(II) The two trees in Fig. 9–51 are 6.6 m apart. A backpacker is trying to lift his pack out of the reach of bears. Calculate the magnitude of the force\(\vec F\)that he must exert downward to hold a 19-kg backpack so that the rope sags at its midpoint by (a) 1.5 m, (b) 0.15 m.

Short Answer

Expert verified

The magnitudes of forces for parts (a) and (b) are:

(a) \({F_{\rm{T}}} = 225.3\;{\rm{N}}\)

(b) \({F_{\rm{T}}} = 2076.2\;{\rm{N}}\)

Step by step solution

01

Given data

The distance between the two trees is\(L = 6.6\,{\rm{m}}\).

The mass of the backpack is\(m = 19\;{\rm{kg}}\).

The magnitude of the force is\(F\).

02

Understanding the direction made by the force

In this question, the backpack is midway between the two trees, and the angles in the diagram will be equivalent.

To find the angle of the force, use the distance between the two trees and the quantity of sag at the midpoint.

03

Free body diagram and calculation of magnitude and direction of force

The following is the free body diagram.

When the sag in the rope at the midpoint is \(y = 1.5\;{\rm{m}}\), the relation to calculate the angle of force can be written as:

\(\begin{array}{c}\tan \theta = \frac{y}{{\left( {\frac{L}{2}} \right)}}\\\tan \theta = \left[ {\frac{{1.5\,{\rm{m}}}}{{\left( {\frac{{6.6\,{\rm{m}}}}{2}} \right)}}} \right]\\\theta = 24.4^\circ \end{array}\)

The relation of the forces in the y-direction can be written as:

\(\begin{array}{c}\sum {F_{\rm{y}}} = 0\\\left[ {2{F_{\rm{T}}}\sin \theta - mg} \right] = 0\\{F_{\rm{T}}} = \frac{{mg}}{{2\sin \theta }}\end{array}\)

Here, \(g\) is the gravitational acceleration.

On plugging the values in the above relation, you get:

\(\begin{array}{l}{F_{\rm{T}}} = \left( {\frac{{19\;{\rm{kg}} \times 9.8\;{\rm{m/}}{{\rm{s}}^2}}}{{2\left( {\sin 24.4^\circ } \right)}}} \right)\\{F_{\rm{T}}} = 225.3\;{\rm{N}}\end{array}\)

Thus, the magnitude of the force is \({F_{\rm{T}}} = 225.3\;{\rm{N}}\).

04

Calculation of magnitude and direction of force

When the sag in the rope at the midpoint is \(y = 0.15\;{\rm{m}}\), the relation to calculate the angle of force can be written as:

\(\begin{array}{c}\tan \theta ' = \frac{y}{{\left( {\frac{L}{2}} \right)}}\\\tan \theta ' = \left[ {\frac{{0.15\,{\rm{m}}}}{{\left( {\frac{{6.6\,{\rm{m}}}}{2}} \right)}}} \right]\\\theta ' = 2.57^\circ \end{array}\)

The relation of the forces in the y-direction can be written as:

\(\begin{array}{c}\sum {F_{\rm{y}}} = 0\\\left[ {2{F_{\rm{T}}}\sin \theta ' - mg} \right] = 0\\{F_{\rm{T}}} = \frac{{mg}}{{2\sin \theta '}}\end{array}\)

On plugging the values in the above relation, you get:

\(\begin{array}{l}{F_{\rm{T}}} = \left( {\frac{{19\;{\rm{kg}} \times 9.8\;{\rm{m/}}{{\rm{s}}^2}}}{{2\left( {\sin 2.57^\circ } \right)}}} \right)\\{F_{\rm{T}}} = 2076.2\;{\rm{N}}\end{array}\)

Thus, the magnitude of the force is \({F_{\rm{T}}} = 2076.2\;{\rm{N}}\).

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Most popular questions from this chapter

(I) A tower crane (Fig. 9–48a) must always be carefully balanced so that there is no net torque tending to tip it. A particular crane at a building site is about to lift a 2800-kg air-conditioning unit. The crane’s dimensions are shown in Fig. 9–48b. (a) Where must the crane’s 9500-kg counterweight be placed when the load is lifted from the ground? (The counterweight is usually moved automatically via sensors and motors to precisely compensate for the load.) (b) Determine the maximum load that can be lifted with this counterweight when it is placed at its full extent. Ignore the mass of the beam.

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