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OPTI 222 Mechanical Design in Optical Engineering
98
Mohr's Circle for Plane Stress
Analysis of Stress and Strain:
As we learned in the previous two lectures, when a structural element is subjected to
several types of loads acting simultaneously, say bending and torsion, principal stresses
occur. These stresses act on principal planes where the shear stresses are zero. In
addition, many engineering problems, such as axial bars, beams in bending and circular
members in torsion, are examples of a state of stress called plane stress (σz = τzx = τzy
= 0). Our procedure for determining principal stresses for a state of plane stress is as
follows:
1. Determine the point on the body in which the principal stresses are to be
determined.
2. Treating the load cases independently and calculated the stresses for the
point chosen. When applicable combine the stresses to determine the state
of stress at the point.
3. Choose a set of x-y reference axes and draw a square element centered on
the axes.
4. Identify the stresses σx, σy, and τxy = τyx and list them with the proper
direction.
5. Calculate the principal stresses, the maximum shear stress and the principal
plane if required.
Principal Stresses (Shear Stress = 0):
2
2
1
2 2
x y x y
xy
σ σ σ σ
σ τ
+ − 
= + + 
 
2
2
2
2 2
x y x y
xy
σ σ σ σ
σ τ
+ − 
= − + 
 
Maximum Shear Stress:
2
2
max
2
x y
xy
σ σ
τ τ
− 
= + 
 
1 2
max
2
σ σ
τ
−
=
OPTI 222 Mechanical Design in Optical Engineering
99
Principal Planes (Planes on which Principal Stresses Act):
1
2
2 tan
xy
p
x y
τ
θ
σ σ
−
=
−
Plane of Maximum Shear Stress:
1
2 tan
2
x y
s
xy
σ σ
θ
τ
−
−
= −
Average Stress (Shear Stress is Maximum):
2
x y
avg
σ σ
σ
+
=
Important Observations:
1. Principal stresses occur on mutually perpendicular planes.
2. Shear stresses are zero on principal planes.
3. Planes of maximum shear stress occur at 45° to the principal planes.
4. The maximum shear stress is equal to one half the difference of the principal
stresses.
It should be noted that the equation for principal planes, 2θp, yields two angles between
0° and 360°. Which one corresponds to σ1 and which to σ2? This can be determined by
substituting one of the values into the stress transformation equation for normal stress.
Normal Stress Transformation
cos2 sin2
2 2
x y x y
n xy
σ σ σ σ
σ θ τ θ
+ −
= + +
Shear Stress Transformation
( ) ( )2 2
sin cos cos sinnt x y xyτ σ σ θ θ τ θ θ= − − + −
OPTI 222 Mechanical Design in Optical Engineering
100
Example Problem:
Determine:
a) The principal planes.
b) The principal stresses.
c) The maximum shear stress and the corresponding normal stress.
Mohr’s Circle for Plane Stress:
The transformation equations for plane stress can be represented in a graphical format
known as Mohr’s circle. This representation is useful in visualizing the relationships
between normal and shear stresses acting on various inclined planes at a point in a
stressed body.
Before we discuss the procedure for constructing Mohr’s circle there a several rules that
apply.
Stress Component Plot
Normal Stresses + For Tension
(Horizontal Axis) - For Compression
Shear Stresses + For Clockwise Shear
(Vertical Axis) - For Counterclockwise Shear
OPTI 222 Mechanical Design in Optical Engineering
101
Construct Mohr’s circle as follows:
1. Determine the point on the body in which the principal stresses are to be
determined.
2. Treating the load cases independently and calculated the stresses for the point
chosen.
3. Choose a set of x-y reference axes and draw a square element centered on the
axes.
4. Identify the stresses σx, σy, and τxy = τyx and list them with the proper sign.
5. Draw a set of σ - τ coordinate axes with σ being positive to the right and τ being
positive in the upward direction. Choose an appropriate scale for the each axis.
6. Using the rules on the previous page, plot the stresses on the x face of the
element in this coordinate system (point V). Repeat the process for the y face
(point H).
7. Draw a line between the two point V and H. The point where this line crosses the
σ axis establishes the center of the circle.
8. Draw the complete circle.
9. The line from the center of the circle to point V identifies the x axis or reference
axis for angle measurements (i.e. θ = 0).
Note: The angle between the reference axis and the σ axis is equal to 2θp.
Mohr’s Circle:
OPTI 222 Mechanical Design in Optical Engineering
102
Consider the previous example.

