equation 33.10 eq:expcav-torque
open in the book ·
parts/03-classical-mechanics/16-exp-cavendish.tex:394
- part of a statement or proof
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Supports
- depends_on proposition 33.9 The time-of-swing method ¶
- depends_on remark 33.14 Why shrinking the balance costs no sensitivity ¶
- step_from equation 33.11 eq:expcav-theta-solved ¶
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Edges
| type | direction | node | provenance | where |
|---|---|---|---|---|
depends_on |
← | The time-of-swing method | declared | parts/03-classical-mechanics/16-exp-cavendish.tex:488 |
depends_on |
← | Why shrinking the balance costs no sensitivity | declared | parts/03-classical-mechanics/16-exp-cavendish.tex:1000 |
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 |