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Low-Field, Time-Domain NMR and its Application to Wood Science and Technology Society of Wood Science and Technology 50 th Annual Convention, June 10, 2007 Advanced Analytical Techniques for Wood and Biomass Knoxville, Tennessee

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Page 1: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Low-Field, Time-Domain NMR and its Application to Wood

Science and TechnologySociety of Wood Science and Technology

50th Annual Convention, June 10, 2007Advanced Analytical Techniques

for Wood and BiomassKnoxville, Tennessee

Page 2: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Thomas ElderUSDA-FS-SRS

Lisbeth Garbrecht ThygesenForest and Landscape, Faculty of Life Sciences, Copenhagen University

Nicole LabbéForest Products Center, University of Tennessee-Knoxville

Page 3: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

NMR

Fourier transform

Time domain

Frequency domain

Page 4: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Time Domain NMR• The time required for the nuclei to return to

equilibrium after excitation is the “relaxation time” (this type of NMR is sometimes referred to as “relaxometry”)

• T1 relaxation or spin-lattice or longitudinal relaxation. – Energy is dissipated to the molecular framework

• T2 relaxation or spin-spin or transverse relaxation. – Energy is dissipated to neighboring nuclei.

• Nuclei in different environments have different T1 and T2 relaxation times

Page 5: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

NMR Experiments

• For T1 determination:– Inversion recovery

• For T2 determination:– Free Induction

Decay – Hahn Spin-Echo

sequence– CPMG

Page 6: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Fitting Decay Curves• The simplest way to

determine T2 is as 36.8% of maximum signal

• Fit exponential functions• Mixtures of gaussian and

exponential functions• These generally give

discreet values for relaxation times

• FID of solids are not fit by exponentials

• Liquids can be fit by exponential functions

0

10

20

30

40

50

60

70

80

0 500 1000

decay

0102030405060708090

0 100 200 300 400 500 600

Page 7: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Relaxation Time Distributions• These methods can fit

multiexponential functions• Width and position

provides information about the various environments

• Methods– Contin– UPEN– NNLS– MVA

control

0

10

20

30

40

50

0.01 0.1 1 10 100 1000 10000

ms%

inte

nsity

Page 8: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Applications of Time Domain NMR

• MRI• Geology

– porosity• Food

– Water/fat content• Textiles

– Fabric finishes• Cosmetics• Polymers

Page 9: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Low-Field NMR

• Typical analytical spectrometers operate at several hundred MHz– FT converts the time domain information to the

frequency domain• The same thing can be done with a low field (20-

60 MHz) instrument but the spectrum is poorly resolved

• Alternatively, information can be extracted on relaxation times (the time required for the atoms to return to equilibrium after the RF pulse)

Page 10: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Low-field NMR spectrometers(not exhaustive or inclusive)

• Bruker Optics (minispec)• Oxford Instruments (Maran)• Magritek• Tel-Atomic• Process NMR• One sided NMR

– NMR-Mouse– Minispec Profiler

Page 11: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

one-sided NMR

Page 12: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Advantages and Disadvantages of Low-Field NMR

• No frequency domain spectra• Accept both solids and liquids• Limited sample preparation• Large sample sizes• Long dead time (9-38 µs)• Detects hydrogen, phosphorus, fluorine• Little maintenance• Ease of operation• Relatively inexpensive

Page 13: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Examples of Literature on Time-Domain NMR of Wood

• Moisture interactions and Imaging– UBC/Forintek (MacKay,

Hartley, Araujo, Menon)– Labbé– Ye (OSB)

• Porosity and Diffusion– STFI (Häggkvist et al.)– Lund University (Topgaard

and Söderman)• Paper

– Capitani et al.• Fungi

– Gilardi– Müller

• Black Liquor– Draheim and Ragauskas

• Adhesives– Pizzi– Root and Soriano

• Cell and Ring size– Wycoff– Johannesen

• Thermal– Hietala et al.

