another, and frequently with even a simple mechanical change of density (for instance by hammering), not to speak of allotropic changes, &c. We will cite several figures5 proving the truth of the conclusions arrived at by Dulong and Petit with respect to solid elementary bodies.
| Li | Na | Mg | P | ||||
|---|---|---|---|---|---|---|---|
| A = | 7 | 23 | 24 | 31 | |||
| Q = | 0·9408 | 0·2934 | 0·245 | 0·202 | |||
| AQ = | 6·59 | 6·75 | 5·88 | 6·26 | |||
| Fe | Cu | Zn | Br | ||||
| A = | 56 | 63 | 65 | 80 | |||
| Q = | 0·112 | 0·093 | 0·093 | 0·0843 | |||
| AQ = | 6·27 | 5·86 | 6·04 | 6·74 | |||
| Pd | Ag | Sn | I | ||||
| A = | 106 | 108 | 118 | 127 | |||
| Q = | 0·0592 | 0·056 | 0·055 | 0·0541 | |||
| AQ = | 6·28 | 6·05 | 6·49 | 6·87 | |||
| Pt | Au | Hg | Pb | ||||
| A = | 196 | 198 | 200 | 206 | |||
| Q = | 0·0325 | 0·0324 | 0·0333 | 0·0315 | |||
| AQ = | 6·37 | 6·41 | 6·66 | 6·49 |
It is seen from this that the product of the specific heat of the element into the atomic weight is an almost constant quantity, which is nearly 6. Hence it is possible to determine the valency by the specific heats of the metals. Thus, for instance, the specific heats of lithium, sodium, and potassium convince us of the fact that their atomic weights are indeed those which we chose, because by multiplying the specific heats found by experiment by the corresponding atomic weights we obtain the following figures: Li, 6·59, Na, 6·75 and K, 6·47. Of the alkaline earth metals the specific heats have been determined: of magnesium = 0·245 (Regnault and Kopp), of calcium = 0·170 (Bunsen), and of barium = 0·05 (Mendeléeff). If the same composition be ascribed to the compounds of magnesium as to the corresponding compounds of potassium, then the equivalent of magnesium will be equal to 12. On multiplying this atomic weight by the specific heat of magnesium, we obtain a figure 2·94, which is half that