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Off-set Coaxial Cable - Capacitance |
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| Sep25-07, 11:50 AM | #1 |
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| Sep25-07, 12:03 PM | #2 |
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Hi,
Just to remind you the calculation for the coaxial cable case. The electric field of an infinite line of charge is given [tex]E = \frac{D}{\epsilon_0 \epsilon_r} = \hat{r} \frac{\rho_l}{2 \pi \epsilon_0 \epsilon_r r}[/tex] in radial direction. [tex]V = -\int_a^b Edl = \frac{Q}{2 \pi \epsilon_0 \epsilon_r}ln \frac{b}{a} [/tex] Finally, [tex]C = \frac{Q}{V} = \frac{2 \pi \epsilon_0 \epsilon_r}{ln \frac{b}{a}}[/tex] |
| Sep27-07, 05:00 AM | #3 |
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Can anyone help me???
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| Sep28-07, 03:46 PM | #4 |
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Off-set Coaxial Cable - Capacitance
boy, that is difficult (for me anyway, im probably at a similar level to you.)
As you said, [tex]C = \frac{Q}{V}[/tex] and, Q doesn't change depending on where you stick the inner conductor, right? I think this is right. The trouble is really the voltage. The capacitance of a coax cable is the capacitance between the inner and outer conductors, right? The only reason you can say something as simple as, "this cable's capacitance is 6pF/meter.", is because the conductor is square in the middle. Clearly, from the integral, Voltage (and therefore capacitance) changes as the conductors get further apart. For this example, that means that the capacitance of the line will vary depending on how you're looking at it, do you know what I mean? You won't just be able to say, this is a 6pF line. If you draw the cable on a coordinate axis, the capacitance will vary in theta. In short, find a function (of theta) that relates the distance from a to b. Integrate Edl from a to this function. the final answer will depend on theta. I think. |
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