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| Alphabetical [« »] axis 1 axle 4 axles 2 b 21 b1 1 back 4 badly 1 | Frequency [« »] 23 law 23 may 22 four 21 b 21 carbon 21 no 21 now | Hermann Ludwig Ferdinand von Helmholtz On the Conservation of Force IntraText - Concordances b |
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1 I | precisely similar. Let "a b" be a simple lever, supported 2 I | supported at "c", the arm"c b" being four times as long 3 I | of one pound be hung at "b", and a weight of four pounds 4 II | of a spherical form: A B, a horizontal line drawn 5 II | swings beyond M towards b, where its motion stops 6 II | traversed on the side of B an arc equal in length to 7 II | has risen to a distance B b above the horizontal line, 8 II | has risen to a distance B b above the horizontal line, 9 II | previously raised it. In b the pendulum returns, swings 10 II | stop there, but ascends to b, in opposition to the action 11 II | raising it to an equal height, B b. The velocity of the moving 12 II | it to an equal height, B b. The velocity of the moving 13 II | another. In the points a and b the mass has no velocity; 14 II | weight goes further m to b the vis viva is changed 15 III| led from the points a and b. If the ends of these wires 16 III| stands in the copper spirals b b. Just over the top of 17 III| in the copper spirals b b. Just over the top of this 18 III| wire, traverses the spirals b b. The magnet c c is rigidly 19 III| traverses the spirals b b. The magnet c c is rigidly 20 III| iron core of the spirals b b, we should obtain in them 21 III| iron core of the spirals b b, we should obtain in them