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# Exploration 26.5: Capacitance of Concentric Cylinders

Please wait for the animation to completely load.

Wait for the calculation to finish. This animation shows a coaxial capacitor with cylindrical geometry: a very long cylinder (extending into and out of the page) in the center surrounded by a very long cylindrical shell** (position is given in centimeters, electric field strength is given in newtons/coulomb, and electric potential is given in volts)**. The outside shell is grounded, while the inside shell is at 10 V. You can click-drag to measure the voltage at any position. Restart.

- Use Gauss's law to show that the magnitude of the radial electric field between the two conductors for a cylindrical coaxial capacitor of length L is E = Q/2πrLε
_{0}= 2kQ/(rL), where Q is the total charge on the inside (or outside) conductor and r is the distance from the center. - If L = 1 m, measure the electric field in the region between the two conductors and determine the charge on the inside (and outside) conductor.
- Use V = -∫
**E ·**d**r**to show that the potential at any point between the two conductors is V = (Q/2πLε_{0}) ln(b/r) = (2kQ/L) ln(b/r), where b is the radius of the outer conductor. - Given that the potential difference between the two cylinders is 10 V, verify your answer to (b) and find the charge on each conductor.
- Given, then, that the potential difference between the two conductors is V = (Q/2πLε
_{0}) ln(b/a) = (2Qk/L) ln(b/a)–b is the radius of the outer shell and a is the radius of the inner cylinder—show that the capacitance of this capacitor is (2πLε_{0})/ln(b/a) = (L/2k)/ln(b/a). - What is the capacitance (numerical value) of this capacitor?

Exploration authored by Anne J. Cox.

Script authored by Mario Belloni, Wolfgang Christian and Anne J. Cox.

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