Biomedical Engineering Reference
In-Depth Information
et al
. 2003). The most widely used calibration methods determine the change in the
resonance frequency due to added mass (Cleveland
et al
. 1993), record the thermal
noise (Hutter and Bechhoefer 1993), or use an accurately calibrated reference cantilever
(Torii
et al
. 1996). The distance between the tip and the sample cannot be determined
directly. For presenting the interaction force as a function of tip-sample separation, the
distance is inferred from the raw data by adding the cantilever deflection to the sample
position. In this way the force can be plotted as a function of relative separation in a
force curve.
6.4
Experimental
6.4.1 Materials
6.4.1.1 Adsorption Experiments
QCM-D crystals.
The sensor crystals used as a substrate for the model film coatings
and in the QCM-D experiments were AT-cut quartz crystals supplied by Q-sense AB,
Gothenburg, Sweden with a resonance frequency
f
0
≈
5 MHz and a sensitivity constant
0
.
177 mg m
−
2
Hz
−
1
. The crystals were spin-coated with polystyrene by the sup-
plier. The polystyrene surface was hydrophobic, the contact angle values of pure water
on the crystal surface were 95
◦
±
C
≈
2
◦
(Tammelin
et al
. 2006b).
Cellulose model film.
Trimethylsilyl cellulose (TMSC) dissolved in chloroform was
deposited on the polystyrene coated QCM-D crystal using Langmuir-Schaefer technique
as described by Tammelin
et al
. (2006b). TMSC was hydrolyzed back to cellulose with
acid hydrolysis according to Schaub
et al
. (1993).
Mixture of dissolved hemicelluloses.
Hemicelluloses used in the adsorption experiments
were isolated from the hexane extracted TMP by using the procedure described by
Thornton
et al
. (1994). Dissolved hemicellulose fractions were isolated from unbleached
and peroxide bleached TMP. The monosaccharide composition of the aqueous hemicel-
lulose fractions determined by gas chromatography is listed in Table 6.1. The fractions
from unbleached and bleached TMP were anionic with a charge density of 0.51 meq g
−
1
and 1.38 meq g
−
1
, respectively. Charge densities were determined by titration with a
cationic polyelectrolyte (1 meq l
−
1
pDADMAC,
M
w
<
300 kDa), using a particle charge
detector (M utek PCD 03, Germany) to indicate the end-point.
GGM (charge density 0.09 meq g
−
1
, weight average
O-acetyl-galactoglucomannan.
M
w
≈
50 kDa with unimodal
M
w
distribution analyzed by size exclusion chromatogra-
phy (SEC) was isolated from the mixture of TMP derived dissolved hemicelluloses by
the ultrafiltration technique described by Willfor
et al
. (2003).
Pectin.
Pectin samples with a
M
w
comparable to pectin found in spruce were pre-
pared from commercial citrus fruit pectin (Sigma-Aldrich Chemie BmbH, Germany) by
alkaline hydrolysis. The reaction mixtures were cooled to room temperature, acidified,
concentrated in a vacuum rotor-evaporator and freeze-dried. The charge density of the
final product was 2.1 meq g
−
1
. The weight average
M
w
was
≈
12 kDa with a unimodal
M
w
distribution analyzed by SEC.
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