LAWS OF FRICTION
Laws of Motion

270381 A\(2 \mathbf{k g}\) block is placed over a \(4 \mathbf{k g}\) block and both are placed on a smooth horizontal surface. The coefficient of friction between the blocks is 0.20 . The acceleration of the two blocks if a horizontal force of \(12 \mathrm{~N}\) is applied to the lower block is \(\left(\mathrm{g}=10 \mathrm{~ms}^{-2}\right)\)

1 \(2 \mathrm{~ms}^{-2}, 2 \mathrm{~ms}^{-2}\)
2 \(2 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
3 \(3 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
4 \(4 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
Laws of Motion

270382 Blocks\(A\) and \(B\) shown in the figure are connected with a bar of negligible weight. A and \(B\) each has mass \(170 \mathrm{Kg}\), the coefficient of friction between \(A\) and the plane is 0.2 and that between \(B\) and the plane is 0.4 . What is the total force of friction between the blocks and the plane \(\left(g=10 \mathrm{~ms}^{-2}\right)\)

1 900N
2 700N
3 600N
4 300N
Laws of Motion

270383 From the above problem what is the force acting on the connectingbar ?

1 \(150 \mathrm{~N}\)
2 \(100 \mathrm{~N}\)
3 \(75 \mathrm{~N}\)
4 \(125 \mathrm{~N}\)
Laws of Motion

270384 A block of mass \(m\), lying on a rough horizontal plane is acted upon by a horizontal force \(P\) and another force \(Q\), inclined at an angle \(\theta\) with vertical. The block will remain in equilibrium, if coefficient of friction between it and surface is

1 \(\frac{(\mathrm{P}+Q \sin \theta)}{(m g+Q \cos \theta)}\)
2 \(\cdot \frac{(\mathrm{P} \cos \theta+Q)}{(m g-Q \sin \theta)}\)
3 \(\frac{(\mathrm{P}+Q \cos \theta)}{(m g+Q \sin \theta)}\)
4 \(\frac{(\mathrm{P} \sin \theta-Q)}{(m g-Q \cos \theta)}\)
Laws of Motion

270381 A\(2 \mathbf{k g}\) block is placed over a \(4 \mathbf{k g}\) block and both are placed on a smooth horizontal surface. The coefficient of friction between the blocks is 0.20 . The acceleration of the two blocks if a horizontal force of \(12 \mathrm{~N}\) is applied to the lower block is \(\left(\mathrm{g}=10 \mathrm{~ms}^{-2}\right)\)

1 \(2 \mathrm{~ms}^{-2}, 2 \mathrm{~ms}^{-2}\)
2 \(2 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
3 \(3 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
4 \(4 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
Laws of Motion

270382 Blocks\(A\) and \(B\) shown in the figure are connected with a bar of negligible weight. A and \(B\) each has mass \(170 \mathrm{Kg}\), the coefficient of friction between \(A\) and the plane is 0.2 and that between \(B\) and the plane is 0.4 . What is the total force of friction between the blocks and the plane \(\left(g=10 \mathrm{~ms}^{-2}\right)\)

1 900N
2 700N
3 600N
4 300N
Laws of Motion

270383 From the above problem what is the force acting on the connectingbar ?

1 \(150 \mathrm{~N}\)
2 \(100 \mathrm{~N}\)
3 \(75 \mathrm{~N}\)
4 \(125 \mathrm{~N}\)
Laws of Motion

270384 A block of mass \(m\), lying on a rough horizontal plane is acted upon by a horizontal force \(P\) and another force \(Q\), inclined at an angle \(\theta\) with vertical. The block will remain in equilibrium, if coefficient of friction between it and surface is

1 \(\frac{(\mathrm{P}+Q \sin \theta)}{(m g+Q \cos \theta)}\)
2 \(\cdot \frac{(\mathrm{P} \cos \theta+Q)}{(m g-Q \sin \theta)}\)
3 \(\frac{(\mathrm{P}+Q \cos \theta)}{(m g+Q \sin \theta)}\)
4 \(\frac{(\mathrm{P} \sin \theta-Q)}{(m g-Q \cos \theta)}\)
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Laws of Motion

