Principal stress: Definition, Equation, Example, Explained

For the safe design of the component, it is necessary to know about the maximum stresses acting inside the component and its location.

The principal stress gives the maximum normal stress acting inside the component and its position. In this article, we will go through comprehensive information on principal stress.

Contents

What is Principal stress?

Principal stress is the normal stress acting onto the principal plane that has zero shear stress.

The above figure. A shows the member subjected to the axial stresses as well as shear stresses and figure. B shows the principal stresses and principal planes.

A principal plane is an oblique plane that bears no shear stress. The principal planes lie at a principal angle (\theta_{p}) from the reference plane as shown in the figure. B and there is no shear stress acts on it.

The normal stresses acting on that plane ( \sigma_{1} and \sigma_{2}) are the principal stresses.

Principal stress explained:

The member shown in the figure. A is subjected to the axial stresses in the x and y direction and complementary shear stresses on horizontal and vertical planes.

Other than horizontal and vertical planes, the member has numerous inclined planes that are inclined at an angle θ (0° to 90°) from the reference plane, These planes are known as the Oblique planes.

As shown in the above figure. B, the oblique plane OA experiences the following two types of stresses:-

A] Normal stress (σₙ):- The stress perpendicular to the oblique plane is the normal stress (\sigma_{n}).
The normal stress on an oblique plane that is inclined at angle θ is given by,

\sigma_{n}=(\frac{\sigma_{x}+\sigma_{y}}{2})+(\frac{\sigma_{x}-\sigma_{y}}{2})cos2\theta + \tau_{xy}sin2\theta

b] Shear stress (𝜏):- The stress acting parallel to the plane is the shear stress on an oblique plane. It is given by,

\tau=(\frac{\sigma_{x}-\sigma_{y}}{2})sin2\theta-\tau_{xy} cos2\theta

Now let’s understand what is principal plane and principal stress.

Principal plane:- It is the oblique plane that experiences zero shear stress.

For the components subjected to biaxial stresses, there are two planes on which the value of shear stress is zero.

Thus to find a position of this principal plane (θ𝗽) from the reference plane, put \tau = 0 in the equation of \tau.

0=(\frac{\sigma_{x}-\sigma_{y}}{2})sin2\theta_{P}-\tau_{xy} cos2\theta_{P}

(\frac{\sigma_{x}-\sigma_{y}}{2})sin2\theta_{P}=\tau_{xy} cos2\theta_{P}

\frac{sin2\theta_{P}}{cos2\theta_{P}}=\frac{2\tau_{xy}}{\sigma_{x}-\sigma_{y}}

tan2\theta_{P}=\frac{2\tau_{xy}}{\sigma_{x}-\sigma_{y}}

\therefore \theta_{P}=\frac{1}{2}tan^{-1}.(\frac{2\tau_{xy}}{\sigma_{x}-\sigma_{y}})

This is the position of the principal plane from the reference plane.

Principal stress:- The normal stress acts onto the principal plane is known as the principal stress.
For biaxial (2D) stress conditions, there are two principal stresses known as Major principal stress and minor principal stress.

What is Maximum and Minimum principal stress?

For the member subjected to the biaxial stresses, the two principal stresses are as follows:-

Maximum principal stress:-

Maximum principal stress or major principal stress is the maximum value of normal stress acting on one of the principal planes where the value of shear stress is zero.

The value of maximum principal stress is given by,

\sigma_{1}=(\frac{\sigma_{x}+\sigma_{y}}{2})+\sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}-\tau_{xy}^{2}}

Minimum principal stress:-

Minimum or minor principal stress is the minimum value of principal stress acting on one of the principal planes where the value of shear stress is zero.

The value of minimum principal stress is given by,

\sigma_{2}=(\frac{\sigma_{x}+\sigma_{y}}{2})-\sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}-\tau_{xy}^{2}}

How to calculate Maximum and Minimum principal stress?

