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A runner whose mass is 50kg accelerates from a stop to a speed of 10m/s in 3s. (A good sprinter can run 100m in about 10s, with an average speed of 10m/s.) (a) What is the average horizontal component of the force that the ground exerts on the runner’s shoes? (b) How much displacement is there of the force that acts on the sole of the runner’s shoes, assuming that there is no slipping? Therefore, how much work is done on the extended system (the runner) by the force you calculated in the previous exercise? How much work is done on the point particle system by this force? (c) The kinetic energy of the runner increases—what kind of energy decreases? By how much?

Short Answer

Expert verified

a) 167N

b) There is no work done on the extended system due to zero displacement and , the work done on the particle system is 2500J.

c) Decrease in the internal energy by 2500J.

Step by step solution

01

Identification of the given data

The given data can be listed below as,

  • The mass of the runner is, 50kg.
  • The velocity of the runner is, 10m/s.
  • The time taken by the runner is, 3s.
02

Significance of the law of conservation of work done and Newton’s second law for the runner

The law of conservation of work done states that energy cannot be destroyed or created, it can only be converted into different forms.

The second law of Newton states that the force exerted is directly proportional to the product of the mass and the acceleration of a body.

According to the work-energy theorem, the work done is the same as that of the change in the kinetic energy.

03

Determination of force’s horizontal component exerted by the ground on the shoes of the runner

(a)

The expression for the horizontal component of the force can be expressed as,

F=ma=mv/t

Here, mis the mass of the runner, ais the acceleration of the runner that is a=vt(here, vis the velocity of the runner and tis the time taken by the runner).

For m=50kg, v=10m/sand t=3s.

F=50kg×10m/s3s=166.66kg.m/s2=166.66kg.m/s2×1N1kg.ms2≈167N

Thus, the average horizontal component of the force is 167N.

04

Determination of the displacement and the work done

(b)

The expression for the displacement of the runner is expressed as,

s=ut

Here, uis the initial velocity of the runner’s shoes that is 0 and tis the time taken.

Substitute all the values in the above equation.

role="math" localid="1653903841151" s=0m/s×3s=0m

Thus, the displacement of the runner’s shoes is 0.

The expression for work done on the extended system can be expressed as,

W=F·d

Here, Fis the force and dis the displacement of the runner.

For F=167Nand d=0.

W=167N×0=0

Thus, the work done on the extended system is 0.

From the law of conservation of work done, the equation of the work done on the point particle system can be expressed as,

W1=12mv2

Here, W1is the work done on the point particle system.

Form=50kgand v=10m/s.

W=12×50kg×10m/s2=2500kg.m2/s2=2500kg.m/s2×1J1kg.m/s2=2500J

Thus, the work done on the point particle system by this force is 2500J.

05

Determination of the energy that decreases

(c)

By the work energy theorem, the work done is same as that of the change in the kinetic energy.

As the Kinetic energy of the runner increases, the internal or the chemical energy of the runner decreases.

As the work done on the point particle system is 2500J so the internal energy also decreased by 2500J.

Thus, the internal energy decreases and it reduces to 2500J.

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