“The wide form of boiler with two coils within the envelope is not absolutely essential. The same amount of steam can be generated from one coil in an envelope in other respects equal to Diagram 1 if a sufficiently hot flame be passed axially through the coils. Such a flame, however, is unstable, and for this reason two milder flames with a good air access are to be preferred on practical grounds even if the weight is thereby increased. “To further understand the boiler construction it is advisable to consider the action of the flame. Inasmuch as wide tubes must be used, the problem of evaporating water as fast as possible is equivalent to getting heat into the current (water and steam circulating through the coils) as fast as possible from without. If, therefore, ‹t› is the mean temperature of the fluids within the coils, and ‹T› the effective temperature surrounding the tube, then the rate at which heat will flow into the tubes is proportional to ‹T›−‹t›. Now ‹t› the temperature of the steam is nearly constant (100°–150°) whereas ‹T› the effective flame temperature may vary from 800° to, say, 1600°. It is for this reason that the heat sponged up by the boiler depends almost directly on the flame temperature. “What conditions, therefore, will make the flame effectively hot? “(1) The coils must obviously be brought as nearly into the flame as feasible: for this purpose the cylindrical helix is better than any other form. But “(2) The turns and coils must not be so crowded together as to chill the flame into imperfect combustion in various parts of its extent. Hence the loose form of winding. Again “(3) There must be oxygen enough to allow complete combustion, and “(4) The flame itself must be hot and the radiation checked by good jacketing. “To take up the last points: the effective heat of the flame depends not only on the combustion heat of the fuel used; it depends also, among other things, on the speed with which this combustion takes place. A flame burning from a low pressure of alcohol gas will be at low temperature as compared with a flame burning from high pressures of the gas. If the flame be burnt from a Bunsen burner in the usual way it is an interesting question to know how flame temperature will vary with gas pressure. At present we know it merely in steam pressures incidently produced in a given engine (No. 4) as for instance: Flame pressure, 10 lbs., 20 lbs., 30 lbs. ┐ Steam pressure, 40 lbs., 80 lbs., 120 lbs. ┘ in the running engine.