A model train with a mass of #4 kg# is moving along a track at #9 (cm)/s#. If the curvature of the track changes from a radius of #180 cm# to #24 cm#, by how much must the centripetal force applied by the tracks change?
The change in centripetal force is
The centripetal force is
The variation in centripetal force is
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To find the change in centripetal force, we first need to calculate the initial and final centripetal forces using the formula:
[ F_c = \dfrac{mv^2}{r} ]
where: ( m = 4 , \text{kg} ) (mass of the train), ( v = 9 , \text{cm/s} ) (velocity of the train), ( r_{initial} = 180 , \text{cm} ) (initial radius of curvature), ( r_{final} = 24 , \text{cm} ) (final radius of curvature).
Initial centripetal force: [ F_{c_initial} = \dfrac{4 , \text{kg} \times (9 , \text{cm/s})^2}{180 , \text{cm}} ]
Final centripetal force: [ F_{c_final} = \dfrac{4 , \text{kg} \times (9 , \text{cm/s})^2}{24 , \text{cm}} ]
Change in centripetal force: [ \Delta F_c = F_{c_final} - F_{c_initial} ]
[ \Delta F_c = \dfrac{4 , \text{kg} \times (9 , \text{cm/s})^2}{24 , \text{cm}} - \dfrac{4 , \text{kg} \times (9 , \text{cm/s})^2}{180 , \text{cm}} ]
[ \Delta F_c = \dfrac{4 \times 81}{24} - \dfrac{4 \times 81}{180} ]
[ \Delta F_c = 13.5 , \text{N} - 1.8 , \text{N} ]
[ \Delta F_c = 11.7 , \text{N} ]
So, the centripetal force applied by the tracks must change by ( 11.7 , \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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