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Figure (a) shows a horizontal uniform beam of massmband lengthLthat is supported on the left by a hinge attached to a wall and on theright by a cable at angle θ with the horizontal. A package of mass mp is positioned on the beam at a distance x from the left end. The total mass ismb+mp=61.22kg. Figure (b) gives the tension T in the cable as a function of the package’s position given as a fraction x/L of the beam length. The scale of the T axis is set by Ta=500N and Tb=700N.

(a) Evaluate angleθ ,

(b) Evaluate massmb , and

(c) Evaluate mass mp.

Short Answer

Expert verified
  1. Angle is30.020
  2. Mass of bar is 51kg
  3. Mass of package is 10.2kg

Step by step solution

01

Listing the given quantities       

Mb+Mp=61.22kg

02

Understanding the concept of force, tension and torque

By using the equilibrium condition along a vertical direction, we can write the equation in terms of tension T. Then compare that equation with the standard equation of line. From that, we can write the slope and y intercept. Once we know the slope and y intercept, then we can find the mass of rod, package and angle.

Equations:

Fx=0

Fy=0

τ=0

03

Free Body Diagram

04

(a) Calculation of Angle (b) Mass of bar (c) Mass of package

Using condition of equilibrium, we can write
Fy=0 (i)

Consider point A as pivot point. We have weight of the beam and weight of the package acting downwards at distanceL/2and x respective. The torque caused by these two forces would be balanced by the vertical component of the tension. Using equation for the torque, we have

TLsinθ=MbgL2+Mpgx (ii)

Now divide both sides of the equation (ii) by Lsinθ

T=MbgL2sinθL+MpgxLsinθ=MpgxLsinθ+Mbg2sinθ

We can write the slope as,

role="math" localid="1663335112681" Slope=Mpgsinθ (iii)

Therefore, the equation for T can be written as,

T=slopeXL+Mbg2sinθ

Now, the slope can be calculated from the graph as,

Slope=7005001=200

Substitute the value of slope in equation (iii), we get

200=Mpgsinθ

sinθ=Mpg200 (iv)

The y intercept on the graph is written as,

yintercept=(Mbg)2sinθ

(v)

But from the graph,yintercept=500 . Substitute the value in equation (v)

500=(Mbg)2sinθ

Simplifying this equation, we get

sinθ=(Mbg)2×500 (vi)

Equating equation (iv) and (vi), we get

Mpg200=(Mbg)2×500Mb=5Mp

But we know

Mb+Mp=61.22kg5Mp+Mp=61.22kgMp=10.2kg

Therefore, the mass of the package is 10.2kg.

We can calculate the mass of bar as,

Mb+Mp=61.22kgMb=61.22kgMp=61.22kg10.2kg=51kg

Therefore, the mass of bar is 51kg.

Now, use equation (vi) to calculate the angle.

inθ=Mpg200θ=sin1(Mpg200)=sin110.2kg×9.81m/s2200=30.02°

Therefore, the angle is 30.02°.

05

(b) Calculation of Mass of bar

Equating equation (iv) and (vi), we get

Mpg200=(Mbg)2×500Mb=5MpMp=Mb5

But we know

Mb+Mp=61.22kgMb+Mb5=61.22kgMb=51kg

Therefore, the mass of the bar is 51kg.

06

(c) Calculation of Mass of package

Equating equation (iv) and (vi), we get

Mpg200=(Mbg)2×500Mb=5Mp

But we know

Mb+Mp=61.22kg5Mp+Mp=61.22kgMp=10.2kg

Therefore, the mass of the package is 10.2kg.

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Most popular questions from this chapter

Question: Figure 12-29 shows a diver of weight 580 N standing at the end of a diving board with a length of L =4.5 mand negligible v mass. The board is fixed to two pedestals (supports) that are separated by distance d = 1 .5 m. Of the forces acting on the board, what are the (a) magnitude and (b) direction (up or down) of the force from the left pedestal and the (c) magnitude and (d) direction (up or down) of the force from the right pedestal? (e) Which pedestal (left or right) is being stretched, and (f) which pedestal is being compressed?

The rigid square frame in Fig. 12-79 consists of the four side bars AB ,BC , CD , and DA plus two diagonal bars ACand BD , which pass each other freely at E. By means of the turnbuckle G, bar ABis put under tension, as if its ends were subject to horizontal, outward forcesT of magnitude535 N .

(a) Which of the other bars are in tension? What are the magnitudes of (b) the forces causing the tension in those bars and (c) the forces causing compression in the other bars?

In Fig. 12-82, a uniform beam of length 12.0 m is supported by a horizontal cable and a hinge at angle θ=50.0°. The tension in the cable is 400 N .

In unit-vector notation, what are

(a) the gravitational force on the beam and

(b) the force on the beam from the hinge?

A uniform ladder is 10 m long and weighs 200 N . In Fig. 12-78, the ladder leans against a vertical, frictionless wall at heighth=8.0 m above the ground. A horizontal force is applied to the ladder at distance d=2.0 mfrom its base (measured along the ladder).

(a) If force magnitudeF=50 N , what is the force of the ground on the ladder, in unit-vector notation?

(b) IfF=150 N , what is the force of the ground on the ladder, also in unit-vector notation?

(c) Suppose the coefficient of static friction between the ladder and the ground is0.38 for what minimum value of the force magnitude Fwill the base of the ladder just barely start to move toward the wall?

In Fig. 12-20, a stationary 5 kg rod ACis held against a wall by a rope and friction between rod and wall. The uniform rod is 1 m long, and angle

(a) If you are to find the magnitude of the force T
on the rod from the rope with a single equation, at what labeled point should a rotation axis be placed? With that choice of axis and counter-clockwise torques positive,

what is the sign of

(b) the torqueτwdue to the rod’s weight and

(c) the torqueτrdue to the pull on the rod the rope?

(d) Is the magnitude of τrgreater than, less than, or equal to the magnitude of τw?

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