A model train, with a mass of #32 kg#, is moving on a circular track with a radius of #9 m#. If the train's kinetic energy changes from #18 j# to #21 j#, by how much will the centripetal force applied by the tracks change by?

Answer 1

The change in centripetal force is #=2/3N#

The centripetal force is

#F=(mv^2)/r#

The kinetic energy is

#KE=1/2mv^2#

The variation of kinetic energy is

#Delta KE=1/2mv^2-1/2m u^2#
#=1/2m(v^2-u^2)#
The mass is #m=32kg#
The radius of the track is #r=9m#

The variation of centripetal force is

#DeltaF=m/r(v^2-u^2)#
#DeltaF=2m/r1/2(v^2-u^2)#
#=(2)/r*1/2m(v^2-u^2)#
#=(2)/r*Delta KE#
#=2/9*(21-18)N#
#=2/3N#
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Answer 2

The centripetal force applied by the tracks can be calculated using the formula:

[ F = \frac{mv^2}{r} ]

where ( m ) is the mass of the train, ( v ) is the velocity of the train, and ( r ) is the radius of the circular track.

Given that the mass of the train is ( 32 , \text{kg} ) and the radius of the track is ( 9 , \text{m} ), we can calculate the initial centripetal force (( F_1 )) when the kinetic energy is ( 18 , \text{J} ):

[ F_1 = \frac{m \cdot (v_1)^2}{r} ]

where ( v_1 ) is the initial velocity of the train.

Given that the initial kinetic energy (( E_1 )) is ( 18 , \text{J} ), we can use the formula for kinetic energy to find ( v_1 ):

[ E_1 = \frac{1}{2} m \cdot (v_1)^2 ]

Solving for ( v_1 ):

[ v_1 = \sqrt{\frac{2 \cdot E_1}{m}} ]

Given that the final kinetic energy (( E_2 )) is ( 21 , \text{J} ), we can find the final velocity (( v_2 )) using the formula for kinetic energy:

[ E_2 = \frac{1}{2} m \cdot (v_2)^2 ]

Solving for ( v_2 ):

[ v_2 = \sqrt{\frac{2 \cdot E_2}{m}} ]

Once we have ( v_1 ) and ( v_2 ), we can calculate the initial and final centripetal forces (( F_1 ) and ( F_2 )) using the formula:

[ F = \frac{m \cdot v^2}{r} ]

Then, the change in centripetal force is given by:

[ \Delta F = F_2 - F_1 ]

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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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