Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A factory worker accidentally releases a 180 kgcrate that was being held at rest at the top of a ramp that is 3.7 m long and inclined at 39ยฐto the horizontal. The coefficient of kinetic friction between the crate and the horizontal factory floor is 0.28. (a) How fast is the crate moving as it reaches the bottom of the ramp? (b) How far will it subsequently slide across the floor? (Assume that the crateโ€™s kinetic energy does not change as it moves from the ramp onto the floor.) (c) Do the answers to (a) and (b) increase, decrease, or remain the same if we halve the mass of the crate?

Short Answer

Expert verified

a) The velocity of the crate at the bottom of the ramp is 5.46m/s.

b) The distance through which it slides across the floor is 5.43m.

c) The answers for parts (a) and (b) remain the same when the mass of the crate is halved.

Step by step solution

01

The given data

The mass of the crate is,m=180 kg

The length of a ramp is, L=3.7 m

The angle of inclination is,ฮธ=39ยฐ

The coefficient of friction,ฮผ=0.28

The initial velocity is,vi=0m/s

02

Understanding the concept of the free body diagram of wedge

Using the formula for workdone on a system by external force when it is on the ramp, we can find the velocityof the crate at the bottom of the ramp. Then, using the formula for workdone on a system by external force when it is sliding along the floor and usingtheresult obtained from part a) we can findthe distance through which the crate slides across the floor.

Formulae:

The work done by the body,W=ฮ”Emech+ฮ”Eth (1)

The thermal energy due to friction,ฮ”Eth=ฮผkNL (2)

The potential energy at a height,PE=mgh (3)

The kinetic energy of the body,KE=12mv2 (4)

03

a) Calculation of the velocity of the crate at the bottom

In this case,W=0 Then, the thermal energy due to friction is given using equation (2):

ฮ”Eth=ฮผkmgcosฮธL...........(5)

(N=mgcosฮธ,fortheramp)

From trigonometry we can write for the given system that, the change in potential energy is given as:

ฮ”P.E.=-mgLsinฮธ...................(6)

Thus, using equations (5) and (6) in equation (1), the final velocity of the crate is given as:

0โ€„J=ฮ”K.E.+ฮ”P.E.+ฮ”Eth0โ€„J=K.E.f-K.E.i+-mgLsinฮธ+ฮผkmgcosฮธL0โ€„J=K.Ef-0+-mgLsinฮธ+ฮผkmgcosฮธLK.E.f=mgLsinฮธ-ฮผkmgcosฮธL12mvf2=mgLsinฮธ-ฮผkmgcosฮธL

Vf=2mmgLsinฮธ-ฮผkmgcosฮธL=2gLsinฮธ-ฮผkcosฮธ=29.8m/s23.7msin39ยฐ-0.28cos39ยฐ=5.46m/s

Therefore, the velocity of the crate at the bottom of the ramp is 5.46ms.

04

b) Calculation of the distance through which it slides across the floor

When the crate moves along the floor a distanceL'thework done on a system by the external force is zero. Thus, the distance traveled by the crate using equation (1) is given as:

0โ€„J=ฮ”Emech+ฮ”Eth0โ€„J=K.E.f-K.E.i+0โ€„J+ฮผkmgL'

The velocity obtained in part (a) is the initial velocity of the crate on the factory floor. Thus, substituting the value we get the distance as:

0โ€„J=0โ€„J-12mvf2+ฮผkmgL'L'=12vf2ฮผkgL'=125.46ms20.289.8m2sL'=5.43m

Therefore, the distance through which it slides across the floor is 5.43 m

05

c) Calculation of part (a) and part (d) when the mass of the crate is halved

From equations (1) and (2) obtained in parts (a) and (b) we can conclude that answers for parts (a) and (b) do not depend on the mass of the crate.

Therefore, the answers for parts (a) and (b) remain the same when the mass of the crate is halved.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A uniform cord of length25 cmand mass15 gis initially stuck to a ceiling. Later, it hangs vertically from the ceiling with only one end still stuck. What is the change in the gravitational potential energy of the cord with this change in orientation? (Hint:Consider a differential slice of the cord and then use integral calculus)

In Fig. 8-60, the pulley has negligible mass, and both it and the inclined plane are frictionless. Block A has a mass of 1.0 kg, block B has a mass of 2.0 kg, and angle ฮธis 30ยฐ. If the blocks are released from rest with the connecting cord taut, what is their total kinetic energy when block B has fallen 25 cm?

A1.50 kgsnowball is shot upward at an angle of34.0ยฐto the horizontal with an initial speed of20.0 m/s.

  1. What is its initial kinetic energy?
  2. By how much does the gravitational potential energy of the snowballโ€“Earth system change as the snowball moves from the launch point to the point of maximum height?
  3. What is that maximum height?

Approximately 5.5ร—106kgof water falls 50 mover Niagara Falls each second. (a) What is the decrease in the gravitational potential energy of the waterโ€“Earth system each second? (b) If all this energy could be converted to electrical energy (it cannot be), at what rate would electrical energy be supplied? (The mass of 1 m3of water is 1000 kg.) (c) If the electrical energy were sold at 1cent/KW.h, what would be the yearly income?

Resistance to the motion of an automobile consists of road friction, which is almost independent of speed, and air drag, which is proportional to speed-squared. For a certain car with a weight of 12,000 N, the total resistant force, Fis given by F=300+1.8v2, with Fin newton, and, v in meters per second. Calculate the power (in horsepower) required to accelerate the car at0.92m/s2when the speed is 80 km/h.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free