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Mohr circle

  • 1. OPTI 222 Mechanical Design in Optical Engineering 98 Mohr's Circle for Plane Stress Analysis of Stress and Strain: As we learned in the previous two lectures, when a structural element is subjected to several types of loads acting simultaneously, say bending and torsion, principal stresses occur. These stresses act on principal planes where the shear stresses are zero. In addition, many engineering problems, such as axial bars, beams in bending and circular members in torsion, are examples of a state of stress called plane stress (σz = τzx = τzy = 0). Our procedure for determining principal stresses for a state of plane stress is as follows: 1. Determine the point on the body in which the principal stresses are to be determined. 2. Treating the load cases independently and calculated the stresses for the point chosen. When applicable combine the stresses to determine the state of stress at the point. 3. Choose a set of x-y reference axes and draw a square element centered on the axes. 4. Identify the stresses σx, σy, and τxy = τyx and list them with the proper direction. 5. Calculate the principal stresses, the maximum shear stress and the principal plane if required. Principal Stresses (Shear Stress = 0): 2 2 1 2 2 x y x y xy σ σ σ σ σ τ + −  = + +    2 2 2 2 2 x y x y xy σ σ σ σ σ τ + −  = − +    Maximum Shear Stress: 2 2 max 2 x y xy σ σ τ τ −  = +    1 2 max 2 σ σ τ − =
  • 2. OPTI 222 Mechanical Design in Optical Engineering 99 Principal Planes (Planes on which Principal Stresses Act): 1 2 2 tan xy p x y τ θ σ σ − = − Plane of Maximum Shear Stress: 1 2 tan 2 x y s xy σ σ θ τ − − = − Average Stress (Shear Stress is Maximum): 2 x y avg σ σ σ + = Important Observations: 1. Principal stresses occur on mutually perpendicular planes. 2. Shear stresses are zero on principal planes. 3. Planes of maximum shear stress occur at 45° to the principal planes. 4. The maximum shear stress is equal to one half the difference of the principal stresses. It should be noted that the equation for principal planes, 2θp, yields two angles between 0° and 360°. Which one corresponds to σ1 and which to σ2? This can be determined by substituting one of the values into the stress transformation equation for normal stress. Normal Stress Transformation cos2 sin2 2 2 x y x y n xy σ σ σ σ σ θ τ θ + − = + + Shear Stress Transformation ( ) ( )2 2 sin cos cos sinnt x y xyτ σ σ θ θ τ θ θ= − − + −
  • 3. OPTI 222 Mechanical Design in Optical Engineering 100 Example Problem: Determine: a) The principal planes. b) The principal stresses. c) The maximum shear stress and the corresponding normal stress. Mohr’s Circle for Plane Stress: The transformation equations for plane stress can be represented in a graphical format known as Mohr’s circle. This representation is useful in visualizing the relationships between normal and shear stresses acting on various inclined planes at a point in a stressed body. Before we discuss the procedure for constructing Mohr’s circle there a several rules that apply. Stress Component Plot Normal Stresses + For Tension (Horizontal Axis) - For Compression Shear Stresses + For Clockwise Shear (Vertical Axis) - For Counterclockwise Shear
  • 4. OPTI 222 Mechanical Design in Optical Engineering 101 Construct Mohr’s circle as follows: 1. Determine the point on the body in which the principal stresses are to be determined. 2. Treating the load cases independently and calculated the stresses for the point chosen. 3. Choose a set of x-y reference axes and draw a square element centered on the axes. 4. Identify the stresses σx, σy, and τxy = τyx and list them with the proper sign. 5. Draw a set of σ - τ coordinate axes with σ being positive to the right and τ being positive in the upward direction. Choose an appropriate scale for the each axis. 6. Using the rules on the previous page, plot the stresses on the x face of the element in this coordinate system (point V). Repeat the process for the y face (point H). 7. Draw a line between the two point V and H. The point where this line crosses the σ axis establishes the center of the circle. 8. Draw the complete circle. 9. The line from the center of the circle to point V identifies the x axis or reference axis for angle measurements (i.e. θ = 0). Note: The angle between the reference axis and the σ axis is equal to 2θp. Mohr’s Circle:
  • 5. OPTI 222 Mechanical Design in Optical Engineering 102 Consider the previous example.