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A torsional pendulum involves the oscillation of a rigid body in which the restoring force is provided by the torsion in the string from which the rigid body is suspended. Ideally, the string should be massless; practically, its mass is much smaller than the rigid body's mass and is neglected.

As long as the rigid body's angular displacement is small, its oscillation can be modeled as a linear angular oscillation. The amplitude of the oscillation is an angle. The role of mass is played by the rigid body's moment of inertia about the point of suspension and the axis passing perpendicular to it.

Using the relationship between torque and angular acceleration, the equation is seen to mimic the equation of the simple harmonic motion of a simple pendulum. This observation allows for the easy determination of the angular frequency of the angular oscillation and its time period.

Tags
Torsional PendulumOscillationRigid BodyRestoring ForceTorsionAngular DisplacementLinear Angular OscillationAmplitudeMoment Of InertiaTorqueAngular AccelerationSimple Harmonic MotionAngular FrequencyTime Period

来自章节 15:

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15.9 : Torsional Pendulum

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15.1 : 简谐运动

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15.3 : 关于平衡位置的振荡

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15.7 : 问题解决:简谐运动中的能量

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15.8 : 单摆

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15.10 : 物理钟摆

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15.11 : 测量重力加速度

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15.12 : 阻尼振荡

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15.14 : 强制振荡

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15.15 : 共振的概念及其特性

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