A model train with a mass of #9 kg# is moving along a track at #15 (cm)/s#. If the curvature of the track changes from a radius of #46 cm# to #35 cm#, by how much must the centripetal force applied by the tracks change?
The variation 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, you can use the formula:
[ \Delta F = \frac{{mv^2}}{{r_1}} - \frac{{mv^2}}{{r_2}} ]
Where:
- ( \Delta F ) is the change in centripetal force,
- ( m ) is the mass of the train (9 kg),
- ( v ) is the velocity of the train (15 cm/s),
- ( r_1 ) is the initial radius (46 cm), and
- ( r_2 ) is the final radius (35 cm).
Plugging in the values:
[ \Delta F = \frac{{9 \times (15^2)}}{{46}} - \frac{{9 \times (15^2)}}{{35}} ]
[ \Delta F = \frac{{9 \times 225}}{{46}} - \frac{{9 \times 225}}{{35}} ]
[ \Delta F = \frac{{2025}}{{46}} - \frac{{2025}}{{35}} ]
[ \Delta F ≈ 390.67 - 579.64 ]
[ \Delta F ≈ -188.97 \text{ N} ]
The change in centripetal force is approximately -188.97 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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