High performance capillary electrophoresis - T.E.A.M.
High performance capillary electrophoresis - T.E.A.M.
High performance capillary electrophoresis - T.E.A.M.
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Principles<br />
determined by the <strong>capillary</strong> dimensions, conductivity of<br />
the buffer, and the applied voltage. Significantly elevated<br />
temperatures will result when the power generation exceeds<br />
dissipation. Typical power generation ranges from<br />
0.5 to 5 W/m. Temperature increases of 10 °C are not<br />
uncommon, although 70 °C and higher can occur.<br />
Normalized zone<br />
deformation<br />
100<br />
80<br />
60<br />
40<br />
20<br />
0<br />
= 0.20 mm<br />
0.10 mm<br />
0.075 mm<br />
0.05 mm<br />
0.025 mm<br />
500 1000 1500<br />
Field strength [V/cm]<br />
Figure 12<br />
Effect of Joule heating and temperature<br />
gradients on solute zone deformation 4<br />
( = <strong>capillary</strong> id)<br />
While the absolute rise in temperature is generally not<br />
detrimental (except possibly for sample degradation, and<br />
so on), temperature gradients are. Thermal dissipation of<br />
the heat through the <strong>capillary</strong> walls can result in higher<br />
temperatures in the center than at the walls. These temperature<br />
gradients cause viscosity differences of the running<br />
buffer and give rise to zone deformation. This is illustrated<br />
in figure 12 for a variety of inner diameter capillaries.<br />
Control of temperature differentials is critical since a one<br />
degree change in temperature results in a 2 to 3 % change<br />
in viscosity (and a 2 to 3 % change in mobility).<br />
The thermal gradient between the center of the <strong>capillary</strong><br />
and the surroundings is illustrated in figure 13. As shown,<br />
the temperature difference depends on the inner radius, the<br />
thickness of the wall, the thickness of the polyimide coating,<br />
and the heat transfer coefficient to the surroundings.<br />
Analytically this can be expressed by<br />
[ ( ) ( ) ( )]<br />
2<br />
Qr 1<br />
1 r 2<br />
1 r 3<br />
1 1<br />
DT T<br />
= 1n + 1n +<br />
2 k 1<br />
r 1<br />
k 2<br />
r 2<br />
r 3<br />
h<br />
(17)<br />
where:<br />
Q = power density<br />
r = radius<br />
k = thermal conductivity<br />
h = thermal transfer rate from the <strong>capillary</strong><br />
to the surrounding<br />
subscripts 1, 2, and 3 refer to the buffer,<br />
32