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In a pure shear state of stress, where the shear stresses are \( \tau \), the coordinates of X and Y to draw the Mohr circle are: (A) \( \left.\mathrm{X} \epsilon_{x}, \tau\right), \mathrm{Y}\left(\sigma_{y}, \tau\right) \) (B) \( \mathrm{X}(\tau, 0), \mathrm{Y}(-\tau, 0) \) (C) \( \mathrm{X}(0, \tau), Y(0,-\tau) \) (D) \( \mathrm{X}(0,0), Y(\tau,-\tau) \)

Ask by Parsons Watson. in Singapore
Feb 25,2025

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Answer

The correct coordinates for drawing the Mohr circle in a pure shear state are \( X(0, \tau) \) and \( Y(0, -\tau) \).

Solution

For a pure shear state, the normal stresses are zero while the shear stress is τ (or -τ on the opposite face). The stress tensor then has:   σₓₓ = 0, σyy = 0, τ_xy = τ In Mohr’s circle, the coordinates for a stress element are plotted as (normal stress, shear stress) = (σ, τ). The center of the circle is given by the average of the normal stresses:   σ_avg = (σₓₓ + σyy) / 2 = (0 + 0)/2 = 0 and the radius R is:   R = √[ ((σₓₓ - σyy)/2)² + τ² ] = √(0 + τ²) = τ Thus, the Mohr circle is centered at (0, 0) with radius τ. Its intersection with the shear stress axis are at:   (0, +τ) and (0, -τ) These are the coordinates used to draw the Mohr circle. Comparing with the given options, option (C) "X(0, τ), Y(0, -τ)" correctly represents the coordinates. So, the answer is (C).

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In a pure shear state of stress, the stress components can be visualized using Mohr's Circle. The correct coordinates for the points on the Mohr Circle for pure shear would be along the shear axis, where the normal stress components are equal to zero. So, you would plot the points at \( \mathrm{X}(0, \tau) \) and \( \mathrm{Y}(0, -\tau) \) for the Mohr Circle representation. This understanding is critical in fields like materials science and mechanical engineering, where Mohr's Circle helps visualize complex stress states. By using this graphical method, engineers can easily determine principal stresses, maximum shear stresses, and the orientation of the material under load—crucial for designing structures that can withstand various forces without failure!

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