270381 A\(2 \mathbf{k g}\) block is placed over a \(4 \mathbf{k g}\) block and both are placed on a smooth horizontal surface. The coefficient of friction between the blocks is 0.20 . The acceleration of the two blocks if a horizontal force of \(12 \mathrm{~N}\) is applied to the lower block is \(\left(\mathrm{g}=10 \mathrm{~ms}^{-2}\right)\)

1 \(2 \mathrm{~ms}^{-2}, 2 \mathrm{~ms}^{-2}\)
2 \(2 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
3 \(3 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
4 \(4 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
Laws of Motion

270382 Blocks\(A\) and \(B\) shown in the figure are connected with a bar of negligible weight. A and \(B\) each has mass \(170 \mathrm{Kg}\), the coefficient of friction between \(A\) and the plane is 0.2 and that between \(B\) and the plane is 0.4 . What is the total force of friction between the blocks and the plane \(\left(g=10 \mathrm{~ms}^{-2}\right)\)

1 900N
2 700N
3 600N
4 300N
Laws of Motion

270383 From the above problem what is the force acting on the connectingbar ?

1 \(150 \mathrm{~N}\)
2 \(100 \mathrm{~N}\)
3 \(75 \mathrm{~N}\)
4 \(125 \mathrm{~N}\)
Laws of Motion

270384 A block of mass \(m\), lying on a rough horizontal plane is acted upon by a horizontal force \(P\) and another force \(Q\), inclined at an angle \(\theta\) with vertical. The block will remain in equilibrium, if coefficient of friction between it and surface is

1 \(\frac{(\mathrm{P}+Q \sin \theta)}{(m g+Q \cos \theta)}\)
2 \(\cdot \frac{(\mathrm{P} \cos \theta+Q)}{(m g-Q \sin \theta)}\)
3 \(\frac{(\mathrm{P}+Q \cos \theta)}{(m g+Q \sin \theta)}\)
4 \(\frac{(\mathrm{P} \sin \theta-Q)}{(m g-Q \cos \theta)}\)
Laws of Motion

270381 A\(2 \mathbf{k g}\) block is placed over a \(4 \mathbf{k g}\) block and both are placed on a smooth horizontal surface. The coefficient of friction between the blocks is 0.20 . The acceleration of the two blocks if a horizontal force of \(12 \mathrm{~N}\) is applied to the lower block is \(\left(\mathrm{g}=10 \mathrm{~ms}^{-2}\right)\)

1 \(2 \mathrm{~ms}^{-2}, 2 \mathrm{~ms}^{-2}\)
2 \(2 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
3 \(3 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
4 \(4 \mathrm{~ms}^{-2}, 1 \mathrm{~ms}^{-2}\)
Laws of Motion

270382 Blocks\(A\) and \(B\) shown in the figure are connected with a bar of negligible weight. A and \(B\) each has mass \(170 \mathrm{Kg}\), the coefficient of friction between \(A\) and the plane is 0.2 and that between \(B\) and the plane is 0.4 . What is the total force of friction between the blocks and the plane \(\left(g=10 \mathrm{~ms}^{-2}\right)\)

1 900N
2 700N
3 600N
4 300N
Laws of Motion

270383 From the above problem what is the force acting on the connectingbar ?

1 \(150 \mathrm{~N}\)
2 \(100 \mathrm{~N}\)
3 \(75 \mathrm{~N}\)
4 \(125 \mathrm{~N}\)
Laws of Motion

270384 A block of mass \(m\), lying on a rough horizontal plane is acted upon by a horizontal force \(P\) and another force \(Q\), inclined at an angle \(\theta\) with vertical. The block will remain in equilibrium, if coefficient of friction between it and surface is

1 \(\frac{(\mathrm{P}+Q \sin \theta)}{(m g+Q \cos \theta)}\)
2 \(\cdot \frac{(\mathrm{P} \cos \theta+Q)}{(m g-Q \sin \theta)}\)
3 \(\frac{(\mathrm{P}+Q \cos \theta)}{(m g+Q \sin \theta)}\)
4 \(\frac{(\mathrm{P} \sin \theta-Q)}{(m g-Q \cos \theta)}\)