 M KOH activation. (a) Cyclic voltammograms and (b) the capacitances of CNOs after 6 M KOH activation at different scan rates. Deposition of MnO 2 on CNOs Experiment steps: After drying, the CNO coated Ni foams were immersed into the precursor solution ( mixture of 0.1 M Na 2 SO 4 and 0.1 M KMnO 4 ) for MnO 2 coating. After immersing, the samples were rinsed using deionized water and then heated at 120 ℃ for 12 h in air. Capacitive properties of MnO 2 /CNO hybrid structure Electrophoretic deposition of CNOs on Ni foams Electrophoretic deposition of CNOs on Ni foams CNOs were dispersed in ethanol. Al(NO 3 ) 3 was added into the solution to stabilize the CNO particles in the solution; The suspension was ultrasonicated for 30 min; Then a layer of CNOs was deposited onto Ni foams by electrophoretic deposition. Deposition of MnO Deposition of MnO 2 on CNO/Ni foam on CNO/Ni foam -0.4 -0.2 0.0 0.2 0.4 0.6 0.8 -600 -400 -200 0 200 400 600 P oten tial(V ) C ap acitan c e (F /g) 0 3 6 9 12 0 100 200 300 D ep o sitio n tim e (h ) C ap acitan c e (F /g) 0 100 200 300 400 -0.4 0.0 0.4 0.8 Tim e (sec) V o ltag e (V ) 400 800 In te n s ity (a . u ) R am an sh ift (cm -1 ) Before MnO 2 deposition 3 h MnO 2 deposition (b ) (a ) 6 h MnO 2 deposition 12 h MnO 2 deposition (c ) (d ) 12 h deposition 6 h deposition 3 h deposition Without deposition 12 h deposition 6 h deposition 3 h deposition Without deposition MnO 2 (e ) (f ) SEM images of CNOs (a) without MnO 2 deposition and with (b) 3 h, (c) 6 h, (d) 12 h deposition. (e) Raman spectra of CNOs without MnO 2 deposition and with (b) 3 h, (c) 6 h, (d) 12 h deposition. (f) Raman spectra of the samples in the spectra range from 200 to 1000 cm -1 . (a) Capacitance of CNOs after MnO 2 deposition. (b) Galvanostatic charge/discharge curves of CNOs before and after 12 h MnO 2 deposition. (c) Cyclic voltammograms of CNOs before and after 12 h MnO 2 deposition. . -0.2 0.0 0.2 0.4 0.6 0.8 -600 -300 0 300 600 10 m v 100 m v 500 m v 1000 m v 5000 m v P o ten tial(V ) C ap ac itan c e (F /g) (a) Cyclic voltammograms and (b) the capacitances of CNOs after 12 h MnO 2 deposition. 0 1000 2000 3000 4000 5000 100 200 300 P oten tial(V ) C ap a c itan ce (F /g) (b ) (a ) (c ) (b ) (a ) (b ) (a ) (c ) (b ) (a ) CNOs deposited onto Ni foam MnO 2 deposited onto CNO/Ni foam Future directions Acknowledgements Scalable production of CNOs 25 welding torches with 3 mm orifice tips will be used to generate the flames. A wavelength-tunable CO 2 laser at a wavelength of 10.532 µm will be used to resonantly couple laser energy to the flame. Another laser at 10.591 µm will be used to control the size of the CNOs. A fume collector will be used to collect CNOs generated from the flames. It is estimated that a production rate of 500 g/h will be achieved. High-performance supercapacitors using hierarchical three-dimensional micro/nanoelectrodes To achieve increased SSAs and reduced internal resistance at the same time; The Ni foams will serve as conductive scaffolds to house CNTs and CNOs to reduce the matrix resistivity; The CNTs will be grown within the Ni foams to reduce the matrix resistivity and increase the SSA significantly; CNOs will be used to fill the remaining spacing among the Ni forms and to further increase the The authors gratefully thank Nebraska Center for Energy Sciences Research (NCESR) and National Science Foundation (NSF) for financial support. (e ) 1200 1500 1800 D4 D1 D3 G D2 In ten s ity (a .u .) R am an sh ift (cm -1 ) 0 200 400 600 800 1000 80 90 100 110 120 C ap acitan c e (F /g) S can rate (m v/s) 12 h deposition: 313 F/g Before activation: 25 F/g 12 h deposition Before activation 500 nm 500 nm 500 nm 500 nm 500 nm 500 nm 500 nm 500 nm CNOs are promising electrode material in fabricating high- performance supercapacitors Ragone plot: www.imechanica.org Carbon materials have high SSAs, long cycle life, and high conductivity but low capacitance. Metal oxides have high theoretical capacitance but suffer from low SSAs, short cycle life, and low conductivity. Metal oxide/CNO composite is a potential approach to improve both capacitance and conductivity. In this study, capacitive properties of MnO 2 /CNO hybrid structure were investigated.

