Slike stranica
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CHAPTER V.

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vibrations. 59. With longitudinal vibrations. 60. Nodes. 61. Antinodes. 62. Verification from the equations. 63. Transverse vibrations. 64. Stationary undulation. 65, 66. Composition of undulations in different planes. 67. Effect of slight inequality of wave-length

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CHAPTER VI.

COMPOSITION OF TWO S.H. MOTIONS OF DIFFERENT PERIODS.

68. Motions at right angles with periods as I to 2. 69, 70. With periods as m to n. 71. Specimens of the curves. 72. Geometrical construction for them. 73. Periods approximately as m to n. 74. Experimental methods of tracing the curves; Blackburn's pendulum. 75, 76. Kaleidophone. 77. Tisley's pendulum apparatus. 78. Lissajous' experiment. 79. Optical tuning. 8o. Appearance as of curve on rotating cylinder. 81. Composition of two parallel S.H. motions represented by the ordinates of a curve. 82. Periods of components approximately as two small integers .

CHAPTER VII.

MECHANICAL ILLUSTRATIONS.

83. Subject of chapter. 84. Crank and slot. 85. Crank and connecting-rod. 86. Link motion for reversing. 87. New method of obtaining S.H. motion by jointed parallelogram. 88. Objection to another construction. 89. S.H. motion obtainable by one circle rolling inside another. 90. Another proof, showing that elliptic harmonic motion is also obtained. 91, 92. Two theoretical methods of obtaining S.H. motion. 93. Donkin's harmonograph for composition of two parallel S.H. motions. 94. Adaptation to the composition of two rectangular S.H. motions. 95, 96. Thomson's tide predicting machine.

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CHAPTER VIII.

PROPAGATION OF SONOROUS UNDULATIONS.

ΙΟΙ.

97. Propagation in air. 98. Co-efficient of elasticity. 99. Effect of
heat of compression. 100. Formula for velocity in air.
Effect of barometric and thermometric changes. 102. Open spaces,
and speaking tubes. 103. Liquids and solids. 104. Strings

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VIBRATORY

AND

MOTION

SOUND.

CHAPTER I.

SIMPLE HARMONIC VIBRATION.

1. WHEN the prongs of a tuning-fork are squeezed between the fingers and suddenly released, they spring back not only to their original position, but to a nearly equal distance on the other side, and swing backwards and forwards a great number of times before they finally come to rest. This is an example of vibration.

The time occupied in swinging from one side to the other and back again is called the periodic time, or the period of vibration, or simply the period; and the distance that any particle of the fork travels, first to one side and then to the other side of its position of equilibrium, is called the amplitude of vibration for this particle.

2. A tuning-fork, when well started, usually makes several thousand vibrations before coming to rest. Their amplitudes gradually decrease, and hence the sound

B

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