Решение до правки #2546 от , автор astrosander. Это не текущая версия.
For problem $2.7.6$
Savchenko Solutions

Solutions of Savchenko Physics Textbook

Aliaksandr Melnichenka
October 2023

    <h3 id="back-link"><a href="/#2.7">$\leftarrow$Back</a></h3>

    <h3> Statement </h3>
    <p>
        $2.7.6.$ A thin-walled cylinder of radius $R$ was spun up to an angular velocity $\omega$ and placed in a corner, as shown in the figure. The coefficient of friction between the corner walls and the cylinder is $\mu$. How many revolutions will the cylinder make before it comes to a complete stop?

For problem

    <h3>Solution</h3>
    <p>
        

Forces acting on the cylinder

Conditions of equilibrium:
Missing or unrecognized delimiter for \left\left{\begin{matrix} O'X\text{: }F_{fr2} = N_1 \ O'Y\text{: }F_{fr1}+N_2 = mg \ \end{matrix}\right.
From where
Missing or unrecognized delimiter for \left\left{\begin{matrix} \mu N_2=N_1 \ \mu N_1+N_2=mg \ \end{matrix}\right.
Let's find friction force

Considering, :

According to rotational motion dynamics, the sum of moments of external forces can be written as

From where, absolute value of angular acceleration is found as



The angle by which the cylinder will rotate to the moment of total stop is

Until the total stop, the cylinder will make total turnovers

From where


    <h4>Answer</h4>
    <p>
        $$N=\omega^{2}R(1+\mu^{2})/[4\pi g\mu(1+\mu)]$$
    </p>
    <p style="text-align: right; font-style: italic; font-size: 14;">   
      Yuldashev Ulugbek<br>
    </p>


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