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Physics · 术语表

什么是 Solid; rotation about a fixed axis?

Definition 19.9 University Physics — Year 1 · 第 19 章 — Systems of Points; Introduction to Rigid Bodies

A rigid body (solid) is a system whose points keep fixed mutual distances. If it turns about an axis Δ\Delta fixed in the frame, every point describes a circle centered on Δ\Delta at the same angular velocity ω=θ˙\omega = \dot\theta; a point at distance rir_i from the axis has speed riωr_i\omega.

Left: the moment of inertia of a disk, summed ring by ring. Right: Huygens’ theorem — about an axis through the rim of a disk, parallel to the axis through its center, J = 1/2 MR2 + MR2.
Left: the moment of inertia of a disk, summed ring by ring. Right: Huygens’ theorem — about an axis through the rim of a disk, parallel to the axis through its center, J=12MR2+MR2J = \tfrac12 MR^2 + MR^2.
Three solids in motion: a compound pendulum swinging about a pivot (moment of the weight about the axis), a torsion pendulum (moment of the wire), and a solid rolling without slipping down an incline — the larger its J/MR2, the slower it rolls.
Three solids in motion: a compound pendulum swinging about a pivot (moment of the weight about the axis), a torsion pendulum (moment of the wire), and a solid rolling without slipping down an incline — the larger its J/MR2J/MR^2, the slower it rolls.

示例

Example 19.12 (Compound pendulum; torsion pendulum)

A solid of mass MM pivoting about a horizontal axis at distance dd from GG: the weight’s moment is −Mgdsin⁡θ-Mgd\sin\theta, so JΔθ¨=−Mgdsin⁡θJ_\Delta\ddot\theta = -Mgd\sin\theta and small swings have the period

T=2πJΔMgd,T = 2\pi\sqrt{\frac{J_\Delta}{Mgd}} ,

that of a simple pendulum of length JΔ/MdJ_\Delta/Md — for a uniform rod pivoted at one end, 2L/32L/3. A disk hung from a wire of torsion constant CC (restoring moment −Cθ-C\theta): Jθ¨=−CθJ\ddot\theta = -C\theta, T=2πJ/CT = 2\pi\sqrt{J/C} — the torsion balance that measured GG and Coulomb’s law.

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