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| + | <meta name="author" content="Aliaksandr Melnichenka"> | ||
| + | <meta name="date" content="2023-10" scheme="YYYY-MM"> | ||
| + | <meta property="og:title" content="In one straight line on a smooth horizontal plane with equal intervals there are bars of mass m each. A constant horizontal force F is applied to the first of the bars. Determine the speed of the bars before and immediately after the nth impact. Consider the speed limit value for n tending to infinity, if the width of the gaps between the bars is l. The blows of the bars are absolutely inelastic."> | ||
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| + | <meta property="og:description" content="In one straight line on a smooth horizontal plane with equal intervals there are bars of mass m each. A constant horizontal force F is applied to the first of the bars. Determine the speed of the bars before and immediately after the nth impact. Consider the speed limit value for n tending to infinity, if the width of the gaps between the bars is l. The blows of the bars are absolutely inelastic."> | ||
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| + | <title>In one straight line on a smooth horizontal plane with equal intervals there are bars of mass m each. A constant horizontal force F is applied to the first of the bars. Determine the speed of the bars before and immediately after the nth impact. Consider the speed limit value for n tending to infinity, if the width of the gaps between the bars is l. The blows of the bars are absolutely inelastic.</title> | ||
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| + | <header style="text-align:center;"> | ||
| + | <h2>Solutions of Savchenko Problems in Physics</h2> | ||
| + | <p class="author"> | ||
| + | Aliaksandr Melnichenka <br/> | ||
| + | October 2023 | ||
| + | </p> | ||
| + | </header> | ||
| + | |||
| + | <h3 id="back-link"><a href="../#2.5">$\leftarrow$Back</a></h3> | ||
| + | |||
| + | <h3> Statement </h3> | ||
| + | <p> | ||
| + | $2.5.38^*.$ In one straight line on a smooth horizontal plane with equal intervals there are bars of mass $m$ each. A constant horizontal force $F$ is applied to the first of the bars. Determine the speed of the bars before and immediately after the nth impact. Consider the speed limit value for $n$ tending to infinity, if the width of the gaps between the bars is $l$. The blows of the bars are absolutely inelastic. | ||
| + | |||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="statement.png" | ||
| + | loading="lazy" width="280" /> | ||
| + | <figcaption> | ||
| + | For problem $2.5.38^*$ | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | </p> | ||
| + | |||
| + | <h3>Solution</h3> | ||
| + | <p> | ||
| + | Let's consider 1st and 2nd collision | ||
| + | <br> | ||
| + | <b>First collision</b>: | ||
| + | <br> | ||
| + | From the law of conservation of energy | ||
| + | $$v_1^2=2a_1l$$ | ||
| + | Considering Newton's 2nd law | ||
| + | $$v_1^2=\frac{2Fl}{m}$$ | ||
| + | Where $v_1$ is the velocity before the collision | ||
| + | <br> | ||
| + | Law of conservation of momentum | ||
| + | $$mv_1=2mv_1'$$ | ||
| + | $$v_1=\sqrt{\frac{Fl}{2m}}\quad\text{(1)}$$ | ||
| + | <b>Second collision</b>:<br> | ||
| + | From the law of conservation of energy | ||
| + | $$v_2^2=v_1^2+2a_2l$$ | ||
| + | Likewise, considering $a_2=\frac{F}{2m}$: | ||
| + | $$v_2^2=\frac{Fl}{2m}+\frac{Fl}{m}=\frac{3Fl}{2m}$$ | ||
| + | $$v_2=\sqrt{\frac{3Fl}{2m}}\quad\text{(2)}$$ | ||
| + | Where $v_2$ is the velocity after the collision | ||
| + | <br> | ||
| + | From $v_1$ and $v_2$, we can see that the velocity index is the same as the coefficient in front of the mass and $\text{index}+1$ at the top | ||
| + | <br> | ||
| + | Thus leading to the following recurrence relation | ||
| + | $$\boxed{v_n=\sqrt{\frac{El}{m}\left( 1+ \frac{1}{n} \right)}}\quad\text{(3)}$$ | ||
| + | Where $v_n$ is the velocity before the $n^\text{th}$ collision | ||
| + | <br> | ||
| + | Law of conservation of momentum of the $n^\text{th}$ collision | ||
| + | $$v_nmn=u_nm(n+1)$$ | ||
| + | $${u_n=\frac{1}{1+\frac{1}{n}}v_n}$$ | ||
| + | Substituting into the expression $\text{(3)}$: | ||
| + | $$\boxed{u_n=\sqrt{\frac{Fl}{m\left(1+\frac{1}{n}\right)}}}$$ | ||
| + | When $n\to\infty$, $\frac{1}{n}\to0$: | ||
| + | $$\lim_{n\to\infty}\frac{1}{n}=0$$ | ||
| + | Whence it follows that the velocity $u_n$ after $n^\text{th}$ collision, where $n\to\infty$, will be equal to | ||
| + | $$\boxed{u_n=\lim_{n\to\infty}\sqrt{\frac{Fl}{m\left(1+\frac{1}{n}\right)}}=\sqrt{\frac{Fl}{m}}}$$ | ||
| + | </p> | ||
| + | |||
| + | <h4>Answer</h4> | ||
| + | <p> | ||
| + | $$v_n=\sqrt{\frac{Fl}{m}(1+1/n)}$$ | ||
| + | $$u_n=\sqrt{\frac{Fl}{m(1+1/n)}}$$ | ||
