A model train, with a mass of #3 kg#, is moving on a circular track with a radius of #8 m#. If the train's rate of revolution changes from #1/4 Hz# to #1/7 Hz#, by how much will the centripetal force applied by the tracks change by?

Answer 1

The change in centripetal force is #=39.88N#

Centripetal force is what

#F=(mv^2)/r=mromega^2N#
The mass of the train, #m=(3)kg#
The radius of the track, #r=(8)m#

The frequencies that are

#f_1=(1/4)Hz#
#f_2=(1/7)Hz#
The angular velocity is #omega=2pif#

The centripetal force fluctuation is

#DeltaF=F_2-F_1#
#F_1=mromega_1^2=mr*(2pif_1)^2=3*8*(2pi*1/4)^2=59.22N#
#F_2=mromega_2^2=mr*(2pif_2)^2=3*8*(2pi*1/7)^2=19.34N#
#DeltaF=|F_2-F_1|=59.22-19.34=39.88N#
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Answer 2

To find the change in centripetal force, we first calculate the initial and final centripetal forces using the formulas:

Initial frequency: ( f_1 = \frac{1}{4} ) Hz Initial angular velocity: ( \omega_1 = 2\pi f_1 ) Initial centripetal force: ( F_1 = m \cdot r \cdot \omega_1^2 )

Final frequency: ( f_2 = \frac{1}{7} ) Hz Final angular velocity: ( \omega_2 = 2\pi f_2 ) Final centripetal force: ( F_2 = m \cdot r \cdot \omega_2^2 )

Substitute the values and find the change in centripetal force:

[ \Delta F = F_2 - F_1 ]

[ \Delta F = m \cdot r \cdot \omega_2^2 - m \cdot r \cdot \omega_1^2 ]

[ \Delta F = m \cdot r \cdot ( \omega_2^2 - \omega_1^2 ) ]

[ \Delta F = m \cdot r \cdot ( (2\pi f_2)^2 - (2\pi f_1)^2 ) ]

[ \Delta F = m \cdot r \cdot ( (2\pi \cdot \frac{1}{7})^2 - (2\pi \cdot \frac{1}{4})^2 ) ]

Calculate the values and subtract to find the change in centripetal force.

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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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