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Development of a Oxygen Sensor for Marine ... - DTU Nanotech

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3.1. CHEMISTRY OF THE CLARK SENSOR 17<br />

PSfrag replacements<br />

y<br />

Cathode<br />

Membrane Liquid<br />

x = 0 x = dm<br />

Figure 3.3: One layer electrode model to illustrate the three assumptions, as<br />

well as to help derive the equations based on them.<br />

Using Fick’s second law and the coordinate system from Figure 3.3, the<br />

unsteady diffusion in the membrane will be described by:<br />

∂p<br />

∂t<br />

∂<br />

= Dm<br />

2p ∂x2 p0<br />

x<br />

(3.1)<br />

Where Dm is the oxygen diffusivity in the membrane, p the partial pressure<br />

<strong>of</strong> oxygen in the membrane, and x is the distance from the cathode<br />

surface.<br />

Under the assumption that diffusion have yet to take place, the initial<br />

boundary conditions are:<br />

p = 0 at t = 0 (3.2)<br />

p = 0 at x = 0 (3.3)<br />

p = p0 at x = dm<br />

(3.4)<br />

where dm is the membrane thickness and po is the partial pressure <strong>of</strong> oxygen<br />

in the bulk liquid.

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