/*! 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 43 A horizontal aluminum rod \(4.8 ... [FREE SOLUTION] | 91Ó°ÊÓ

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A horizontal aluminum rod \(4.8 \mathrm{~cm}\) in diameter projects \(5.3 \mathrm{~cm}\) from a wall. A \(1200 \mathrm{~kg}\) object is suspended from the end of the rod. The shear modulus of aluminum is \(3.0 \times 10^{10} \mathrm{~N} / \mathrm{m}^{2}\). Neglecting the rod's mass, find (a) the shear stress on the rod and (b) the vertical deflection of the end of the rod.

Short Answer

Expert verified
(a) Shear stress: \(6.51 \times 10^6 \text{ N/m}^2\). (b) Vertical deflection: \(1.15 \times 10^{-4} \text{ m}\).

Step by step solution

01

Calculate Area of Rod's Cross-section

The rod's cross-section is a circle with a diameter of \(4.8 \text{ cm}\). First, we convert the diameter to meters: \(d = 4.8 \text{ cm} = 0.048 \text{ m}\). The radius is half of the diameter, \(r = \frac{0.048}{2} = 0.024 \text{ m}\). The area \(A\) is calculated using the formula for the area of a circle, \(A = \pi r^2\). Substituting the radius, we get:\[A = \pi (0.024)^2 = 1.8096 \times 10^{-3} \text{ m}^2\].
02

Compute Shear Stress on the Rod

Shear stress \(\tau\) is calculated as the force applied divided by the area. The force \(F\) is from the weight of the object: \(F = mg\), where \(m = 1200 \text{ kg}\) and \(g = 9.81 \text{ m/s}^2\). Thus, \(F = 1200 \times 9.81 = 11772 \text{ N}\). Then \[\tau = \frac{F}{A} = \frac{11772}{1.8096 \times 10^{-3}} = 6.51 \times 10^6 \text{ N/m}^2\].
03

Determine the Vertical Deflection of the Rod

The vertical deflection \(\Delta L\) for a cantilever rod can be found using the formula: \[\Delta L = \frac{FL}{AG}\] where \(F\) is the force, \(L = 0.053 \text{ m}\) is the length of the rod, \(A\) is the cross-sectional area, and \(G = 3.0 \times 10^{10} \text{ N/m}^2\) is the shear modulus. Substituting the known values, we have:\[\Delta L = \frac{11772 \times 0.053}{1.8096 \times 10^{-3} \times 3.0 \times 10^{10}} = 1.15 \times 10^{-4} \text{ m} \].

