A model train, with a mass of #3 kg#, is moving on a circular track with a radius of #1 m#. If the train's kinetic energy changes from #21 j# to #36 j#, by how much will the centripetal force applied by the tracks change by?
To make it simple, lets find out the relation of kinetic energy and centripetal force with the things we know:
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The change in kinetic energy is equal to the work done by the centripetal force. Therefore, ( \Delta K = W = F \times d ), where ( \Delta K ) is the change in kinetic energy, ( W ) is the work done, ( F ) is the force, and ( d ) is the distance traveled.
The work done by the centripetal force is given by ( W = F \times d = F \times 2\pi r ), where ( r ) is the radius of the circular track.
So, we have ( \Delta K = F \times 2\pi r ).
We know that the change in kinetic energy ( \Delta K ) is ( 36 , \text{J} - 21 , \text{J} = 15 , \text{J} ).
Substituting the values, we get ( 15 = F \times 2\pi \times 1 ), which simplifies to ( F = \frac{15}{2\pi} ) N.
Therefore, the centripetal force applied by the tracks changes by ( \frac{15}{2\pi} ) N.
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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