A model train, with a mass of #4 kg#, is moving on a circular track with a radius of #4 m#. If the train's rate of revolution changes from #1/9 Hz# to #1/3 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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The centripetal force acting on an object moving in a circular path is given by the formula:
[ F = m \times \omega^2 \times r ]
Where:
- ( F ) is the centripetal force
- ( m ) is the mass of the object
- ( \omega ) is the angular velocity of the object (in radians per second)
- ( r ) is the radius of the circular path
The angular velocity ( \omega ) is related to the frequency ( f ) by the formula ( \omega = 2\pi f ).
Given:
- ( m = 4 , \text{kg} )
- Initial frequency ( f_1 = \frac{1}{9} , \text{Hz} )
- Final frequency ( f_2 = \frac{1}{3} , \text{Hz} )
- ( r = 4 , \text{m} )
First, we need to find the initial and final angular velocities:
[ \omega_1 = 2\pi f_1 ] [ \omega_1 = 2\pi \times \frac{1}{9} ] [ \omega_1 = \frac{2\pi}{9} ]
[ \omega_2 = 2\pi f_2 ] [ \omega_2 = 2\pi \times \frac{1}{3} ] [ \omega_2 = \frac{2\pi}{3} ]
Now, we can calculate the initial and final centripetal forces:
[ F_1 = m \times \omega_1^2 \times r ] [ F_1 = 4 \times \left(\frac{2\pi}{9}\right)^2 \times 4 ]
[ F_2 = m \times \omega_2^2 \times r ] [ F_2 = 4 \times \left(\frac{2\pi}{3}\right)^2 \times 4 ]
Finally, we can find the change in centripetal force:
[ \Delta F = F_2 - F_1 ]
Substitute the calculated values and compute:
[ \Delta F = \left(4 \times \left(\frac{2\pi}{3}\right)^2 \times 4\right) - \left(4 \times \left(\frac{2\pi}{9}\right)^2 \times 4\right) ]
[ \Delta F ≈ 42.97 , \text{N} ]
Therefore, the centripetal force applied by the tracks changes by approximately ( 42.97 , \text{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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