• pH– Ahvazi and Argyropoulos

• Wood-Adhesive interactions– Frazier

Page 14: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Relaxation Times for Wood Components

• Solid matrix– Fastest relaxation times T2<1

ms (Labbé et al. 2002)• Bound water

– T2 ~ 1ms• Free water

– T2 ~10-100 ms• Extractives

– T2 ~7-150 ms (Labbé et al. 2002)

• Detecting the hydrogens in the solid matrix requires a short dead time

• FIDs of solids are not fit well by exponential functions so it’s difficult to extract accurate relaxation times

Page 15: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Relaxation Times for Wood

Components• Liquids are well

described by exponential functions

• As such, water in various environments in the woody cell wall can be detected and analyzed

• This has mainly been done by the analysis of T2 by CPMG (Carr-Purcell-Meiboom-Gill) pulse sequence.

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

0

20

40

60

80

100

120

0.01 0.1 1 10 100 1000 10000

Bound water

Free water

0

500

1000

1500

2000

0.01 0.1 1 10 100 1000 10000

Deionized water

Page 16: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Current work on Low-field Time-domain-NMR

• Bruker minispec mq20• Low field proton NMR (20

MHz)• Relaxation times of

protons– Free induction decay– T1 (spin-lattice)– T2 (spin-spin) (CPMG

experiments)

• Decay curves were analyzed using Contin to determine distributions of relaxation times

Page 17: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Furfuryl Alcohol Modified Wood

• Introduction– Modification with

furfuryl alcohol is proposed as a method for improving dimensional stability of wood and its resistance to biological degradation.

OCH2OH

Page 18: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Furfuryl Alcohol Modified Wood

• Polymerization– Furfuryl alcohol in the presence of a catalyst

forms Poly(FA)– The polymer and the mechanism by which it

is formed is complex• Head-to-tail and head-to-head dimers are initially

formed• Conjugated chromophore segments are also

produced.

Page 19: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Methods

• Scots pine (Pinus sylvestris) was collected from northern Zealand in Denmark

• Samples were machined to 15x25x30 mm and conditioned at 20°C at 65% RH

• Samples were treated by– Pre-drying-at 103°C for 16 hours– Impregnation-under vacuum– Curing-wrapped in aluminum foil and cured at 103°C

for 16 hours– Drying-40°C for 144 hours

Page 20: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Methods• Sample treatments

– Furfuryl alcohol (FA)• Undiluted (98%)

– Citric acid (CA)• 2% in DI

– Citric acid (CA)+maleic anhydride • CA (2%)+MA (1%) in DI

– FA+CA, low WPG• FA(20%)+CA (0.77%)+ETOH(77%)+DI(2.23%)

– FA+CA, high WPG• FA(72.5%)+CA(2.78%)+ETOH(19.7%)+DI(5.02%

– FA+CA+MA, low WPG• FA(22.6%)+CA(0.25%)+MA(0.125%)+DI(5%)

– FA+CA+MA, high WPG• FA(72%)+CA(1%)+MA(0.5%)+ETOH(19%)+DI(17.5%)

– WPT• Commercial furfuryl alcohol treatment

Page 21: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Results

• Weight gain– CA, 3%– CA+MA, 4%– FA, 51%– FA+CA, low, 15%– FA+CA, high, 96%– FA+CA+MA, low, 17%– FA+CA+MA, high,

92%– WPT, 39%

0

20

40

60

80

100

120

CACA+M

A FAFA

+CA, lo

wFA

+CA, h

igh

FA+C

A+MA, lo

w

FA+C

A+MA, h

ighWPT

Page 22: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

• Samples were placed into 18mm diameter test tubes, covered with water, a vacuum was applied, and the samples were conditioned for a week.

• NMR parameters– CPMG experiment– Tau=0.5ms– 512 echoes– 32 scans– 5 second recycle delay– Gain was tuned for each sample

• Decay curves were analyzed using Contin to determine distributions of relaxation times

Low-field Time-domain-NMR

Page 23: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Control

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

0

20

40

60

80

100

120

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

0 2 4 6 8 10 12 14 16

contin distribution

020406080

100120140160

0.01 0.1 1 10 100 1000 10000

• Decay curves are exponential• T2 results show peaks for bound water,

~1ms • Free water appears as two fairly well-

resolved peaks at about 15 ms and 50ms • Bound water at FSP relaxes more rapidly

because there is only interaction with the cell wall

Page 24: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Citric Acid

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

0102030405060708090

100

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

0 2 4 6 8 10 12 14 16

contin distribution

0

50

100

150

200

250

300

0.01 0.1 1 10 100 1000 10000

• Both the decay and Contin distributions are similar to the control– Bound water and free

water are readily evident

Page 25: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Citric acid+maleic anhydride

