Vibratory Motion and SoundLongmans, Green, 1882 - Broj stranica: 135 |
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Stranica 4
... perpendicular to the path be drawn from the particle , the point in which this perpendicular meets the circle will travel round the circle with uniform velocity . The circle so described is called the auxiliary circle . 6. The greatest ...
... perpendicular to the path be drawn from the particle , the point in which this perpendicular meets the circle will travel round the circle with uniform velocity . The circle so described is called the auxiliary circle . 6. The greatest ...
Stranica 5
... perpendicular to the sides of the triangle C Y P , which may therefore be taken as the triangle of velocities . Hence CY represents the velocity of x . and , since P and x have identical motions in SIMPLE HARMONIC MOTION . 5.
... perpendicular to the sides of the triangle C Y P , which may therefore be taken as the triangle of velocities . Hence CY represents the velocity of x . and , since P and x have identical motions in SIMPLE HARMONIC MOTION . 5.
Stranica 10
... perpendicular to the plane of vibra- tion . 14. To show that the vibrations of a pendulum follow the simple harmonic law , it will suffice to consider the case of the simple pendulum , that is , of a heavy particle suspended by a ...
... perpendicular to the plane of vibra- tion . 14. To show that the vibrations of a pendulum follow the simple harmonic law , it will suffice to consider the case of the simple pendulum , that is , of a heavy particle suspended by a ...
Stranica 19
... perpendicular to it equal and opposite . Their resultant will therefore be S.H. motion along this dia- meter , with amplitude double the radius of either circle . 27. When the two circular motions in opposite direc- tions have unequal ...
... perpendicular to it equal and opposite . Their resultant will therefore be S.H. motion along this dia- meter , with amplitude double the radius of either circle . 27. When the two circular motions in opposite direc- tions have unequal ...
Stranica 20
... perpendicular direction will be the difference of two S.H. motions of the same epoch , and will be s.H. motion of amplitude a - b . The final resultant will therefore be obtained by com- pounding two S.H. motions of amplitudes a + b and ...
... perpendicular direction will be the difference of two S.H. motions of the same epoch , and will be s.H. motion of amplitude a - b . The final resultant will therefore be obtained by com- pounding two S.H. motions of amplitudes a + b and ...
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amplitude approximately axis boards Books Cabinet Edition called centre Chapter Church circle circular cloth component compound compression constant continued Crown 8vo curve denote described difference direction displacement distance double Edition elasticity ellipse energy English epoch equal equation Essays extension extreme figure fixed force fork given gives half Hence History horizontal Illustrations increase length Maps maximum mean middle moving nearly nodes obtained opposite directions original parallel particle pendulum period perpendicular phase pipe pitch places plane Plates position present produce projection propagation ratio reflected regarded represented resultant revolving right angles round S.H. motions Series shows sides simple harmonic motion sound square straight line string tion tone traced Translated travelling undulations uniform velocity vertical vibrations vols wave-length waves whole Woodcuts
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