equation 33.6 eq:expcav-torsion-period

open in the book · parts/03-classical-mechanics/16-exp-cavendish.tex:309

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equation 33.6: eq:expcav-torsion-period33.6equation 33.5: eq:expcav-torsion-eom33.5equation 9.108: eq:slt-helmholtz-real9.108experiment : The Cavendish Torsion Balanceexperime…proposition 33.6: The working formula of the torsion balance33.6remark 33.5: Why the fibre must be fine, quantitatively33.5equation 33.11: eq:expcav-theta-solved33.11proposition 33.9: The time-of-swing method33.9phenomenon 33.4: A twisted fibre restores in proportion to the twist33.4equation 33.1: eq:expcav-newton-law33.1phenomenon 33.12: The Earth is much denser than its crust33.12proof : ch:16-exp-cavendish@proof-4proofequation 33.10: eq:expcav-torque33.10

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step_from eq:expcav-torsion-eom declared — reading off $\omega=\sqrt{\kappa/I}$ from the harmonic solution and inverting $T=2\pi/\omega$ parts/03-classical-mechanics/16-exp-cavendish.tex:313
step_from eq:slt-helmholtz-real declared — reading off $\omega=\sqrt{\kappa/I}$ from the harmonic solution and inverting $T=2\pi/\omega$ parts/03-classical-mechanics/16-exp-cavendish.tex:313
assumes The Cavendish Torsion Balance declared parts/03-classical-mechanics/16-exp-cavendish.tex:4
depends_on The working formula of the torsion balance declared parts/03-classical-mechanics/16-exp-cavendish.tex:385
depends_on Why the fibre must be fine, quantitatively declared parts/03-classical-mechanics/16-exp-cavendish.tex:347
step_from eq:expcav-theta-solved declared — substituting $\kappa=4\pi^{2}I/T^{2}$ with $I=2md^{2}$, so that $m$ cancels between torque and inertia parts/03-classical-mechanics/16-exp-cavendish.tex:406