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

0102030405060708090

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

100

0 2 4 6 8 10 12 14 16

contin distribution

0

50

100

150

200

250

300

350

0.01 0.1 1 10 100 1000 10000

• Also similar to control

Page 26: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Furfuryl Alcoholdecay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

0

10

20

30

40

50

60

70

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

0 2 4 6 8 10 12 14 16

contin distribution

0102030405060708090

0.01 0.1 1 10 100 1000 10000

• Decay curve is still exponential• Free water distribution is not as

well-resolved • The bound water is relaxing more

rapidly (T2(1) is shorter)

• Incomplete decay• Longer relaxing peak (~10ms)

– may be an artifact of the incomplete decay

– May be FA itself or water bound to FA

Page 27: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Furfuryl alcohol+citric acid (low)

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

01020304050607080

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

0 2 4 6 8 10 12 14 16

0

50

100

150

200

250

0.01 0.1 1 10 100 1000 10000

• Decay curve remains exponential

• Resolution in free water continues to degrade

Page 28: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Furfuryl alcohol+citric acid (high)

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

0

5

10

15

20

25

30

35

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

100

0 2 4 6 8 10 12 14 16

Contin distribution

0102030405060708090

0.01 0.1 1 10 100 1000 10000

• The initial part of the decay curve is reasonably well-behaved, but neither sample completely decays

• The bound water peak for the saturated sample is much broader and the relaxation time is shorter

• The free water is very poorly resolved• Multiple peaks in the sample at FSP

Page 29: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

FA+CA+MA low

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

01020304050607080

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

100

0 2 4 6 8 10 12 14 16

contin distribution

020406080

100120140160180

0.01 0.1 1 10 100 1000 10000

• Decay curves are typically exponential

• Bound water relaxation time is somewhat longer than previously observed

• Free water is fairly well-resolved.

Page 30: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

FA+CA+MA high

decay

0102030405060708090

0 100 200 300 400 500 600contin distribution

0

5

10

15

20

25

30

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

100

0 2 4 6 8 10 12 14 16contin distribution

0

20

40

60

80

100

120

0.01 0.1 1 10 100 1000 10000

• Decay curve of saturated sample is similar to the FA+CA, high treatment, exhibiting incomplete decay.

• Poor resolution in free water• Bound water amplitude is higher for

the saturated sample• Sample at FSP shows reasonable

decay, but shoulder at longer T2

Page 31: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

WPT

decay

0102030405060708090

0 100 200 300 400 500 600

contin distribution

0

10

20

30

40

50

60

0.01 0.1 1 10 100 1000 10000

decay

0102030405060708090

0 2 4 6 8 10 12 14 16

contin distribution

0

50

100

150

200

250

0.01 0.1 1 10 100 1000 10000

• Typical exponential decay curve

• Somewhat longer relaxation time for bound water

• Only one free water peak

Page 32: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Saturated samplesContin T2(1) values and MC

1

1.1

1.2

1.3

1.4

1.5

1.6

cont

rol

CA

CA

+MA FA

FA+C

A, l

ow

FA+C

A,

high

FA+C

A+M

A,

low

FA+C

A+M

A,

high

WPT

T2(1

)

020406080100120140160180

MC

(dry

)T2(1) MC

• As might be expected moisture contents markedly changed with treatment

• Inclusion of FA consistently lowered MC, particularly at high weight gains

• T2 and MC correspond closely

R2 = 0.8545

1

1.1

1.2

1.3

1.4

1.5

1.6

0 50 100 150 200

MC

T2

Page 33: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Samples at FSP Contin T2(1) values and MC

00.10.20.30.40.50.60.70.8

cont

rol

CA

CA

+MA FA

FA+C

A, l

ow

FA+C

A,

high

FA+C

A+M

A,

low

FA+C

A+M

A,

high

WPT

T2

051015202530

MC

(dry

)

T2 MC

R2 = 0.507

0.2

0.3

0.4

0.5

0.6

0.7

0.8

5 10 15 20 25 30

MC

T2

• MC for these samples is also sensitive to treatment, and becomes quite low (~9%) with the high weight gain treatments

• As before MC and T2 correspond fairly well.