| + | $$v_n\to\sqrt{\frac{Fl}{m}}\text{ with }n\to\infty.$$ | ||
| + | </p> | ||
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| <meta charset="utf-8"> | |||
| <meta name="viewport" content="width=device-width, initial-scale=1.0"> | |||
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| <meta name="author" content="Aliaksandr Melnichenka"> | |||
| <meta name="date" content="2023-10" scheme="YYYY-MM"> | |||
| <meta property="og:title" content="In one straight line on a smooth horizontal plane with equal intervals there are bars of mass m each. A constant horizontal force F is applied to the first of the bars. Determine the speed of the bars before and immediately after the nth impact. Consider the speed limit value for n tending to infinity, if the width of the gaps between the bars is l. The blows of the bars are absolutely inelastic."> | |||
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| <title>In one straight line on a smooth horizontal plane with equal intervals there are bars of mass m each. A constant horizontal force F is applied to the first of the bars. Determine the speed of the bars before and immediately after the nth impact. Consider the speed limit value for n tending to infinity, if the width of the gaps between the bars is l. The blows of the bars are absolutely inelastic.</title> | |||
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| </head> | |||
| <body style=""> | |||
| <header style="text-align:center;"> | |||
| <h2>Solutions of Savchenko Problems in Physics</h2> | |||
| <p class="author"> | |||
| Aliaksandr Melnichenka <br/> | |||
| October 2023 | |||
| </p> | |||
| </header> | |||
| <h3 id="back-link"><a href="../#2.5">$\leftarrow$Back</a></h3> | |||
| <h3> Statement </h3> | |||
| <p> | |||
| $2.5.38^*.$ In one straight line on a smooth horizontal plane with equal intervals there are bars of mass $m$ each. A constant horizontal force $F$ is applied to the first of the bars. Determine the speed of the bars before and immediately after the nth impact. Consider the speed limit value for $n$ tending to infinity, if the width of the gaps between the bars is $l$. The blows of the bars are absolutely inelastic. | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="statement.png" | |||
| loading="lazy" width="280" /> | |||
| <figcaption> | |||
| For problem $2.5.38^*$ | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| </p> | |||
| <h3>Solution</h3> | |||
| <p> | |||
| Let's consider 1st and 2nd collision | |||
| <br> | |||
| <b>First collision</b>: | |||
| <br> | |||
| From the law of conservation of energy | |||
| $$v_1^2=2a_1l$$ | |||
| Considering Newton's 2nd law | |||
| $$v_1^2=\frac{2Fl}{m}$$ | |||
| Where $v_1$ is the velocity before the collision | |||
| <br> | |||
| Law of conservation of momentum | |||
| $$mv_1=2mv_1'$$ | |||
| $$v_1=\sqrt{\frac{Fl}{2m}}\quad\text{(1)}$$ | |||
| <b>Second collision</b>:<br> | |||
| From the law of conservation of energy | |||
| $$v_2^2=v_1^2+2a_2l$$ | |||
| Likewise, considering $a_2=\frac{F}{2m}$: | |||
| $$v_2^2=\frac{Fl}{2m}+\frac{Fl}{m}=\frac{3Fl}{2m}$$ | |||
| $$v_2=\sqrt{\frac{3Fl}{2m}}\quad\text{(2)}$$ | |||
| Where $v_2$ is the velocity after the collision | |||
| <br> | |||
| From $v_1$ and $v_2$, we can see that the velocity index is the same as the coefficient in front of the mass and $\text{index}+1$ at the top | |||
| <br> | |||
| Thus leading to the following recurrence relation | |||
| $$\boxed{v_n=\sqrt{\frac{El}{m}\left( 1+ \frac{1}{n} \right)}}\quad\text{(3)}$$ | |||
| Where $v_n$ is the velocity before the $n^\text{th}$ collision | |||
| <br> | |||
| Law of conservation of momentum of the $n^\text{th}$ collision | |||
| $$v_nmn=u_nm(n+1)$$ | |||
| $${u_n=\frac{1}{1+\frac{1}{n}}v_n}$$ | |||
| Substituting into the expression $\text{(3)}$: | |||
| $$\boxed{u_n=\sqrt{\frac{Fl}{m\left(1+\frac{1}{n}\right)}}}$$ | |||
| When $n\to\infty$, $\frac{1}{n}\to0$: | |||
| $$\lim_{n\to\infty}\frac{1}{n}=0$$ | |||
| Whence it follows that the velocity $u_n$ after $n^\text{th}$ collision, where $n\to\infty$, will be equal to | |||
| $$\boxed{u_n=\lim_{n\to\infty}\sqrt{\frac{Fl}{m\left(1+\frac{1}{n}\right)}}=\sqrt{\frac{Fl}{m}}}$$ | |||
| </p> | |||
| <h4>Answer</h4> | |||
| <p> | |||
| $$v_n=\sqrt{\frac{Fl}{m}(1+1/n)}$$ | |||
| $$u_n=\sqrt{\frac{Fl}{m(1+1/n)}}$$ | |||
| $$v_n\to\sqrt{\frac{Fl}{m}}\text{ with }n\to\infty.$$ | |||
| </p> | |||
| <footer class="row container"> | |||
| <br> | |||
| <p> | |||
| <small> © <strong>Savchenko Solutions</strong>, 2023-2024 <br></small> | |||
| </p> | |||
| <p> | |||
| <small>All rights belong to the authors. <br> Commercial use of materials - with the written permission of the authors. <br> astrosander01@gmail.com <br></small> | |||
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