Conservtion laws- simple problems 4
Problem 9.
A cyclist intends to cycle up a 8 degrees hill whose vertical height is 150 m. If each complete revolution of the pedals moves the bike 6 m along its path, calculate the average force that must be exerted on the pedals tangent to their circular path. Neglect work done by friction and other losses. The pedals turn in a circle of diameter 30 cm. The total mass of the cyclist and his bike is 100 kg.
Solution:
In this problem we need to use generalized work-energy theorem: work done by an external force is equal to the change of the net mechanical energy of the system:
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We assume that the cyclist moves with constant speed. Then the initial and the final kinetic energies are the same. Therefore in the above expression we need to take into account only the gravitational potential energy:
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where
is the total mass of the cyclist and bike.
Then
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Now we need to define the initial and the final states of the system. We introduce the final state as the state after one complete revolution (relative to the initial state).

We know that after one complete revolution the cyclist moves 6 meters (as show in the figure). Then the change in the height of the cyclist is
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Therefore the change in the gravitation potential energy of the cyclist+bike is
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The work done by the force is
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During one revolution the pedal travels a distance of
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(circumference of a circle with diameter
). Where
is the diameter of the circle. Then the work done by the force is
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This work is equal to the change in gravitational potential energy:
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From this expression we can find the force:
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Problem 10. A body of mass 5 kg slides a distance of 6 m down a rough Inclined plane 30 degree.Then it moves on frictionless horizontal surface and compresses a spring. The coefficient of kinetic friction is 0.1 and the spring constant is 300 N/m. Find the maximum compression of the spring. Solution: In this problem we need to use the work-energy theorem, which determines the relation between the work done by the friction force and the change of the net mechanical energy. According the work-energy theorem the work done by the friction force (which is alwaysnegative) is equal to the difference between the final mechanical energy and the initial mechanical energy. The mechanical energy is the sum of kinetic energy, gravitational potential energy, and elastic energy of the spring. The initial velocity of the body is zero, the initial compression of the spring is zero, the initial height of the body is In the final state we have a maximum compression of the spring. It means that in the final state the velocity of the body is zero. The final height of the body is 0 (ground level). Then the final mechanical energy of the body is Then equation (1) takes the form Now we need to find the work done by the friction force. The work done by the friction force (see figure) is where To find the normal force we need to write down the second Newton's law for the motion along the incline. There are three forces acting on the body: gravitational force, normal force, and the friction force. Then the second Newton's law takes the form: The direction of the acceleration is along the incline. It means that the acceleration has only x component (see figure). The y-component of acceleration is zero. Then to find the normal force we need to write down only the y-component of equation (2): From this equation we can find the normal force: Now we can find the friction force and the work done by the friction force Then we can find the maximum (final) compression of the spring:
................................................. (1)
. Then the initial mechanical energy of the body is![]()

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is the displacement of the body over incline plane. The friction force is determined by the normal force and the coefficient of kinetic friction:![]()
...........................................................(2)
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