A model train with a mass of #8 kg# is moving along a track at #15 (cm)/s#. If the curvature of the track changes from a radius of #45 cm# to #225 cm#, by how much must the centripetal force applied by the tracks change?

Answer 1

The centripetal force is #0.1N#

The centripetal force is

#F=(mv^2)/r#

The variation in centripetal force is

#DeltaF=(mv^2)/(Delta r)#
#=(8*(0.15)^2)/(2.25-0.45)#
#=(8*0.0225)/1.8#
#=0.1N#
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Answer 2

The centripetal force must increase by 40 N.

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Answer 3

The centripetal force required to keep an object moving in a curved path is given by the formula:

[ F_{\text{centripetal}} = \frac{mv^2}{r} ]

Where:

  • ( F_{\text{centripetal}} ) is the centripetal force,
  • ( m ) is the mass of the object,
  • ( v ) is the velocity of the object, and
  • ( r ) is the radius of curvature of the path.

Given:

  • Mass ( m = 8 ) kg,
  • Initial radius ( r_1 = 45 ) cm,
  • Final radius ( r_2 = 225 ) cm, and
  • Initial velocity ( v = 15 ) cm/s.

First, we need to convert all measurements to SI units (kilograms, meters, seconds) for consistency in calculations.

[ r_1 = 45 , \text{cm} = 0.45 , \text{m} ] [ r_2 = 225 , \text{cm} = 2.25 , \text{m} ] [ v = 15 , \text{cm/s} = 0.15 , \text{m/s} ]

Now we can calculate the initial and final centripetal forces:

[ F_{\text{initial}} = \frac{m \cdot v^2}{r_1} ] [ F_{\text{final}} = \frac{m \cdot v^2}{r_2} ]

Substitute the given values:

[ F_{\text{initial}} = \frac{8 \times (0.15)^2}{0.45} \approx 0.8 , \text{N} ] [ F_{\text{final}} = \frac{8 \times (0.15)^2}{2.25} \approx 0.0533 , \text{N} ]

The change in centripetal force is the difference between the final and initial forces:

[ \Delta F_{\text{centripetal}} = F_{\text{final}} - F_{\text{initial}} ] [ \Delta F_{\text{centripetal}} = 0.0533 , \text{N} - 0.8 , \text{N} \approx -0.7467 , \text{N} ]

Therefore, the centripetal force applied by the tracks must decrease by approximately ( 0.7467 , \text{N} ) to accommodate the change in curvature from a radius of 45 cm to 225 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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