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?
The change in centripetal force is
Centripetal force is what
The frequencies that are
The centripetal force fluctuation is
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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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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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