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+ <meta name="description" content="In case of an elastic impact of a body against a fixed wall, its velocity v changes only in the direction. Determine the change after the impact of the velocity of this body, if the wall is moving: a) at a speed u towards the body; b) at a speed w < v in the direction of movement of the body.">
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+ <meta name="date" content="2023-10" scheme="YYYY-MM">
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+ <title>In case of an elastic impact of a body against a fixed wall, its velocity v changes only in the direction. Determine the change after the impact of the velocity of this body, if the wall is moving: a) at a speed u towards the body; b) at a speed w < v in the direction of movement of the body.</title>
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+ <h2>Solutions of Savchenko Problems in Physics</h2>
+ <p class="author">
+ Aliaksandr Melnichenka <br/>
+ October 2023
+ </p>
+ </header>
+
+ <h3 id="back-link"><a href="../../#1.4">$\leftarrow$Back</a></h3>
+
+ <h3> Statement </h3>
+ <p>
+ $1.4.8.$ In case of an elastic impact of a body against a fixed wall, its velocity $v$ changes only in the direction. Determine the change after the impact of the velocity of this body, if the wall is moving: a) at a speed $u$ towards the body; b) at a speed $w < v$ in the direction of movement of the body.
+
+</p>
+<center>
+ <figure>
+ <img src="https://savchenkosolutions.com/1/1.4.8/statement.png"
+ loading="lazy" width="180" />
+ <figcaption>
+ For problem $1.4.8$
+ </figcaption>
+ </figure>
+</center>
+<p>
+ </p>
+
+ <h3>Solution</h3>
+ <p>
+ <p>The whole point of the problem is to move to an inertial system associated with the wall, correctly describing the relative velocity.</p>
+<p>$a)$ In the case when the wall "catches up" with the ball, it is necessary to move to a frame of reference in which the wall is at rest.</p>
+<p>In this frame of reference, the relative velocity of the ball before the impact is</p>
+<p class="exp">$$v_{0} + u$$</p>
+<p>After the elastic impact, the velocity projection changes sign: it becomes equal to </p>
+<p class="exp">$$(- v_{0} - u)$$</p>
+<p>If we then return to the original (laboratory) frame of reference, where the wall moves with a velocity of $u$, then the velocity of the ball here is </p>
+<p class="exp">
+$${v}' = - v_{0} - 2u$$</p>
+<p>The change in velocity in this case is </p>
+<p class="exp">
+$$\fbox{$\Delta v = {v}' - v_{0}$ $= - 2(v_{0} + u)$}$$
+</p>
+<p>$b)$ Similarly, we need to go to the frame of reference in which the wall is at rest. </p>
+<p>In this frame of reference, the relative velocity of the ball before the impact is $v_{0} - w$. After the elastic impact, the projection of the velocity changes sign: it becomes equal to </p>
+<p class="exp">
+$$(- v_{0} + w)$$
+</p>
+<p>If we then return to the original (laboratory) frame of reference, where the wall moves with the velocity $w$, then the velocity of the ball is </p>
+<p class="exp">
+$${v}' = - v_{0} + 2w$$
+</p>
+<p>The change in velocity in this case is </p>
+<p class="exp">
+$$\fbox{$\Delta v = {v}' - v_{0}$ $= - 2(v_{0} - w)$}$$
+</p>
+ </p>
+
+ <h4>Answer</h4>
+ <p>
+ $\begin{aligned}&{a) }\Delta v = -2(v + u).\quad б) \Delta v = -2(v - w). (\text{Projection on the direction of the initial}\\&\text{speeds are considered positive.)}\end{aligned}$
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