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A uniform beam is hinged at one end and held in a horizontal position by a cable, as shown in Fig. 9–42. The tension in the cable

(a) must be at least half the weight of the beam, irrespective of the angle of the cable.

(b) could be less than half the beam’s weight for some angles.

(c) will be half the beam’s weight for all angles.

(d) will be equal to the beam’s weight for all angles.

Short Answer

Expert verified

The correct option is (a).

Step by step solution

01

Concepts

At equilibrium, the net torque is zero. For this problem, the clockwise torque due to the weight of the beam is equal to the torque due to the tension in the cable.

02

Explanation

Let m be the mass of the beam, T be the tension in the cable, and L be the length of the beam.

You can assume that the beam is uniform, and the weight of the beam is acting at the middle of the beam.

Also, assume that the cable makes \(\theta \) angle with the beam.

Now, at equilibrium, the net torque is zero. Then,

\(\begin{aligned}{c}T\sin \theta \times L = mg \times \frac{L}{2}\\\sin \theta = \frac{{\frac{{mg}}{2}}}{T}\end{aligned}\).

Now, you know that

\(\begin{aligned}{c}\sin \theta \le 1\\\frac{{\frac{{mg}}{2}}}{T} \le 1\\T \ge \frac{{mg}}{2}\end{aligned}\).

Hence, the tension in the cable must be at least half the weight of the beam.

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Most popular questions from this chapter

Two identical, uniform beams are symmetrically set up against each other (Fig. 9–87) on a floor with which they have a coefficient of friction\({\mu _{\rm{s}}} = 0.50\). What is the minimum angle the beams can make with the floor and still not fall?

(II) Calculate\({F_{\rm{A}}}\)and\({F_{\rm{B}}}\)for the uniform cantilever shown in Fig. 9–9 whose mass is 1200 kg.

A steel rod of radius\(R = 15\;{\rm{cm}}\)and length\({l_0}\)stands upright on a firm surface. A 65-kg man climbs atop the rod. (a) Determine the percent decrease in the rod’s length. (b) When a metal is compressed, each atom moves closer to its neighboring atom by exactly the same fractional amount. If iron atoms in steel are normally\(2.0 \times {10^{ - 10}}\;{\rm{m}}\)apart, by what distance did this interatomic spacing have to change in order to produce the normal force required to support the man? [Note: Neighboring atoms repel each other, and this repulsion accounts for the observed normal force.

(II) (a) Calculate the magnitude of the force, required of the “deltoid” muscle to hold up the outstretched arm shown in Fig. 9–72. The total mass of the arm is 3.3 kg. (b) Calculate the magnitude of the force exerted by the shoulder joint on the upper arm and the angle (to the horizontal) at which it acts.

(II) A 0.75-kg sheet is centered on a clothesline as shown in Fig. 9–63. The clothesline on either side of the hanging sheet makes an angle of 3.5° with the horizontal. Calculate the tension in the clothesline (ignore its mass) on either side of the sheet. Why is the tension so much greater than the weight of the sheet?

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