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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, often denoted as \( G \), is a measure of how a material will deform under shear stress. It quantifies the relationship between the applied shear stress and the resultant shear strain. In simple terms, if you apply a force that tries to slide layers of the material over each other, the shear modulus will tell you how much those layers will actually move.
For aluminum, which is the material of the rod in our exercise, the shear modulus is quite high at \( 3.0 \times 10^{10} \text{ N/m}^2 \). This means aluminum is relatively resistant to shear deformation, which is beneficial in situations where structural integrity is crucial. Always remember, a higher shear modulus indicates material is stiffer in terms of shear.
  • Shear modulus helps determine how a material behaves under shear forces.
  • It is crucial for predicting material performance in engineering applications.
Deflection of Cantilever
Deflection in cantilever beams is the bending or displacement of a beam when a force is applied at one end, while the other end is fixed. The amount of deflection is critical as it dictates how much a structure will move under load.
For the horizontal aluminum rod in our exercise, which acts like a cantilever, the deflection is calculated using the relation \( \Delta L = \frac{FL}{AG} \). Here, \( F \) is the force (due to the 1200 kg weight), \( L \) is the length of the beam extending from the wall, \( A \) is the cross-sectional area, and \( G \) is the shear modulus. Substituting the values provided gives the deflection as \( 1.15 \times 10^{-4} \text{ m} \). This formula is a cornerstone in structural engineering for ensuring safe and efficient designs when dealing with overhanging structures.
  • Cantilever deflection needs to be minimized for safety and durability.
  • Excessive deflection can lead to structural failure or operational issues.
Area of Circle
The area of a circle is a fundamental concept that frequently appears in calculations involving round or cylindrical objects. The formula for calculating this area is \( A = \pi r^2 \), where \( r \) is the radius. The radius is half the diameter. For our problem, converting the diameter of 4.8 cm to meters, we have:
\[ r = \frac{0.048}{2} = 0.024 \text{ m} \]
Thus, the area calculation becomes: \[ A = \pi (0.024)^2 = 1.8096 \times 10^{-3} \text{ m}^2 \] This area is critical as it is used to determine how much stress the rod can handle before deformation occurs. In structural contexts, knowing how to compute the area of a circle ensures that components can be correctly designed to withstand applied forces.
  • The area of a circle is key in stress and load calculations.
  • Ensuring accurate area measurements is crucial for component strength.
Force Calculation
Calculating force involves understanding Newton's second law, which states that Force (\( F \)) equals mass (\( m \)) times acceleration (\( a \)), typically gravitational acceleration (\( g \)) when dealing with suspended weights: \[ F = mg \]
In this exercise, a 1200 kg object is hanging from the aluminum rod, so the force is calculated as: \[ F = 1200 \times 9.81 = 11772 \text{ N} \]This force value is essential for further calculations, like determining the shear stress experienced by the rod or the resulting deflection. Thus, accurate force calculations are paramount in ensuring the stability and safety of structures.
  • Force calculations are fundamental in determining structural reactions.
  • Precise force application helps in assessing material suitability and safety margins.

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Most popular questions from this chapter

A \(73 \mathrm{~kg}\) man stands on a level bridge of length \(L .\) He is at distance \(L / 4\) from one end. The bridge is uniform and weighs \(2.7 \mathrm{kN}\). What are the magnitudes of the vertical forces on the bridge from its supports at (a) the end farther from him and (b) the nearer end?

A meter stick balances horizontally on a knife-edge at the \(50.0 \mathrm{~cm}\) mark. With two \(5.00 \mathrm{~g}\) coins stacked over the \(12.0 \mathrm{~cm}\) mark, the stick is found to balance at the \(45.5 \mathrm{~cm}\) mark. What is the mass of the meter stick?

A \(75 \mathrm{~kg}\) window cleaner uses a \(10 \mathrm{~kg}\) ladder that is \(5.0 \mathrm{~m}\) long. He places one end on the ground \(2.5 \mathrm{~m}\) from a wall, rests the upper end against a cracked window, and climbs the ladder. He is \(3.0 \mathrm{~m}\) up along the ladder when the window breaks. Neglect friction between the ladder and window and assume that the base of the ladder does not slip. When the window is on the verge of breaking, what are (a) the magnitude of the force on the window from the ladder, (b) the magnitude of the force on the ladder from the ground, and (c) the angle (relative to the horizontal) of that force on the ladder?

A rope of negligible mass is stretched horizontally between two supports that are 3.44 m apart. When an object of weight 3160 N is hung at the center of the rope, the rope is observed to sag by 35.0 cm. What is the tension in the rope?

Figure 12-61 represents an insect caught at the midpoint of a spider-web thread. The thread breaks under a stress of \(8.20 \times 10^{8} \mathrm{~N} / \mathrm{m}^{2}\) and a strain of 2.00. Initially, it was horizontal and had a length of \(2.00 \mathrm{~cm}\) and a cross-sectional area of \(8.00 \times\) \(10^{-12} \mathrm{~m}^{2}\). As the thread was stretched under the weight of the insect, its volume remained constant. If the weight of the insect puts the thread on the verge of breaking, what is the insect's mass? (A spider's web is built to break if a potentially harmful insect, such as a bumble bee, becomes snared in the web.)

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