If the values of the axial stresses (\sigma_{x} and \sigma_{y}) and complementary shear stresses (\tau_{xy} or \tau_{yx}) are known, then the maximum and minimum principal stress can be calculated by the following methods:-

1] Analytical method:-

In the analytical method, the principal stresses can be calculated by using the following formulae,

\sigma_{\text{max}}=\sigma_{1} = (\frac{\sigma_{x}+\sigma_{y}}{2})+\sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}+\tau_{xy}^{2}}

\sigma_{\text{min}} = \sigma_{2}=(\frac{\sigma_{x}+\sigma_{y}}{2})-\sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}+\tau_{xy}^{2}}

2] Graphical method (Mohr’s circle):-

The mohr’s circle is another and easy method to find the stresses on each oblique plane and principal stresses.

From above mohr’s circle,

\sigma_{\text{max}}=\sigma_{1}=\text{Distance OF}
\sigma_{\text{min}}=\sigma_{2}=\text{Distance OG}

Principal stress sign convention:

Following is the sign convention used for the principal stress:-

1] Axial force:-

The tensile axial force is considered positive.

The compressive axial force is considered negative.

2] Complementary shear stress:-

If the shear stress on the vertical plane (shown by red arrows) is in a clockwise sense, then it is considered as positive.

If the shear stresses on the vertical plane (shown by red arrows) are in an anticlockwise sense, then it is considered as negative.

Principal stress example:

1] The state of stress on members is shown below, find the maximum and minimum amount of principal stress.

Given:
\sigma_{x} = 100 Mpa
\sigma_{y} = 45 Mpa
\tau_{\text{xy}} = 30 Mpa

Solution:-

The maximum principal stress on the member is given by,

\sigma_{1} = (\frac{\sigma_{x}+\sigma_{y}}{2}) + \sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}+\tau_{xy}^{2}}

\sigma_{1} = (\frac{100+45}{2}) + \sqrt{(\frac{100-45}{2})^{2}+30^{2}}

\mathbf{\sigma_{1}} = 113.197 Mpa

The minimum principal stress on a member is given by,

\sigma_{1} = (\frac{\sigma_{x}+\sigma_{y}}{2}) – \sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}+\tau_{xy}^{2}}

\sigma_{1} = (\frac{100+45}{2}) – \sqrt{(\frac{100-45}{2})^{2}+30^{2}}

\mathbf{\sigma_{2}} = 31.802 Mpa

2] Find the stresses acting on the principal planes for the below stress condition.

Given:
\sigma_{x} = 50 Mpa
\sigma_{y} = -75 Mpa
\tau_{xy} = 20 Mpa

Solution:-

The stresses acting on the plane is a principal plane is given by,

\sigma_{1}=\frac{\sigma_{x}+\sigma_{y}}{2}+ \sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}+\tau_{xy}^{2}}

\sigma_{1}=\frac{50+(-75)}{2}+\sqrt{(\frac{50-(-75)}{2})^{2} +20^{2}}

\sigma_{1} = 53.122 MPa

\sigma_{2}=\frac{\sigma_{x}+\sigma_{y}}{2}-\sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}+\tau_{xy}^{2}}

\sigma_{2}=\frac{\sigma_{x}+\sigma_{y}}{2}-\sqrt{(\frac{\sigma_{x}-\sigma_{y}}{2})^{2}+\tau_{xy}^{2}}

\sigma_{2} = -78.122 MPa

Thus the principal stresses for the above biaxial stress condition are,
\sigma_{1}=\text{53.122 MPa}
\sigma_{2}=\text{-78.122 MPa}

FAQs:

1. What exactly is principle stress?

Principal stress is the normal stress acting onto the principal plane.

2. What is the purpose of principle stress?

The principal stress is the maximum normal stress acting on the object which is considered as criteria for the maximum principal stress theory of failure.

3. What mean by the 1st principal stress?

The principal stress that has the maximum value is known as the first principal stress.

4. How do you find principal stresses and directions?

The value of the principal stresses and their directions can be found by using analytical formulae or by using mohr’s circle.

5. What is the major principal stress?

The maximum value of normal stress acting on any one of the principal planes is known as the maximum principal stress.

6. Can maximum principal stress have a negative value?

The maximum principal stress can be positive or negative which is decided on the basis of the direction of the stress. If the principal stress is compressive then it is considered negative and if it is tensile then it is considered positive.

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Pratik is a Graduated Mechanical engineer. He enjoys sharing the engineering knowledge learned by him with people.

1 thought on “Principal stress: Definition, Equation, Example, Explained”

1. Great stuff. Thanks a lot.