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Page 1: 5 nm 10.333  m (b) What is carbon nano-onion Experiment set-up Controllable Growth of Carbon Nano-Onions for Developing High-Performance Supercapacitors

-0.3 0.0 0.3-400

-200

0

200

400

Cap

acit

ance

(F

/g)

10 mv/s 50 mv/s 100 mv/s 500 mv/s 1000 mv/s

Potential (V)

5 nm5 nm

10.333 m(b)

800 1600

Inte

nsity

(a. u

)

Raman shift (cm-1)

What is carbon nano-onion

Experiment set-up

Controllable Growth of Carbon Nano-Onions for Developing High-Performance Controllable Growth of Carbon Nano-Onions for Developing High-Performance SupercapacitorsSupercapacitors

Y. Gao, Y. S. Zhou, J. Hudgins,Y. Gao, Y. S. Zhou, J. Hudgins, and Y. F. Lu*and Y. F. Lu*Department of Electrical Engineering, University of Nebraska, LincolnDepartment of Electrical Engineering, University of Nebraska, Lincoln

E-mail: E-mail: [email protected] website: http://lane.unl.edu website: http://lane.unl.edu

Fresh Onion: edibleCarbon Nano-Onion: non-edible

Carbon nano-onions (CNOs) are concentric multilayer giant fullerenes, which consist of multiple concentric graphitic shells to form encapsulated structures

Motivations

High specific surface area

High electrochemical stability

High electronic conductivity

Emergency doors on jet planesEmergency doors on jet planes Hybrid autoHybrid auto

Backup power supplyBackup power supply Wind energy storageWind energy storage

Battleship ignitionBattleship ignition

Experiments and results

Synthesis of CNOs Capacitive properties of CNOs Capacitive properties of MnO2/CNO hybrid structure

Illustration of the experimental setup for CNO growth with resonant excitation by a wavelength-tunable CO2 laser.

10.532 m10.333 mWithout laser

Photographs of ethylene-oxygen flames under laser excitation (The images below show molecular vibration under the excitation conditions).

A laser-assisted combustion process for growing CNO in open air was developed by using laser irradiations to achieve resonant excitation of precursor molecules. The laser energy was much more effectively coupled into the flame through the resonant excitation of ethylene molecules at 10.532 µm than other non-resonant wavelength.

Without laser

10.333 m

10.532 m2D

CNOs FWHM of G-band (cm-1) R3=ID3/( ID3 +ID2 +IG)

Without laser 71.4 0.24

10.333 m 64.6 0.23

10.532 m 59.5 0.19

DG

10.532 m

5 nm5 nm

Experiment results

1500 2000 2500 3000

2400 2700 3000

In

ten

sit

y (

a.u

.)

Raman shift (cm-1)

5 nm5 nm

5 nm5 nm

10.532 µm-400 W

10.532 µm-600 W

TEM images of CNOs grown (a) without laser excitation and with laser excitations at (b) 10.333 and (c) 10.532 µm. (d) Raman spectra of CNOs grown without laser excitation and with laser excitations at 10.333 and 10.532 µm . (e) Typical curve fitting of a first-order Raman spectrum.

5 nm5 nm

Without laser(a) (c)

1500 2000 2500 3000

In

ten

sity

(a.

u.)

Raman shift (cm-1)

(d)

Summary of G-band FWHM and R3 for CNOs grown without laser excitation and with excitation at wavelengths of 10.333 and 10.532 µm at 1000 W.

