/*! 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 80 Between each pair of vertebrae i... [FREE SOLUTION] | 91Ó°ÊÓ

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Between each pair of vertebrae in the spinal column is a cylindrical disc of cartilage. Typically, this disc has a radius of about \(3.0 \times 10^{-2} \mathrm{m}\) and a thickness of about \(7.0 \times 10^{-3} \mathrm{m} .\) The shear modulus of cartilage is \(1.2 \times 10^{7} \mathrm{N} / \mathrm{m}^{2}\) . Suppose that a shearing force of magnitude 11 \(\mathrm{N}\) is applied parallel to the top surface of the disc while the bottom surface remains fixed in place. How far does the top surface move relative to the bottom surface?

Short Answer

Expert verified
The top surface moves approximately \(2.27 \times 10^{-6} \text{ m}.\)

Step by step solution

01

Understand the Problem

We need to find how far the top surface of the cartilage disc moves relative to the bottom when a shearing force is applied. This involves using the formula for shear deformation.
02

Recall the Shear Deformation Formula

The formula for shear deformation is \( \Delta x = \frac{F \cdot L}{A \cdot G} \), where \( \Delta x \) is the displacement, \( F \) is the force, \( L \) is the thickness of the disc, \( A \) is the area, and \( G \) is the shear modulus.
03

Calculate the Area of the Disc

The area \( A \) of the circular disc is given by \( A = \pi r^2 \). Using the radius \( r = 3.0 \times 10^{-2} \text{ m} \), we find \( A = \pi (3.0 \times 10^{-2})^2 \).
04

Substitute Values and Compute Area

Substitute the radius into the area formula: \[ A = \pi (3.0 \times 10^{-2})^2 = \pi \times 9.0 \times 10^{-4} = 2.827 \times 10^{-3} \text{ m}^2 \]
05

Substitute into Shear Deformation Formula

Now, substitute \( F = 11 \text{ N} \), \( L = 7.0 \times 10^{-3} \text{ m} \), \( A = 2.827 \times 10^{-3} \text{ m}^2 \), and \( G = 1.2 \times 10^7 \text{ N/m}^2 \) into the shear deformation formula: \[ \Delta x = \frac{11 \times 7.0 \times 10^{-3}}{2.827 \times 10^{-3} \times 1.2 \times 10^7} \]
06

Calculate Shear Deformation

Perform the calculation: \[ \Delta x = \frac{77 \times 10^{-3}}{3.3924 \times 10^4} = 2.27 \times 10^{-6} \text{ m} \] Thus, the top surface moves approximately \( 2.27 \times 10^{-6} \text{ m} \) relative to the bottom surface.

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Key Concepts

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

Shear Modulus
The shear modulus is a key concept when understanding how materials deform under shear stress. It is a measure of a material's rigidity or stiffness. Think of it as the "stiffness constant" for shear deformation. The larger the shear modulus, the stiffer the material and the less it deforms when shear force is applied.
\[ G = \frac{F}{A} \cdot \frac{1}{\Delta x / L} \]
In this formula, \( G \) represents the shear modulus, \( F \) the force applied, \( A \) the area over which the force is applied, \( \Delta x \) the resulting deformation, and \( L \) the original length or thickness of the material. In our exercise, the cartilage disc has a shear modulus of \( 1.2 \times 10^7 \, \mathrm{N/m}^2 \), indicating that it is reasonably stiff—which helps maintain spinal stability under various loads.
Cartilage Disc
Cartilage discs play a crucial role in our spine, acting as cushions between vertebrae. These discs handle various forces, including shearing forces. They are special because they allow slight movement between the bones, which is essential for flexibility and shock absorption.
These discs are like small, thick pancakes with a radius. In this exercise, the disc has a radius of \( 3.0 \times 10^{-2} \, \mathrm{m} \) and a thickness of \( 7.0 \times 10^{-3} \, \mathrm{m} \). These dimensions are important as they directly relate to the area and the shear deformation calculation when a force is applied. Understanding the physical properties of the cartilage disc is essential for calculating how much it deforms under stress.
Displacement Calculation
To calculate how much the top surface of a disc moves under a shearing force, we use the displacement formula for shear. The equation is:
\[ \Delta x = \frac{F \cdot L}{A \cdot G} \]
Here, \( \Delta x \) stands for the displacement, and it’s what we’re solving for. Substituting the known values from the cartilage disc problem, such as force \( F = 11 \, \mathrm{N} \), thickness \( L = 7.0 \times 10^{-3} \, \mathrm{m} \), area \( A = 2.827 \times 10^{-3} \, \mathrm{m}^2 \), and shear modulus \( G = 1.2 \times 10^7 \, \mathrm{N/m}^2 \), we follow through the calculation steps to determine the displacement. This calculation helps in understanding how the structure mechanically behaves under force.
Shearing Force
A shearing force is a type of force that causes shearing action—an effect where parts of a material slide past each other. In the context of our cartilage disc, this type of force is applied parallel to the surface of the disc, causing one side to move relative to the other.
The exercise gives us a shearing force of \( 11 \, \mathrm{N} \). This force's direction and magnitude affect how much deformation occurs. Different materials have different responses to shearing forces; thus, knowing the exact force and material properties allows us to predict and calculate the deformation accurately. Understanding shearing forces is essential because it explains how materials behave in real-world applications, especially in biological systems like the human spine.

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Most popular questions from this chapter

The length of a simple pendulum is 0.79 \(\mathrm{m}\) and the mass of the particle (the bob) at the end of the cable is 0.24 \(\mathrm{kg}\) . The pendulum is pulled away from its equilibrium position by an angle of \(8.50^{\circ}\) and released from rest. Assume that friction can be neglected and that the resulting oscillatory motion is simple harmonic motion. (a) What is the angular frequency of the motion? (b) Using the position of the bob at its lowest point as the reference level, determine the total mechanical energy of the pendulum as it swings back and forth. (c) What is the bob's speed as it passes through the lowest point of the swing?

A block rests on a frictionless horizontal surface and is attached to a spring. When set into simple harmonic motion, the block oscillates back and forth with an angular frequency of 7.0 \(\mathrm{rad} / \mathrm{s}\) . The drawing indicates the position of the block when the spring is unstrained. This position is labeled \( x=0 \mathrm{m} .\) The drawing also shows a small bottle located 0.080 \(\mathrm{m}\) to the right of this position. The block is pulled to the right, stretching the spring by \(0.050 \mathrm{m},\) and is then thrown to the left. In order for the block to knock over the bottle, it must be thrown with a speed exceeding \(v_{0}\) . Ignoring the width of the block, find \(v_{0}\) .

Astronauts on a distant planet set up a simple pendulum of length 1.2 \(\mathrm{m}\) . The pendulum executes simple harmonic motion and makes 100 complete vibrations in 280 s. What is the magnitude of the acceleration due to gravity on this planet?

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In preparation for shooting a ball in a pinball machine, a spring \((k=675 \mathrm{N} / \mathrm{m})\) is compressed by 0.0650 \(\mathrm{m}\) relative to its unstrained length. The ball \((m=0.0585 \mathrm{kg})\) is at rest against the spring at point A. When the spring is released, the ball slides (without rolling). It leaves the spring and arrives at point \(B\) , which is 0.300 m higher than point A. Ignore friction, and find the ball's speed at point B.

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