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?

Answer 1

The change in centripetal force is #=0.177N#

The centripetal force is

#F=(mv^2)/r#
mass, #m=(4)kg#
speed, #v=(0.09)ms^-1#
radius, #=(r) m#

The variation in centripetal force is

#DeltaF=F_2-F_1#
#F_1=mv^2/r_1=4*0.09^2/1.8=0.018N#
#F_2=mv^2/r_2=4*0.09^2/0.24=0.135N#
#DeltaF=0.135-0.018=0.177N#
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Answer 2

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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Answer from HIX Tutor

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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