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?

Answer 1

To make it simple, lets find out the relation of kinetic energy and centripetal force with the things we know:

We know: #"K.E." = 1/2momega^2r^2#
and #"centripetal force"=momega^2r#
Hence, #"K.E" = 1/2xx"centripetal force"xxr#
Note, #r# remain constant in the course of the process.
Hence, #Delta"centripetal force" = (2Delta"K.E.")/r = (2(36-21)J)/(1m)=30N#
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Answer 2

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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Answer from HIX Tutor

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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