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A block of mass 10 kg slides down on an ...

A block of mass 10 kg slides down on an incline 5 m long and 3 m high. A man pushes up on the ice block parallel to the incline so that it slides down at constant speed. The coefficient of friction between the ice and the incline is 0.1. Find :
(a) the work done by the man on the block.
(b) the work done by gravity on the block.
(c) the work done by the surface on the block.
(d) the work done by the resultant forces on the block.
(e) the change in K.E. of the block.

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To solve the problem step by step, we will analyze the forces acting on the block and calculate the required work done by different forces. ### Given Data: - Mass of the block, \( m = 10 \, \text{kg} \) - Length of incline, \( L = 5 \, \text{m} \) - Height of incline, \( h = 3 \, \text{m} \) - Coefficient of friction, \( \mu = 0.1 \) - Gravitational acceleration, \( g = 10 \, \text{m/s}^2 \) ### Step 1: Calculate the angle of the incline Using the right triangle formed by the height and length of the incline: \[ \sin \theta = \frac{h}{L} = \frac{3}{5} \quad \text{and} \quad \cos \theta = \frac{4}{5} \] ### Step 2: Calculate the gravitational force components The gravitational force acting on the block is: \[ F_g = mg = 10 \times 10 = 100 \, \text{N} \] The components of the gravitational force along the incline: \[ F_{g \parallel} = mg \sin \theta = 100 \times \frac{3}{5} = 60 \, \text{N} \] \[ F_{g \perpendicular} = mg \cos \theta = 100 \times \frac{4}{5} = 80 \, \text{N} \] ### Step 3: Calculate the normal force The normal force \( N \) is equal to the perpendicular component of the gravitational force: \[ N = F_{g \perpendicular} = 80 \, \text{N} \] ### Step 4: Calculate the frictional force The frictional force \( F_f \) opposing the motion is given by: \[ F_f = \mu N = 0.1 \times 80 = 8 \, \text{N} \] ### Step 5: Calculate the force exerted by the man Since the block is sliding down at constant speed, the net force along the incline must be zero: \[ P + F_f = F_{g \parallel} \] Thus, the force exerted by the man \( P \) is: \[ P = F_{g \parallel} - F_f = 60 - 8 = 52 \, \text{N} \] ### Step 6: Calculate the work done by the man The work done by the man \( W_m \) is: \[ W_m = P \cdot d \cdot \cos(180^\circ) = 52 \cdot 5 \cdot (-1) = -260 \, \text{J} \] ### Step 7: Calculate the work done by gravity The work done by gravity \( W_g \) is: \[ W_g = F_{g \parallel} \cdot d = 60 \cdot 5 = 300 \, \text{J} \] ### Step 8: Calculate the work done by the surface (friction) The work done by friction \( W_f \) is: \[ W_f = F_f \cdot d \cdot \cos(180^\circ) = 8 \cdot 5 \cdot (-1) = -40 \, \text{J} \] ### Step 9: Calculate the work done by the resultant forces Since the block moves with constant velocity, the net work done by the resultant forces \( W_r \) is: \[ W_r = 0 \, \text{J} \] ### Step 10: Calculate the change in kinetic energy Since the velocity is constant, the change in kinetic energy \( \Delta KE \) is: \[ \Delta KE = 0 \, \text{J} \] ### Summary of Results: (a) Work done by the man on the block: \( -260 \, \text{J} \) (b) Work done by gravity on the block: \( 300 \, \text{J} \) (c) Work done by the surface on the block: \( -40 \, \text{J} \) (d) Work done by the resultant forces on the block: \( 0 \, \text{J} \) (e) Change in K.E. of the block: \( 0 \, \text{J} \)
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