TEM images of CNOs grown (a) without laser excitation and with different laser powers of (b) 400, (c) 600, and (d) 1000 W at 10.532 µm. (e) Raman spectra of CNOs grown with different laser powers.

Without laser(a) (b)

(c) (d)

(e)

A simple method was used to activate the primitive CNOs by using KOH solution to achieve the increased specific surface areas of CNOs. In brief, (1) CNOs was firstly impregnated in KOH solution for 24 h; (2) The solution was filtered to get the impregnated CNOs. (3) The obtained CNOs was dried in an oven for 12 h at ~90 ; (4) At last, the CNOs were annealed at ~800 in N℃ ℃ 2 atmosphere for 1 h.

Capacitive properties of CNOs before KOH activation

-0.4 -0.2 0.0 0.2 0.4-30

-20

-10

0

10

20

30

Cap

acit

ance

(F

/g)

Potential (V)

-0.4 -0.2 0.0 0.2 0.4-45

-30

-15

0

15

30

Potential (V)

Cap

acit

ance

(F

/g)

-0.4 -0.2 0.0 0.2 0.4-60

-40

-20

0

20

40

Potential (V)

Cap

acit

ance

(F

/g)

(a) Specific surface areas (SSAs) of CNOs grown at different laser powers. (b - d) Cyclic voltammograms of CNO electrodes.

(a) (b) (c) (d)400 W: 16 F/g 800 W: 25 F/g 1000 W: 30 F/g

Capacitive properties of CNOs after KOH activation

The SSAs increase with the increase in laser power. Consequently, the capacitance of CNOs increases. However, CNOs with much larger SSAs are needed to achieve improved capacitances.

1 10 100

0.00

0.02

0.04

0.06

0.08

0.10

0.12

Without activation 4M KOH activation 5M KOH activation 6M KOH activation 7M KOH activation

Po

re v

olu

me

(cm

3 /g/n

m)

Pore size (nm)0 2 4 6 8

400

500

600

700

800

KOH concentration for activation (mol/L)

Sp

ecif

ic s

urf

ace

area

(m

2 /g)

(a) SSAs and (b) Pore size distributions of CNOs activated at different KOH concentrations.

The SSAs increase with the increase of KOH concentration. After activation, pores (<= 5 nm) contribute significantly to the total pore volume of CNOs.

It is suggested that the activation of carbon with KOH proceeds as

6KOH + C ↔ 2K +3H2 + 2K2CO3 Then it followed by decomposition of K2CO3 and/or reaction of K/K2CO3/CO2, with carbon.

5nm5nm 5nm5nm

(b)(a)

TEM images of CNOs (c) before activation (d) after 6M activation.

Before activation After activation(c) (d)

-0.4 -0.2 0.0 0.2 0.4

-150

-100

-50

0

50

100

150

Potential (V)

Ca

pa

cit

an

ce

(F

/g)

0 50 100

-0.4

-0.2

0.0

0.2

0.4

Time (Sec)

Po

ten

tial

(V

)

6 M activation: 108 F/g

Before activation: 25 F/g

6 M activation

Before activation

0 2 4 6 8

20

40

60

80

100

120

KOH concentration for activation (mol/L)

C

ap

ac

ita

nc

e (

F/g

)

(a) Capacitance of CNOs after KOH activation. (b) Galvanostatic charge/dischargecurves of CNOs before and after 6 M KOH activation. (c) Cyclic voltammograms of CNOs before and after 6 M KOH activation.

(a) Cyclic voltammograms and (b) the capacitances of CNOs after 6 M KOH activation at different scan rates.

Deposition of MnO2 on CNOs

Experiment steps:

• After drying, the CNO coated Ni foams were immersed into the precursor solution ( mixture of 0.1 M Na2SO4 and 0.1 M KMnO4) for MnO2 coating.

• After immersing, the samples were rinsed using deionized water and then heated at 120 for 12 h in air.℃

Capacitive properties of MnO2/CNO hybrid structure

Electrophoretic deposition of CNOs on Ni foamsElectrophoretic deposition of CNOs on Ni foams

• CNOs were dispersed in ethanol. Al(NO3)3 was added into the solution to stabilize the CNO particles in the solution;

• The suspension was ultrasonicated for 30 min;• Then a layer of CNOs was deposited onto Ni foams by

electrophoretic deposition.

