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The floor of a railroad flatcar is loaded with loose crates having a coefficient of static friction 0.25 ofwith the floor. If the train is initially moving at a speed of 48 km/h, in how short a distance can the train be stopped at constant acceleration without causing the crates to slide over the floor?

Short Answer

Expert verified

The distance is 36.23 m

Step by step solution

01

Given

Coefficient of static friction,μs=0.25

Initial speed of the train,v0=48km/h=13.33m/s

Final speed of the train,vf=0m/s

02

Determining the concept

The problem is based on Newton’s second law of motion which states that the rate of change of momentum of a body is equal in both magnitude and direction of the force acting on it. Use the Newton's 2nd law of motion to find the acceleration of the train and then by using the Kinematic equations of motion, find the distance travelled by train.

Formula:

Fnet=ma

03

Determining the distance

The frictional force acting on the train is given by,

fs=μsN=μsmg

By using Newton's 2nd law along the horizontal direction,

F=ma-fs=ma-μsmg=maa=-μsg

This is the acceleration of the train.

Now, by using the Kinematic equation of motion,

v2=v02+2ass=v2-v022a=-13.3322-0.259.81=36.23m

Therefore, the distance is 36.23 m.

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Most popular questions from this chapter

The two blocks(m=16kgandM=88kg)in Fig. 6-38 are not attached to each other. The coefficient of static friction between the blocks is μs=0.38,but the surface beneath the larger block is frictionless. What is the minimum magnitude of the horizontal force Frequired to keep the smaller block from slipping down the larger block?

Repeat Question 1 for force F angled upward instead of downward as drawn.

In Fig. 6-58, force is applied to a crate of mass mon a floor where the coefficient of static friction between crate and floor is μs. Angle u is initially 0°but is gradually increased so that the force vector rotates clockwise in the figure. During the rotation, the magnitude Fof the force is continuously adjusted so that the crate is always on the verge of sliding. For μs=0.70, (a) plot the ratio F/mgversus θand (b) determine the angle θinfat which the ratio approaches an infinite value. (c) Does lubricating the floor increase or decrease θinf, or is the value unchanged? (d) What is θinffor μs=0.60?

In Fig. 6-61 a fastidious worker pushes directly along the handle of a mop with a force. The handle is at an angleθwith the vertical, andμsandμkare the coefficients of static and kinetic friction between the head of the mop and the floor. Ignore the mass of the handle and assume that all the mop’s mass mis in its head. (a) If the mop head moves along the floor with a constant velocity, then what is F? (b) Show that ifθ.is less than a certain valueθ0, thenf(still directed along the handle) is unable to move the mop head. Findθ0.

Suppose the coefficient of static friction between the road and the tires on a car is0.60and the car has no negative lift. What speed will put the car on the verge of sliding as it rounds a level curve of30.5mradius?

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