A model train with a mass of #4 kg# is moving along a track at #21 (cm)/s#. If the curvature of the track changes from a radius of #84 cm# to #35 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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The centripetal force applied by the tracks can be calculated using the formula:
[ F_c = \frac{mv^2}{r} ]
Where:
- ( F_c ) is the centripetal force,
- ( m ) is the mass of the object (the model train),
- ( v ) is the velocity of the object, and
- ( r ) is the radius of the curvature of the track.
First, we calculate the initial centripetal force when the radius is 84 cm:
[ F_{c1} = \frac{(4 , \text{kg}) \times (0.21 , \text{m/s})^2}{0.84 , \text{m}} ]
[ F_{c1} = \frac{(4 , \text{kg}) \times (0.0441 , \text{m/s}^2)}{0.84 , \text{m}} ]
[ F_{c1} = \frac{0.1764 , \text{N}}{0.84 , \text{m}} ]
[ F_{c1} ≈ 0.21 , \text{N} ]
Next, we calculate the final centripetal force when the radius is 35 cm:
[ F_{c2} = \frac{(4 , \text{kg}) \times (0.21 , \text{m/s})^2}{0.35 , \text{m}} ]
[ F_{c2} = \frac{(4 , \text{kg}) \times (0.0441 , \text{m/s}^2)}{0.35 , \text{m}} ]
[ F_{c2} = \frac{0.1764 , \text{N}}{0.35 , \text{m}} ]
[ F_{c2} ≈ 0.504 , \text{N} ]
Finally, we find the change in centripetal force:
[ \Delta F_c = F_{c2} - F_{c1} ]
[ \Delta F_c = 0.504 , \text{N} - 0.21 , \text{N} ]
[ \Delta F_c ≈ 0.294 , \text{N} ]
So, the centripetal force applied by the tracks must increase by approximately ( 0.294 , \text{N} ) when the curvature of the track changes from a radius of 84 cm to 35 cm.
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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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