October 9
He made the last measurements of the change of capacity of a sphere with height on October 5th, but did not give the calculation results. He subsequently improved the apparatus as a whole and in the present entry describes a different way of connecting the âspecial coilâ, the chief effect of which was to loosen the coupling, which immediately proved its advantages. With weaker excitation it was easier to adjust the âspecial coilâ to resonance because there were no streamers. Parasitic capacities were reduced, mainly to the distributed capacity of the âspecial coilâ.
Tesla first determined the distributed capacity of the âspecial coilâ. He assumed that the ball circuit resonated at Ï0, determined by the primary circuit, so that one can write
Lp1Cp = Lsc (c + C)
where Lp1 and Cp are the total inductance (including the regulating coil) and capacity of the primary circuit, Lsc is the inductance of the âspecial coilâ (including connecting wires), C is the distributed or parasitic capacity of the âspecial coilâ, and c the capacity of the ball.
Subsequent changes in the height of the ball changed the capacity in the circuit of the âspecial coilâ. To bring the oscillator into resonance with this circuit again, Tesla changed the inductance in the primary circuit. When resonance is achieved, according to Tesla, one can write
Lp2Cp = Lsc (c' + C)
Dividing this by the preceding equation yields
c' = $! {{L_{p}}_{2} \over {L_{p}}_{1}} $! (c + C) - C
which is in fact the equation Tesla uses to find c'. Because of an arithmetical error in calculating C, Tesla's numerical results for the ball capacity are about 10% higher than they should be, but this does not essentially affect the conclusions. To calculate the distributed capacity of the coil** he uses the relation LpCp = Lsc (C + c) for the ball at