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Alphabetical    [«  »]
q 1
quaker 1
quantities 3
quantity 36
quarter 1
quay 1
question 10
Frequency    [«  »]
38 velocity
37 into
37 was
36 quantity
34 i
34 must
33 chemical
Hermann Ludwig Ferdinand von Helmholtz
On the Conservation of Force

IntraText - Concordances

quantity

   Part
1 I | question asserts, that the quantity of force which can be brought 2 I | you what is understood by quantity of force; or, as the same 3 I | countries is it present in any quantity; in level countries extensive 4 II | store of coal and the small quantity of water which are the sources 5 II | discussed we have seen that the quantity of force which can be produced 6 II | indestructible, and unchangeable in quantity, which is an essential fundamental 7 II | of natural processes, the quantity of heat which can be demonstrated 8 II | to colder bodies; but the quantity of heat which the former 9 II | state, exactly the same quantity of heat reappeared which 10 II | in containing a certain quantity of heat bound, which, just 11 II | vapour contains a far greater quantity of heat thus bound. But 12 II | experiments have shown that the quantity of heat which is developed 13 II | entirely unchangeable in quantity. The natural processes which 14 II | the invariability in the quantity of heat in all these processes 15 III| hand, he has determined the quantity of heat which is thereby 16 III| consumption of work, a definite quantity of work is required to produce 17 III| one degree centigrade. The quantity of work necessary for this 18 III| observers.~Thus then: a certain quantity of heat may be changed into 19 III| changed into a definite quantity of work; this quantity of 20 III| definite quantity of work; this quantity of work can also be retransformed 21 III| indeed, into exactly the same quantity of heat as that from which 22 III| is a new form in which a quantity of work may appear.~These 23 III| as a substance, for its quantity is not unchangeable. It 24 III| physicists to be the constant quantity of heat is nothing more 25 III| or fast, so also the same quantity of heat is produced by the 26 III| carbonic acid the entire quantity of carbon and the entire 27 III| of carbon and the entire quantity of oxygen, and also the 28 III| oxygen, a very considerable quantity of heat is produced; for 29 III| oxygen, though in far smaller quantity than by the aid of the battery 30 III| work.~If, now, a certain quantity of mechanical work is lost, 31 III| point show, an equivalent quantity of heat, or, instead of 32 III| lost, we gain an equivalent quantity of chemical or mechanical 33 III| reappears in exactly equivalent quantity in some other form; it is 34 III| remains in exactly the same quantity. We shall subsequently see 35 III| follows thence that the total quantity of all the forces capable 36 III| and locality without its quantity being changed. The universe


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