A System of Mechanical Philosophy, Bindi 4J. Murray, 1822 - 50 síður |
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Síða 22
... side of B , the appearances will be reversed , and the bodies will attract each other with the force F'f ' X z - z ... side of B , it will be repelled ; and if on the overcharged side of B , it will be attracted . 39. Second , If the ...
... side of B , the appearances will be reversed , and the bodies will attract each other with the force F'f ' X z - z ... side of B , it will be repelled ; and if on the overcharged side of B , it will be attracted . 39. Second , If the ...
Síða 23
... side of B. B may be said to be NEU- TRAL with respect to A , although A and the adjoining side of B are both overcharged . 40. But if A be placed at the same distance on the other side of B , the effect will be very different : For ...
... side of B. B may be said to be NEU- TRAL with respect to A , although A and the adjoining side of B are both overcharged . 40. But if A be placed at the same distance on the other side of B , the effect will be very different : For ...
Síða 24
... so situated near the overcharged side of the electrophorus as to be neutral , it is repelled when brought nearer , but attracted when removed to a great dis- 1 tance . This shews that z increases faster than z 24 ELECTRICITY . ELECTRICITY ...
... so situated near the overcharged side of the electrophorus as to be neutral , it is repelled when brought nearer , but attracted when removed to a great dis- 1 tance . This shews that z increases faster than z 24 ELECTRICITY . ELECTRICITY ...
Síða 30
... side of n , and also by the attraction of the redundant matter on the side of s ; and the repulsion of the 30 ELECTRICITY .
... side of n , and also by the attraction of the redundant matter on the side of s ; and the repulsion of the 30 ELECTRICITY .
Síða 32
... side , and less undercharged in its remote side than if B were taken away . This must in- crease the inequability of distribution of the fluid in B , and both will be put farther from their natural state ; but A will never become ...
... side , and less undercharged in its remote side than if B were taken away . This must in- crease the inequability of distribution of the fluid in B , and both will be put farther from their natural state ; but A will never become ...
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action angle appear arch axis balance ball beats body canal centre coating concord conductor constipated cord curve cylinder Daniel Bernoulli degree density diameter diminished dipping needle direction distance effect elec electric fluid electrified electrometer electrophorus equal experiments explain farther force give glass globe greater harmony harpsichord headsails impulse inches increase length limma loadstone magnet major third manner mean tones motion moveable musical natural natural density nearly needle north pole observed octave overcharged pallet particle pendulum perfect perpendicular phenomena piece of iron pipe plate polarity position precisely produced proportion pulses quantity ratio reader redundant fluid redundant matter repel round sails scapement sensible shew ship side sound south pole stratum string suppose surface temperament tetrachords theory tion tooth touch tricity trumpet tune undercharged undulations velocity vibrations wheel whole wind wire