/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q26P In Figure 12-43, a climber leans... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

In Figure 12-43, a climber leans out against a vertical ice wall that has negligible friction. Distance ais 0.914″¾ and distance Lis2.10″¾. His center of mass is distance d=0.940″¾from the feet–ground contact point. If he is on the verge of sliding, what is the coefficient of static friction between feet and ground?

Short Answer

Expert verified

The coefficient of static friction between the feet and the groundis0.216 .

Step by step solution

01

Understanding the given information 

i) Distance from the ice wall to the feet, a=0.914″¾.

ii) Length of the climber, L=2.10″¾.

iii) Distance of center of mass from the bottom, d=0.940″¾.

02

Concept and formula used in the given question

Using the concept of static equilibrium, you can write the equation for torque in terms of force and distances. Using these equations, you can find the frictional force. From the frictional force value, it is possible to find the value of the coefficient of friction.

03

Calculation for thecoefficient of static friction between feet and ground 

A free body diagram can be drawn as;

From the diagram, we can conclude that:

Forces acting in the x direction can be written as,

FN2−Fs=0 (1)

Forces acting in the y direction can be written as,

FN1−mg=0FN1=mg (2)

Torque can be calculated as,

mgdcosθ−FN2Lsinθ=0FN2=mgdcotθL

Substituting values from equation 2 in the above equation and we get,

FN2=FN1dcotθL

Substituting values from equation 1 in the above equation and we get,

Fs=FN1cotθdL (3)

We know that,

Fs=μFN1 (4)

And

cotθ=aL2−a2 (5)

Comparing equations 3 and 4, we get,

μ=dcotθL

Substitute values from equation 5 in the above expression, and we get,

μ=dLaL2−a2

Substitute values in the above expression, and we get,

μ=0.9402.100.9142.102−0.9142=0.4476×0.4834=0.2163

Thus, the coefficient of static friction between the feet and the ground is 0.216.

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 91Ó°ÊÓ!

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

Figure 12-85ashows details of a finger in the crimp holdof the climber in Fig. 12-50. A tendon that runs from muscles inthe forearm is attached to the far bone in the finger. Along the way, the tendon runs through several guiding sheaths called pulleys. The A2 pulley is attached to the first finger bone; the A4 pulley is attached to the second finger bone. To pull the finger toward the palm, the forearm muscles pull the tendon through the pulleys, much like strings on a marionette can be pulled to move parts of the marionette. Figure 12-85bis a simplified diagram of the second finger bone, which has length d. The tendon’s pull F→ton the bone acts at the point where the tendon enters the A4 pulley, at distance d/3 along the bone. If the force components on each of the four crimped fingers in Fig. 12-50 are Fh=13.4 Nand Fv=162.4 N, what is the magnitude ofF→t ? The result is probably tolerable, but if the climber hangs by only one or two fingers, the A2 and A4 pulleys can be ruptured, a common ailment among rock climbers.

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.

In Fig12-46, a 50.0 k²µ uniform square sign, of edge lengthL=2.00″¾, is hung from a horizontal rod of length dh=3.00″¾and negligible mass. A cable is attached to the end of the rod and to a point on the wall at distance dv=4.00″¾above the point where the rod is hinged to the wall.(a) What is the tension in the cable? What are the (b) magnitude and) of the horizontal component of the force on the rod from the wall, and the (c) direction (left or right) of the horizontal component of the force on the rod from the wall, and the (d) magnitude of the vertical component of this force? And (e) direction (up or down) of the vertical component of this force?

Question: In Fig 12-30, trying to get his car out of mud, a man ties one end of a rope around the front bumper and the other end tightly around a utility pole 18 maway. He then pushes sideways on the rope at its midpoint with a force of 550 N , displacing the center of the rope 0.30 m, but the car barely moves. What is the magnitude of the force on the car from the rope? (The rope stretches somewhat.)

A construction worker attempts to lift a uniform beam off the floor and raise it to a vertical position. The beam is 2.50″¾long and weighs500 N . At a certain instant the worker holds the beam momentarily at rest with one end at distanced=1.50″¾ above the floor, as shown in Fig. 12-75, by exerting a force on the beam, perpendicular to the beam. (a) What is the magnitude P? (b) What is the magnitude of the (net) force of the floor on the beam? (c) What is the minimum value the coefficient of static friction between beam and floor can have in order for the beam not to slip at this instant?

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.