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General Physics I:

Section 4.4 Examples B

Example 4.4.1.

A 10-kg block of wood rests on the top of a 20-kg block which rests on a horizontal surface. The lower block is then pulled to the right at constant speed by a horizontal force while the top block is held at rest by a horizontal string attached to it. If the coefficient of kinetic friction for bottom surfaces and coefficient of static friction between top surfaces are 0.25.
  1. what is the tension in the string, and
  2. the force pulling the bottom block?
Solution.
Given: \(m_{1} =10 kg, \quad m_{2} =20 kg,\) and \(\mu =0.25\text{.}\)
From figure,
in static equilibrium
\begin{equation*} \sum F_{x1} = f_{1}-T =0;\qquad \sum F_{y1} = N_{1}-w_{1} =0 \end{equation*}
\begin{equation*} w_{1} = m_{1}g; \qquad f_{1} = \mu N_{1} \end{equation*}
From figure,
in translational equilibrium along x-axis,
\begin{equation*} \sum F_{x2} = F-f_{1}-f_{2} =0 \end{equation*}
in static equilibrium along y-axis,
\begin{equation*} \sum F_{y2} = N_{2}-N_{1}-w_{2} =0 \end{equation*}
and
\begin{equation*} w_{2} = m_{2}g; \qquad f_{2} = \mu N_{2} \end{equation*}
Solving all these equations, we have -
\begin{equation*} w_{1} = m_{1}g = 98N; \end{equation*}
\begin{equation*} N_{1} =w_{1} =98N; \end{equation*}
\begin{equation*} f_{1} = \mu N_{1} = 24.5N; \end{equation*}
  1. \begin{equation*} \therefore \quad T = f_{1}= 24.5N \end{equation*}
    \begin{equation*} w_{2} = m_{2}g = 196N; \end{equation*}
    \begin{equation*} N_{2} =N_{1}+w_{2} =294N; \end{equation*}
    \begin{equation*} f_{2} = \mu N_{2} = 73.5N \end{equation*}
  2. \begin{equation*} \therefore\quad F = f_{1}+f_{2} = 98N \end{equation*}

Example 4.4.2.

A block of wood weighing 20 N is pulled to the right at constant speed up an inclined plane rising 10 cm per meter by a 10-N force making an angle of \(30^{o}\) above the plane. What is the coefficient of kinetic friction?
Solution.
Given: \(w =20N, \quad h =10 cm =0.1m, \quad L =1m, \quad F=10N,\) and \(\theta_{2}=30^{o}\text{.}\)
From figure From figure,
\begin{equation*} \sum F_{x} = F\cos\theta_{2}-f-w\sin\theta_{1} =0; \end{equation*}
\begin{equation*} \sum F_{y} = N+F\sin\theta_{2}-w\cos\theta_{1} =0 \end{equation*}
\begin{equation*} f = \mu N; \end{equation*}
\begin{equation*} \text{and}\quad \sin\theta_{1}=\frac{h}{L} \end{equation*}
on solving these equations, we get -
\begin{equation*} \sin\theta_{1}=\frac{h}{L}=0.1 \quad \Rightarrow \theta_{1} = 5.739^{o} \end{equation*}
\begin{equation*} f=F\cos\theta_{2}-w\sin\theta_{1} =6.660N \end{equation*}
\begin{equation*} N=w\cos\theta_{1}-F\sin\theta_{2}=14.90N \end{equation*}
\begin{equation*} \therefore\quad \mu= \frac{f}{N} =0.447 \end{equation*}