
A small block starts slipping down from a point B on an inclined plane AB, which is making an angle θ with the horizontal section BC is smooth and the remaining section CA is rough with a coefficient of friction. It is found that the block comes to rest as it reaches the bottom (point A) of the inclined plane. If\[BC = 2AC\], the coefficient of friction is given by \[\mu = k\tan \theta \]. Find the value of k.

Answer
161.4k+ views
Hint: In order to proceed into the problem, it is important to know about work energy theorem and the frictional force. Work-energy theorem states that the net work done by the forces on an object is equal to the change in kinetic energy of an object. Frictional force is the force acting in the opposite direction of the motion of an object.
Formula Used:
According to the work-energy theorem we have,
Work done =change in kinetic energy
At point B, \[u = 0\] i.e., the initial velocity is zero.
At point A, \[v = 0\] i.e., the final velocity is zero.
Hence change in kinetic energy is zero, then the work energy theorem can be written as,
\[{W_{mg}} + {W_{FF}} + {W_N} = 0\]……………… (1)
Where,
\[{W_{mg}}\] is the work done due to downward force mg.
\[{W_{FF}}\] is the frictional force acting on the block.
\[{W_N}\] is the normal force.
Complete step by step solution:
Now let us solve the problem step by step considering the definition.

Image: Small block slipping down from a point B to A on an inclined plane AB
By the definition of work done we know that,
\[W = \overrightarrow F \times \overrightarrow S \]
Here \[\overrightarrow F \] is the force and \[\overrightarrow S \] is the displacement.
Consider the equation (1)
\[{W_{mg}} + {W_{FF}} + {W_N} = 0\]
\[ \Rightarrow 3mgx\sin \theta + \mu mg\cos \theta \times x \times ( - 1) = 0\]
\[ \Rightarrow 3mgx\sin \theta = \mu mg\cos \theta \times x\]
\[ \Rightarrow \mu = 3\tan \theta \]……….. (2)
By data, \[ \Rightarrow \mu = K\tan \theta \]……… (3)
On comparing the equations (2) and (3) we obtain,
\[K = 3\]
Therefore, the value of K is 3.
Note: Suppose when an object is moving horizontally and then vertically upwards, the force which is required for this motion is more when compared to an object which is moving on an inclined plane upwards. This is the advantage of an inclined plane. When two bodies are in contact with each other the normal force is the force that acts between the objects individually between them. It is a surface force and is normal to the surface of contact of the bodies. If two surfaces are not in contact then, they can't exert a normal force.
Formula Used:
According to the work-energy theorem we have,
Work done =change in kinetic energy
At point B, \[u = 0\] i.e., the initial velocity is zero.
At point A, \[v = 0\] i.e., the final velocity is zero.
Hence change in kinetic energy is zero, then the work energy theorem can be written as,
\[{W_{mg}} + {W_{FF}} + {W_N} = 0\]……………… (1)
Where,
\[{W_{mg}}\] is the work done due to downward force mg.
\[{W_{FF}}\] is the frictional force acting on the block.
\[{W_N}\] is the normal force.
Complete step by step solution:
Now let us solve the problem step by step considering the definition.

Image: Small block slipping down from a point B to A on an inclined plane AB
By the definition of work done we know that,
\[W = \overrightarrow F \times \overrightarrow S \]
Here \[\overrightarrow F \] is the force and \[\overrightarrow S \] is the displacement.
Consider the equation (1)
\[{W_{mg}} + {W_{FF}} + {W_N} = 0\]
\[ \Rightarrow 3mgx\sin \theta + \mu mg\cos \theta \times x \times ( - 1) = 0\]
\[ \Rightarrow 3mgx\sin \theta = \mu mg\cos \theta \times x\]
\[ \Rightarrow \mu = 3\tan \theta \]……….. (2)
By data, \[ \Rightarrow \mu = K\tan \theta \]……… (3)
On comparing the equations (2) and (3) we obtain,
\[K = 3\]
Therefore, the value of K is 3.
Note: Suppose when an object is moving horizontally and then vertically upwards, the force which is required for this motion is more when compared to an object which is moving on an inclined plane upwards. This is the advantage of an inclined plane. When two bodies are in contact with each other the normal force is the force that acts between the objects individually between them. It is a surface force and is normal to the surface of contact of the bodies. If two surfaces are not in contact then, they can't exert a normal force.
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