Category: Advance Concept Mechanical Eng
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TEMPERATURE STRESS
If the temperature of a material is increased, there will be expansion in the material (except ice) and if the temperature is decreased, there will be contraction in the material. If these expansion and contraction occur freely there will be no stress in the material and if these expansion or contraction is prevented then stress…
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STRESS AND STRAIN IN COMPOSITE BAR
Any tensile or compressive member which consists of two or more bars in series, usually of different materials, is called composite bars (Figure 12.18). In this case, load on both the rods will be same but strain produced will be different. Figure 12.18 Composite Bar where A1, E1 ∈1 are cross-section area, modulus of elasticity, and strain produced in material…
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STRESS AND STRAIN IN AN ASSEMBLY OF TUBE AND BOLT
Figure 12.13 shows stress and strain produced in a compound rod. Figure 12.13 An Assembly of Tube and Bolt where r subscript is used for rod. Rod is subjected to tensile stress and tube is subjected to compressive stress. The reduction in length of tube and extension in rod may be different due to difference in materials…
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STRESS AND STRAIN IN COMPOUND BAR
Any tensile or compressive member which consists of two or more bars or tubes in parallel, usually of different materials, is called a compound bar. Figure 12.12 shows an example of compound bar; it consists of a tube and a rod of different materials. Since the initial length of tube and rod are same, it will remain…
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STRESS AND STRAIN IN VARYING CROSS-SECTION BAR OF UNIFORM STRENGTH
Consider a bar of varying cross-section of uniform strength subjected by a longitudinal stress σ as shown in Figure 12.10. Now consider a small element of axial length δx at a distance of x from smaller end. Let area of cross-section at section x be A and at section x + δx be A + δA. For the element of length δx to be in equilibrium, the total downward force must be equal to the total…
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EXTENSION IN VARYING CROSS-SECTION OR TAPER ROD
A rod of length l tapers uniformly from a diameter D at one end to diameter d at other end as shown in Figure 12.8. Considering an small element of thickness dx at distance x from the end of diameter d, the diameter of the element is calculated as Figure 12.8 Extension in Taper Rod Example 12.4: A rod tapers uniformly from 50 to 20 mm diameter in a length…
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HOOKE’S LAW
Hooke’s law states that stress and strain are proportional to each other under elastic limit. Originally, Hooke’s law specified that stress was proportional to strain but later Thomas Young introduced constant of proportionality which is known as Young’s modulus of elastic. Further, this name was superseded by modulus of elasticity. Figure 12.3 demonstrates the Hooke’s Law. Figure…
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INTRODUCTION TO STRESS AND STRAIN
There are certain behaviours of all materials under the influence of external force. Stress and strain are one of the measures to show these behaviours. Stress is a resistive force per unit area, which is developed internally to oppose the external force subjected to the material. Strain is a measure of deformation of the material…
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Mass Moment of Inertia of a Circular Cone
Consider an elemental plate at a distance x from apex of radius r and thickness dx as shown in Figure 11.25. Mass of elemental plate = ρπr2dx. Figure 11.25 Mass Moment of Inertia of Circular Cone about Its Axis of Rotation The moment of inertia of circular plate about normal axis through its centre is Moment of inertia of the elemental plate about the axis…
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Mass Moment of Inertia of Sphere
Consider an elemental plate of thickness dy at a distance y from the diametral axis as shown in Figure 11.24. Radius of this elemental circular plate x is given by, Figure 11.24 Mass Moment of Inertia of Sphere x2 = R2 − y2 Mass of the elemental plate, dm = ρπx2 dy = ρπ (R2 − y2)dy Moment of inertia of the plate element about axis But, mass of sphere, Mass moment of inertia of hemisphere…