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From the Rolls-Royce experimental archive: a quarter of a million communications from Rolls-Royce, 1906 to 1960's. Documents from the Sir Henry Royce Memorial Foundation (SHRMF).
Page of calculations for the electric potential and force between cylindrical conductors.

Identifier  ExFiles\Box 54\3\  Scan233
Date  16th July 1924
  
EFC1/T16.7.24. -2- Contd.

The excess of potential (V) of the central wire over that of the outer conducting cylinder will then, by the definition of potential (as work done on unit charge) be

∫ from b to a (2e/r) dr = [ 2 e log_e r ] from a to b

i.e. V = 2e log_e (b/a)

Hence e = V / (2 log_e (b/a))

Hence the electric force at radius r

2e/r . V / (2 log_e (b/a)) = V / (r log_e (b/a))

At radius a, i.e. just off the surface of the wire it is

V / (a log_e (b/a))

and at radius b it is

V / (b log_e (b/a))

The former of the two is the larger, because a is smaller than b.

If while b and V are constant a increases, 1/a diminishes but 1 / log_e(b/a) increases, so that the electric force

V / (a log_e (b/a))

just off the surface of the wire, may increase or diminish as a increases, according to circumstances.

Contd.
  
  


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