A model train with a mass of #5 kg# is moving along a track at #14 (cm)/s#. If the curvature of the track changes from a radius of #88 cm# to #28 cm#, by how much must the centripetal force applied by the tracks change?

Answer 1

The change in centripetal force is #=0.239N#

Centripetal force is what

#F=(mv^2)/r#
#m=mass=5kg#
#v=0.14ms^-1#

The centripetal force fluctuation is

#DeltaF=F_2-F_1#
#F_1=5*0.14^2/0.88=0.1114N#
#F_2=5*0.14^5/0.28=0.35N#
#DeltaF=0.35-0.1114=0.239N#
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Answer 2

To calculate the change in centripetal force, we first need to determine the initial and final centripetal forces acting on the train as it moves along the track. The centripetal force is given by the equation:

[ F_c = \frac{mv^2}{r} ]

where:

  • ( m ) = mass of the train (5 kg)
  • ( v ) = velocity of the train (14 cm/s)
  • ( r ) = radius of curvature of the track

Using the initial radius of curvature (( r = 88 ) cm), we can calculate the initial centripetal force (( F_{c1} )):

[ F_{c1} = \frac{(5 , \text{kg}) \times (14 , \text{cm/s})^2}{88 , \text{cm}} ]

Then, using the final radius of curvature (( r = 28 ) cm), we can calculate the final centripetal force (( F_{c2} )):

[ F_{c2} = \frac{(5 , \text{kg}) \times (14 , \text{cm/s})^2}{28 , \text{cm}} ]

Finally, we can find the change in centripetal force (( \Delta F_c )) by subtracting the initial force from the final force:

[ \Delta F_c = F_{c2} - F_{c1} ]

Plugging in the values and calculating:

[ F_{c1} = \frac{(5 , \text{kg}) \times (14 , \text{cm/s})^2}{88 , \text{cm}} = 10 , \text{N} ] [ F_{c2} = \frac{(5 , \text{kg}) \times (14 , \text{cm/s})^2}{28 , \text{cm}} = 50 , \text{N} ]

[ \Delta F_c = F_{c2} - F_{c1} = 50 , \text{N} - 10 , \text{N} = 40 , \text{N} ]

So, the centripetal force applied by the tracks must increase by 40 N when the curvature of the track changes from a radius of 88 cm to 28 cm.

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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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