1388. The following is a Table of results; the gas named is that in the vessel a. The smallest, greatest, and mean interval at u in air is expressed in parts of an inch, the interval v being constantly 0.62 of an inch.

Smallest.Greatest.Mean.
Air, s and S, pos.0.600.790.695
Air, s and S, neg.0.590.680.635
Oxygen, s and S, pos.0.410.600.505
Oxygen, s and S, neg.0.500.520.510
Nitrogen, s and S, pos.0.550.68 0.615
Nitrogen, s and S, neg.0.590.700.645
Hydrogen, s and S, pos.0.300.440.370
Hydrogen, s and S, neg.0.250.300.275
Carbonic acid, s and S, pos.0.560.720.640
Carbonic acid, s and S, neg.0.580.600.590
Olefiant gas, s and S, pos.0.640.860.750
Olefiant gas, s and S, neg.0.690.770.730
Coal gas, s and S, pos.0.37 0.610.490
Coal gas, s and S, neg.0.470.580.525
Muriatic acid gas, s and S, pos.0.891.321.105
Muriatic acid gas, s and S, neg.0.670.750.710

1389. The above results were all obtained at one time. On other occasions other experiments were made, which gave generally the same results as to order, though not as to numbers. Thus:

Hydrogen, s and S, pos.0.230.570.400
Carbonic acid, s and S, pos.0.511.050.780
Olefiant gas, s and S, pos.0.661.270.965

I did not notice the difference of the barometer on the days of experiment[273].

1390. One would have expected only two distances, one for each interval, for which the discharge might happen either at one or the other; and that the least alteration of either would immediately cause one to predominate constantly over the other. But that under common circumstances is not the case. With air in the receiver, the variation amounted to 0.2 of an inch nearly on the smaller interval of 0.6, and with muriatic acid gas, the variation was above 0.4 on the smaller interval of 0.9. Why is it that when a fixed interval (the one in the receiver) will pass a spark that cannot go across 0.6 of air at one time, it will immediately after, and apparently under exactly similar circumstances, not pass a spark that can go across 0.8 of air?

1391. It is probable that part of this variation will be traced to particles of dust in the air drawn into and about the circuit (1568.). I believe also that part depends upon a variable charged condition of the surface of the glass vessel a. That the whole of the effect is not traceable to the influence of circumstances in the vessel a, may be deduced from the fact, that when sparks occur between balls in free air they frequently are not straight, and often pass otherwise than by the shortest distance. These variations in air itself, and at different parts of the very same balls, show the presence and influence of circumstances which are calculated to produce effects of the kind now under consideration.

1392. When a spark had passed at either interval, then, generally, more tended to appear at the same interval, as if a preparation had been made for the passing of the latter sparks. So also on continuing to work the machine quickly the sparks generally followed at the same place. This effect is probably due in part to the warmth of the air heated by the preceding spark, in part to dust, and I suspect in part, to something unperceived as yet in the circumstances of discharge.

1393. A very remarkable difference, which is constant in its direction, occurs when the electricity communicated to the balls s and S is changed from positive to negative, or in the contrary direction. It is that the range of variation is always greater when the small bulls are positive than when they are negative. This is exhibited in the following Table, drawn from the former experiments.

Pos.Neg.
In Air the range was0.190.09
Oxygen0.190.02
Nitrogen0.180.11
Hydrogen0.140.05
Carbonic acid0.160.02
Olefiant gas 0.220.08
Coal gas0.240.12
Muriatic acid0.430.08