Page 34: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Results and Conclusions

• Weight gain occurs with the inclusion of FA

• LF-TD-NMR, shows decreased relaxation times for free water (which correlate well with moisture content) indicating lower levels of free water (reduction in “pools” of water)

Page 35: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Enzyme-cellulose-water studies• Hypothesis

– Cellulase enzymes bind to cellulose surfaces displacing bound water

• 1 g of Whatmann # 1 filter paper• 2 g of buffer with or without enzyme(s)

– Control –just buffer– 5 mg protein endohydrolase T.

longibrachiatum (EG)– 5 mg protein cellobiohydrolase T.

longibrachiatum (CBH)– 10 mg protein Celluclast (Novozymes)

• Allowed to soak for 5 min• No mechanical mixing!• NMR recorded from 0 to 360 min.

Page 36: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Control

05

101520253035404550

1 10 100 1000 10000

01530456090120180240300360

• Bound water (~10ms) and free water (~100ms) are readily apparent.

• There is also a small shoulder just below 1000ms that disappears over time.– This is probably “bulk”

water that is being adsorbed as the experiment progresses

– Relaxation times of bound and free water increase initially and then remain fairly constant

7.58

8.59

9.5

1010.5

1111.5

0 100 200 300

T2(1

)

70

75

80

85

90

95T2

(2)

T2(1) T2(2)

Page 37: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Endoglucanase

0

10

20

30

40

50

60

1 10 100 1000 10000

01530456090120180240300360

• Both bound and free water relaxation times increase with time

7.5

8.5

9.5

10.5

11.5

12.5

13.5

0 100 200 300

T2(1

)

9293949596979899100101

T2(2

)

T2(1) T2(2)

Page 38: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Cellobiohydrolase

05

101520253035404550

1 10 100 1000 10000

01530456090120180240300360

• Bound and free water T2s fluctuate over a narrow range

7.57.77.98.18.38.58.78.99.19.3

0 100 200 300

T2(1

)

69

70

71

72

73

74

75

76T2

(2)

T2(1) T2(2)

Page 39: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Celluclast

01020304050607080

1 10 100 1000 10000

01530456090120180240300360

• After an initial rapid increase, both bound and free water relaxation times increase slightly with time

7.5

8.5

9.5

10.5

11.5

12.5

13.5

14.5

0 100 200 300

T2(1

)

9293949596979899100101102103

T2(2

)

cellulclast celluclast

Page 40: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Comparison of bound water T2s

7.5

8.5

9.5

10.5

11.5

12.5

13.5

14.5

0 50 100 150 200 250 300 350

control cellulclast endoglucanase cellobiohydrolase

• In general, relaxation times for endoglucanase and cellulclast are longer than control

• Cellobiohydrolaseresults in shorter relaxation times

Page 41: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Comparison of free water T2s• More pronounced

difference between endoglucanase/celluclast and control/CBH

• Free water is relaxing more slowly with treatment and time.– This could be due to

an increase in “bulk” water or an increase in porosity

6570758085

9095

100105

0 50 100 150 200 250 300 350 400

control celluclast endoglucanase cellobiohydrolase

Page 42: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

A2/A1

02468

10121416

0 50 100 150 200 250 300 350 400

control celluclast endoglucanase cellobiohydrolase

• Ratios of amplitudes indicates that the relative amount of free water increases with celluclasttreament

• Very small difference between control and endoglucanase

Page 43: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Results• The relaxation times for bound water (T2(1)) do

not vary much and don’t show much in terms of patterns between the treatments. Although the control is generally faster.

• The relaxation times for the free water (T2(2)) are similar for the enzyme treatment and both are longer than the control.– The longer relaxation times could mean

• an increase in porosity due to the action of the enzyme• Simply interaction of the water with the enzyme• An increase in of free water (?)

Page 44: Low-Field, Time-Domain NMR and its Application to Wood Science and Technology · 2007. 7. 19. · • FID of solids are not fit by exponentials • Liquids can be fit by exponential

Other completed and ongoing studies

• Charcoal• Cellulose treated in electron beam• Effect of pre-treatment on biomass• Detection of extractives• Thermal treatment of MDF furnish