Three long bands of fine oiled silk crape (each being effectively a plate of fine dry oil - impervious & insulating.) respectively 108 inches long and 6 1/2 inches wide[.]
Two similar bands of tin foil each 106 or 107 inches long and only 6 inches wide[.]
so that the oiled silk shall overlap the edges of the tin foil[.]
The compound band is then bent backwards and forwards thus
so as to make a packet 6 1/2 inches wide & 18 inches long which lies in the bottom of the box and yet is equivalent to 702 square inches of doubly coated surface or a square of 25 inches in the side - the induction being through a thickness no more than that of one oiled silk. Then by proper easy fittings one end of one of these plates is connected with the primary current wire on one side of the breaker & the other plate with the same current wire at the other side of the breaker - hence the good effect.
Ever dear Gassiot Truly yours | M. Faraday
17 Jany 1854
Endorsement: Grove PM. Vol 4 501 | 4 series1
Ruhmkorffs small coil
30 metres long
2 millime diameter
200 convolutions of the wire
2503 metres length
1/4 millim diameters
10,000 convolutions
Primary wire 2 1/2 mil. thick = .08 Inch
40 metres long about 1560 feet
300 turns
Secondary 1/3 mil. thick - .01 inch
70,000 metres 227,500 yds above 116 miles
30,000 turns
Millimetre = .03957 Inch
GASSIOT, John Peter (1854): “On some Experiments made with Ruhmkorff’s Induction Coil”, Phil. Mag., 7: 97-9.
GROVE, William Robert (1852b): “On the Electro-chemical Polarity of Gases”, Phil. Mag., 4: 498-515.
KATER, Henry (1818): “On the length of the French Mètre estimated in parts of the English standard”, Phil. Trans., 108: 103-9.
Please cite as “Faraday2777,” in Ɛpsilon: The Michael Faraday Collection accessed on 25 April 2024, https://epsilon.ac.uk/view/faraday/letters/Faraday2777