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| Alphabetical [« »] varying 1 vegetable 3 vegetation 1 velocity 38 verge 1 vertical 1 very 14 | Frequency [« »] 43 motion 41 been 40 other 38 velocity 37 into 37 was 36 quantity | Hermann Ludwig Ferdinand von Helmholtz On the Conservation of Force IntraText - Concordances velocity |
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1 I | another with greater or less velocity; of changing the rotating 2 I | uniform into those of varying velocity, and so forth. Hence this 3 I | that in proportion as the velocity of the motion increases 4 I | the power increases the velocity diminishes, but that the 5 I | strikes with considerable velocity. It is the velocity of the 6 I | considerable velocity. It is the velocity of the water, exerting an 7 I | instance of the action of velocity. The sails are driven by 8 I | force depends here on the velocity of moving masses.~A bullet 9 I | fired and endowed with great velocity it drives through all obstacles 10 I | allow it to fall with great velocity, it acquires a new force, 11 II | Part II - Velocity And Motive Force~These examples 12 II | examples teach us that the velocity of a moving mass can act 13 II | motive force. In mechanics, velocity in so far as it is motive 14 II | and of the bullet, that velocity is lost, as such, when it 15 II | prove that part of their velocity has been lost by the work 16 II | performed.~The relation of velocity to working power is most 17 II | arrives there with a certain velocity, and no longer remains quietly 18 II | only to be sought in its velocity. The velocity which it has 19 II | sought in its velocity. The velocity which it has acquired in 20 II | an equal height, B b. The velocity of the moving mass, M, is 21 II | if we had imparted such a velocity to the suspended weight 22 II | measure the working power of velocity or, what is the same thing, 23 II | mass can exert after its velocity has been used to raise it, 24 II | on the direction of the velocity; for if we swing a weight 25 II | a and b the mass has no velocity; at the point M it has fallen 26 II | possible, but possesses velocity. As the weight goes from 27 II | it force in the form of velocity. To stretch the cord my 28 II | and impart to it a great velocity, which we have already seen 29 II | continues to roll until its velocity is destroyed by friction 30 II | height has acquired a certain velocity on reaching the earth; this 31 II | mechanical work; so long as this velocity continues as such, we can 32 II | impact has destroyed its velocity, and therewith apparently 33 II | mechanical work which this velocity could have affected.~If 34 II(2)| weight into the square of the velocity. To reduce it to the technical 35 II(2)| gravity; that is, by the velocity at the end of the first 36 III | to expand with moderate velocity becomes cooled. Joule was 37 III | doing it becomes loose. The velocity of a moving mass can do 38 III | work, it either acquired velocity or produced heat. We might