Deposition of MnODeposition of MnO22 on CNO/Ni foam on CNO/Ni foam

-0.4 -0.2 0.0 0.2 0.4 0.6 0.8-600

-400

-200

0

200

400

600

Potential (V)

Ca

pa

cit

an

ce

(F

/g)

0 3 6 9 120

100

200

300

Deposition time (h)

Ca

pa

cit

an

ce

(F

/g)

0 100 200 300 400

-0.4

0.0

0.4

0.8

Time (sec)

Vo

ltag

e (V

)

400 800

In

ten

sit

y (

a.

u)

Raman shift (cm-1)

Before MnO2 deposition 3 h MnO2 deposition(b)(a)

6 h MnO2 deposition 12 h MnO2 deposition(c) (d)

12 h deposition

6 h deposition

3 h deposition

Without deposition

12 h deposition

6 h deposition

3 h deposition

Without deposition

MnO2

(e) (f)

SEM images of CNOs (a) without MnO2 deposition and with (b) 3 h, (c) 6 h, (d) 12 h deposition. (e) Raman spectra of CNOs without MnO2 deposition and with (b) 3 h, (c) 6 h, (d) 12 h deposition. (f) Raman spectra of the samples in the spectra range from 200 to 1000 cm-1 .

(a) Capacitance of CNOs after MnO2 deposition. (b) Galvanostatic charge/dischargecurves of CNOs before and after 12 h MnO2 deposition. (c) Cyclic voltammograms of CNOs before and after 12 h MnO2 deposition. .

-0.2 0.0 0.2 0.4 0.6 0.8

-600

-300

0

300

600 10 mv 100 mv 500 mv 1000 mv 5000 mv

Potential (V)

Ca

pa

cit

an

ce

(F

/g)

(a) Cyclic voltammograms and (b) the capacitances of CNOs after 12 h MnO2 deposition.

0 1000 2000 3000 4000 5000

100

200

300

Potential (V)

Ca

pa

cit

an

ce

(F

/g)

(b)(a)

(c)

(b)(a)

(b)(a)

(c)

(b)(a)

CNOs deposited onto Ni foam

MnO2 deposited onto CNO/Ni foam

Future directions Acknowledgements

Scalable production of CNOs

25 welding torches with 3 mm orifice tips will be used to generate the flames.

A wavelength-tunable CO2 laser at a wavelength of 10.532 µm will be used to resonantly couple laser energy to the flame.

Another laser at 10.591 µm will be used to control the size of the CNOs.

A fume collector will be used to collect CNOs generated from the flames.

It is estimated that a production rate of 500 g/h will be achieved.

High-performance supercapacitors using hierarchical three-dimensional micro/nanoelectrodes

To achieve increased SSAs and reduced internal resistance at the same time; The Ni foams will serve as conductive scaffolds to house CNTs and CNOs to

reduce the matrix resistivity; The CNTs will be grown within the Ni foams to reduce the matrix resistivity

and increase the SSA significantly; CNOs will be used to fill the remaining spacing among the Ni forms and to

further increase the total SSA; Since all CNTs and CNOs will be filled within the Ni foams, no binder is

required.

The authors gratefully thank Nebraska Center for Energy Sciences Research (NCESR) and National Science Foundation (NSF) for financial support.

(e)

1200 1500 1800

D4

D1

D3G

D2

Inte

ns

ity

(a

.u.)

Raman shift (cm-1)

0 200 400 600 800 100080

90

100

110

120

Ca

pa

cit

an

ce

(F

/g)

Scan rate (mv/s)

12 h deposition: 313 F/g

Before activation: 25 F/g

12 h deposition

Before activation500 nm500 nm

500 nm500 nm 500 nm500 nm

500 nm500 nm

CNOs are promising electrode material in fabricating high-performance supercapacitors

Ragone plot: www.imechanica.org

Carbon materials have high SSAs, long cycle life, and high conductivity but low capacitance. Metal oxides have high theoretical capacitance but suffer from low SSAs, short cycle life, and low conductivity. Metal oxide/CNO composite is a potential approach to improve both capacitance and conductivity. In this study, capacitive properties of MnO2/CNO hybrid structure were investigated.