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In Fig. 12-67a, a uniform40.0kgbeam is centered over two rollers. Vertical lines across the beam mark off equal lengths. Two of the lines are centered over the rollers; a 10.0kgpackage of tamales is centered over roller B.What are the magnitudes of the forces on the beam from (a) roller Aand (b) roller B? The beamis then rolled to the left until the right-hand end is centered over roller B(Fig. 12-67b).What now are the magnitudes of the forces on the beam from (c) roller Aand (d) roller B? Next, the beam is rolled to the right. Assume that it has a length of 0.800 m. (e) what horizontal distance between the package and roller Bputs the beam on the verge of losing contact with rollerA?

Short Answer

Expert verified

a) The magnitude of the force on roller A in diagram (a)=196 N .

b) The magnitude of the force on roller B in diagram (a)=294 N .

c) The magnitude of the force on roller A in diagram (b) =441 N.

d) The magnitude of the force on roller B in diagram (b) =49 N.

e)0.16m is the horizontal distance between the package and roller B that puts the beam on the verge of losing contact with roller A

Step by step solution

01

Listing the given quantities

Massofthebeam=40kg

Massofpackage=10kg

Lengthofbeam=0.8m

02

Understanding the concept of force and torque

From the Free Body Diagrams for the beam and using equilibrium conditions, we can find the reactions on rollers A and B.

Using the equilibrium conditions for net torque, we can find the horizontal distance between the package and roller B.

Equations:

∑Fy=0

∑Momentatanypointonthebeam=0

Weight=mass×gravitationalacceleration

Weightofbeam(WB)=mbeam×gravitationalacceleration=40 kg×9.8 m/s2=392 N

Weightofpackage(WP)=mpackage×gravitationalacceleration=10 kg×9.8 m/s2=98 N

03

Free body diagram

04

(a) Calculations of the magnitude of the force on roller A in diagram (a)

From the equilibrium conditions,

∑Fy=0

RA+RB−392 N−98 N=0RA+RB=490 N

∑MomentB=0(0.4 m×RA)−(392 N×0.2 m)=0RA=78.4 N⋅m0.4 mRA=196 N

05

(b)Calculations of the magnitude of the force on roller B in diagram (a) 

RA+RB=490 N196 N+RB=490 NRB=294 N

06

(c)Calculations of the magnitude of the force on roller A in diagram (b)

Assuming that axis of rotation passes through point B, we can write the equations as

L4WP+L2WB−L2RA=0

Simplifying this we get,

RA=WB+WP2=392 N+98 N2=441 â¶Ä‰N

07

(d)Calculations of the magnitude of the force on roller B in diagram (b) 

Free body diagram for (a),

∑Fy=0RA+RB−392 N−98 N=0RA+RB=490 N

Putting the value ofRAwe get,

RB=49 N

08

(e)Calculations of the horizontal distance between the package and roller B that puts the beam on the verge of losing contact with roller A. 

Free body diagram:

Assuming the axis of rotation passes through point B, we can write

∑MomentB=0

When the beam is about to lose contact with point A,RA=0,

So we can write,

weightofpackage×x-(weightofbeam×(L4-x))=098 N×x=392 N×(L4−x)98 N×x=(98 N) L−(392 N)x(98 N)x+(392 N)x=98 N×0.8 m(490 N)x=78.4 N⋅mx=78.4 N⋅m490 Nx =0.16 m

0.16 m Is the horizontal distance between the package and roller B that puts the beam on the verge of losing contact with roller A

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