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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

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