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| <h3 id="back-link"><a href="../#1.1">$\leftarrow$Back</a></h3> | | <h3 id="back-link"><a href="../#1.1">$\leftarrow$Back</a></h3> |
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| <h3> Statement </h3> | | <h3> Statement </h3> |
| <p> | | <p> |
| $1.1.22.$ Inside a fixed smooth-walled cylinder of radius $R$ a small ball is flying, elastically reflecting from the walls so that the minimal distance from it to the cylinder axis is $h$. What fraction of time is the distance from the cylinder axis less than $r$ but greater than $h$? | | $1.1.22.$ Inside a fixed smooth-walled cylinder of radius $R$ a small ball is flying, elastically reflecting from the walls so that the minimal distance from it to the cylinder axis is $h$. What fraction of time is the distance from the cylinder axis less than $r$ but greater than $h$? |
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| For problem $1.1.22$ | | For problem $1.1.22$ |
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| <h3>Solution</h3> | | <h3>Solution</h3> |
| <p> | | <p> |
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| <center> | | <center> |
| <figure> | | <figure> |
| <img src="animation.gif" alt="1.1.22" | | <img src="animation.gif" alt="1.1.22" |
| loading="lazy" width="250" /> | | loading="lazy" width="250" /> |
| <figcaption> | | <figcaption> |
| Impact on cylinder walls | | Impact on cylinder walls |
| </figcaption> | | </figcaption> |
| </figure> | | </figure> |
| </center> | | </center> |
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| <p> | | <p> |
| Let's consider the motion of the ball described in the problem condition | | Let's consider the motion of the ball described in the problem condition |
| </p> | | </p> |
| <center> | | <center> |
| <figure> | | <figure> |
| <img src="drawing.png" alt="1.1.22" | | <img src="drawing.png" alt="1.1.22" |
| loading="lazy" width="250" /> | | loading="lazy" width="250" /> |
| <figcaption> | | <figcaption> |
| The path of the ball between impacts | | The path of the ball between impacts |
| </figcaption> | | </figcaption> |
| </figure> | | </figure> |
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| <p> | | <p> |
| Since the impact velocity does not change between impacts, and impacts are absolutely elastic, we can consider the velocity unchanged. Consequently, for equal time intervals the body passes equal distances. | | Since the impact velocity does not change between impacts, and impacts are absolutely elastic, we can consider the velocity unchanged. Consequently, for equal time intervals the body passes equal distances. |
| </p> | | </p> |
| <p> | | <p> |
| Then the required ratio $\frac{\Delta t}{t}$ is found as the ratio $\frac{BC}{AD}$ | | Then the required ratio $\frac{\Delta t}{t}$ is found as the ratio $\frac{BC}{AD}$ |
| </p> | | </p> |
| <p style="text-align: center;"> | | <p style="text-align: center;"> |
| $$\frac{\Delta t}{t} = \frac{BC}{AD}$$ | | $$\frac{\Delta t}{t} = \frac{BC}{AD}$$ |
| </p> | | </p> |
| <p> | | <p> |
| By Pythagoras' theorem: | | By Pythagoras' theorem: |
| </p> | | </p> |
| <p style="text-align: center;"> | | <p style="text-align: center;"> |
| $BC = 2 \sqrt{r^2-h^2}$ | | $BC = 2 \sqrt{r^2-h^2}$ |
| </p> | | </p> |
| <p style="text-align: center;"> | | <p style="text-align: center;"> |
| $AD = 2 \sqrt{R^2-h^2}$ | | $AD = 2 \sqrt{R^2-h^2}$ |
| </p> | | </p> |
| <p> | | <p> |
| From where | | From where |
| </p> | | </p> |
| <p style="text-align: center;"> | | <p style="text-align: center;"> |
| $$\frac{BC}{AD} = \frac{\sqrt{r^2-h^2}}{\sqrt{R^2-h^2}}$$ | | $$\frac{BC}{AD} = \frac{\sqrt{r^2-h^2}}{\sqrt{R^2-h^2}}$$ |
| </p> | | </p> |
| <p> | | <p> |
| Or | | Or |
| </p> | | </p> |
| <p style="text-align: center;"> | | <p style="text-align: center;"> |
| $$\frac{\Delta t}{t} = \frac{\sqrt{r^2-h^2}}{\sqrt{R^2-h^2}}$$ | | $$\frac{\Delta t}{t} = \frac{\sqrt{r^2-h^2}}{\sqrt{R^2-h^2}}$$ |
| </p> | | </p> |
| </p> | | </p> |
| | | |
| <h4>Answer</h4> | | <h4>Answer</h4> |
| <p> | | <p> |
| $$\Delta t/t=\sqrt{(r^2-h^2)/(R^2-h^2)}$$ | | $$\Delta t/t=\sqrt{(r^2-h^2)/(R^2-h^2)}$$ |
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