/*! 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} Problem 66 \(\mathrm{A}\) square plate is \... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

\(\mathrm{A}\) square plate is \(1.0 \times 10^{-2} \mathrm{m}\) thick, measures \(3.0 \times 10^{-2} \mathrm{m}\) on a side, and has a mass of \(7.2 \times 10^{-2} \mathrm{kg} .\) The shear modulus of the material is \(2.0 \times 10^{10} \mathrm{N} / \mathrm{m}^{2} .\) One of the square faces rests on a flat horizontal surface, and the coefficient of static friction between the plate and the surface is 0.91. A force is applied to the top of the plate, as in Figure 10.29 a. Determine (a) the maximum possible amount of shear stress, (b) the maximum possible amount of shear strain, and (c) the maximum possible amount of shear deformation \(\Delta X\) (see Figure \(10.29 b\) ) that can be created by the applied force just before the plate begins to move.

Short Answer

Expert verified
(a) 713.44 Pa, (b) \(3.5672 \times 10^{-8}\), (c) \(3.5672 \times 10^{-10}\) m.

Step by step solution

01

Calculate Maximum Static Friction Force

The maximum force before the plate slips is determined by static friction. This force is given by \( F_{ ext{max}} = \mu_s \times F_n \), where \( \mu_s = 0.91 \) (coefficient of static friction) and \( F_n = mg \) (normal force, equal to weight). The weight \( mg = 7.2 \times 10^{-2} \times 9.8 = 0.7056 \) N. Therefore, \( F_{\text{max}} = 0.91 \times 0.7056 = 0.642096 \) N.
02

Calculate Maximum Shear Stress

Shear stress \( \tau \) is defined as the force per unit area. The area \( A \) of the square face is \((3.0 \times 10^{-2})^2 = 9.0 \times 10^{-4} \) m². Therefore, the maximum shear stress is \( \tau = \frac{F_{\text{max}}}{A} = \frac{0.642096}{9.0 \times 10^{-4}} = 713.44 \) Pa.
03

Calculate Maximum Shear Strain

Shear strain \( \gamma \) is related to shear stress \( \tau \) and shear modulus \( G \) by the formula \( \gamma = \frac{\tau}{G} \). Given \( G = 2.0 \times 10^{10} \) N/m², the shear strain is \( \gamma = \frac{713.44}{2.0 \times 10^{10}} = 3.5672 \times 10^{-8} \).
04

Calculate Maximum Shear Deformation

Shear deformation \( \Delta X \) is related to shear strain by the formula \( \gamma = \frac{\Delta X}{t} \), where \( t = 1.0 \times 10^{-2} \) m is the thickness. So, \( \Delta X = \gamma \times t = 3.5672 \times 10^{-8} \times 1.0 \times 10^{-2} = 3.5672 \times 10^{-10} \) m.

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!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Shear Strain
When a force is applied parallel to the surface of an object, the material experiences shear strain. Imagine it as a shift between layers in the material without any change in its volume. It's like sliding a deck of cards sideways - the top card shifts relative to the bottom one. In mathematical terms, shear strain \( \gamma \) is defined as the displacement (deformation) across the thickness of a material divided by its thickness.

It's calculated using the formula:
  • \[ \gamma = \frac{\tau}{G} \]
where \( \tau \) is the shear stress and \( G \) is the shear modulus. This relationship helps illustrate how the material's response (strain) to an applied force (stress) depends on its properties (shear modulus).
Shear Deformation
Shear deformation in a material is the actual change or distortion that occurs when a force is applied. It reflects the physical shift of particles from their initial alignment. Consider a block of gelatin - when you push the top surface slightly, it causes the block to tilt and deform, akin to the shear deformation concept.
  • The extent of this deformation can be quantified by the formula:
  • \[ \Delta X = \gamma \cdot t \]
Here, \( \Delta X \) is the deformation, \( \gamma \) is the shear strain, and \( t \) is the thickness of the material. This formula highlights that the amount of deformation depends on both the strain and the thickness.
Static Friction
Static friction is the force that keeps an object at rest when a force is applied, preventing it from sliding. Think of trying to push a heavy box on the floor; the resistance you feel before it starts moving is static friction. This frictional force must be overcome to initiate motion. It is dependent on two factors: the coefficient of static friction and the normal force.
  • Mathematically, it's expressed as:
  • \[ F_{\text{max}} = \mu_s \times F_n \]
where \( \mu_s \) is the coefficient of static friction and \( F_n \) is the normal force (often the weight of the object if on a horizontal surface). This formula helps calculate the maximum force needed to move an object before it starts to slide.
Shear Modulus
The shear modulus, also known as the modulus of rigidity, describes how a material reacts to shear stress. It measures the material's stiffness when subject to shear forces, and it is an intrinsic property of materials. Think of it as how difficult it is to twist or shift the material. The higher the shear modulus, the stiffer the material, meaning it will deform less under the same applied shear stress.
  • It's calculated through the relationship:
  • \[ G = \frac{\tau}{\gamma} \]
Here, \( G \) is the shear modulus, \( \tau \) is the shear stress, and \( \gamma \) is the shear strain. This formula showcases a direct link between stress and strain controlled by the material's stiffness.

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

When an object of mass \(m_{1}\) is hung on a vertical spring and set into vertical simple harmonic motion, it oscillates at a frequency of \(12.0 \mathrm{Hz} .\) When another object of mass \(m_{2}\) is hung on the spring along with the first object, the frequency of the motion is \(4.00 \mathrm{Hz}\). Find the ratio \(m_{2} / m_{1}\) of the masses.

A uniform 1.4-kg rod that is 0.75 m long is suspended at rest from the ceiling by two springs, one at each end of the rod. Both springs hang straight down from the ceiling. The springs have identical lengths when they are unstretched. Their spring constants are 59 N/m and 33 N/m. Find the angle that the rod makes with the horizontal.

A block of mass \(\mathrm{m}=0.750 \mathrm{kg}\) is fastened to an unstrained horizontal spring whose spring constant is \(k=82.0 \mathrm{N} / \mathrm{m}\). The block is given a displacement of \(+0.120 \mathrm{m},\) where the \(+\) sign indicates that the displacement is along the \(+x\) axis, and then released from rest. (a) What is the force (magnitude and direction) that the spring exerts on the block just before the block is released? (b) Find the angular frequency \(\omega\) of the resulting oscillatory motion. (c) What is the maximum speed of the block? (d) Determine the magnitude of the maximum acceleration of the block.

A spiral staircase winds up to the top of a tower in an old castle. To measure the height of the tower, a rope is attached to the top of the tower and hung down the center of the staircase. However, nothing is available with which to measure the length of the rope. Therefore, at the bottom of the rope a small object is attached so as to form a simple pendulum that just clears the floor. The period of the pendulum is measured to be \(9.2 \mathrm{s}\). What is the height of the tower?

A horizontal spring is lying on a frictionless surface. One end of the spring is attached to a wall, and the other end is connected to a movable object. The spring and object are compressed by \(0.065 \mathrm{m}\), released from rest, and subsequently oscillate back and forth with an angular frequency of 11.3 rad/s. What is the speed of the object at the instant when the spring is stretched hy \(0.048 \mathrm{m}\) relative to its \(\mathrm{un}\) strained length?

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.