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en/10.1.29.md
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| + | ### Statement | ||
| + | |||
| + | $10.1.29.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | The proof here will be very brief, referring to the solution of problem 10.1.24, the value of the invariant for the spiral trajectory was derived.: | ||
| + | |||
| + | $$\frac{Be(d^2-R^2)}{2} = const$$ | ||
| + | |||
| + | Where $d$ is the distance from the side circle to the axis of the main orbit, with $d=0$ this equality inevitably follows: | ||
| + | |||
| + | $$BR^2 = const$$ | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
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| ### Statement | |||
| $10.1.29.$ [Insert the problem statement] | |||
| ### Solution | |||
| The proof here will be very brief, referring to the solution of problem 10.1.24, the value of the invariant for the spiral trajectory was derived.: | |||
| $$\frac{Be(d^2-R^2)}{2} = const$$ | |||
| Where $d$ is the distance from the side circle to the axis of the main orbit, with $d=0$ this equality inevitably follows: | |||
| $$BR^2 = const$$ | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||