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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

   Part
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


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