notes on asymmetrical beam bending
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uni/mmme/2xxx/2053_mechanics_of_solids/asymmetrical_bending.md
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---
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author: Akbar Rahman
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date: \today
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title: MMME2053 // Asymmetrical Beam Bending
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tags: [ mmme2053, beam_bending, asymmetrical_beam_bending ]
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uuid: 7afb5f13-4d55-4e00-927a-5d622520d844
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---
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# Product Moments of Area
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To analyse asymmetrically loaded sections, we need the second moments of area $I_{yy}$, and $I_{xx}$
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but we also need $I_{xy}$, the product moment of area:
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$$I_{xy} = \int_A xy \mathrm{d}A$$
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# Parallel Axis Theorem
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The parallel axis theorem allows calculation of 2nd moments of area and product moments of area with
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respect to $x'$ and $y'$ axes:
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![](./images/vimscrot-2023-02-02T14:40:20,244467338+00:00.png)
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\begin{align*}
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I_{x'x'} &= \int_A y'^2 \mathrm{d}A \\
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&= \int_A (y+b)^2 \mathrm{d}A \\
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&= \int_A (y^2 + b^2 + 2by) \mathrm{d}A \\
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\\
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I_{x'x'} &= I_{xx} + Ab^2
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\end{align*}
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Similarly you can get
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\begin{align*}
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I_{y'y'} &= I_{yy} + Aa^2 \\
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I_{x'y'} &= I_{xy} + abA
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\end{align*}
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# Principal Axes and Principal 2nd Moments of Area
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Once the second moments of area and product moments are found, they can be used to plot a Mohr's circle where:
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- Point A is plotted at $(I_{xx}, I_{xy})$
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- Point B is plotted at $(I_{yy}, -I_{xy})$
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- Points P and Q show the positions of the principal 2nd moments of area, $I_p$, and $I_q$.
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- $\theta$ is the angular position $e$ of the principal axes with respect to the $x$-$y$ axes
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The principal axes are the axes where the product moment of area is 0.
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![](./images/vimscrot-2023-02-02T14:44:15,574579179+00:00.png)
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$$C = \frac{I_{xx} + I_{yy}}{2}$$
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$$R = \sqrt{\left(\frac{I_{xx}-I{yy}}{2}\right)^2 + I_{xy}^2}$$
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$$I_p = C + R$$
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$$I_q = C - R$$
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$$\sin{2\theta} = \frac{I_{xy}}{R}$$
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# Analyse Bending of a Beam with Asymmetric Section by Resolving Bending Moments onto Princial Axes
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![](./images/vimscrot-2023-02-02T14:53:05,040998048+00:00.png)
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If a bending moment, $M_x$ is applied about the x-axis only, then the stress in the flanges will
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cause bending to takeplace about both x and y axes.
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This is a consequence of $I_{xy} \neq 0$.
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To avoid this moment coupling effect, it is usually convenient to solve bending problems by
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considering bending about the principal axes, for which $I_{xy} = 0$.
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## Resolving onto Principal Axes
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![](./images/vimscrot-2023-02-02T14:54:13,309546586+00:00.png)
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If bending moments $M_x$ and $M_y$ are applied about the x and y axes respectively, these can be
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resolved onto the principal axes, P and Q:
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![](./images/vimscrot-2023-02-02T14:54:26,513070327+00:00.png)
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\begin{align*}
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\cos\theta &= \frac{M_{P_x}}{M_x} \rightarrow M_{P_x} = M_x\cos\theta\\
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\sin\theta &= \frac{-M_{Q_x}}{M_x} \rightarrow M_{Q_x} = -M_x\sin\theta\\
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\end{align}
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![](./images/vimscrot-2023-02-02T14:54:32,264829706+00:00.png)
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Similarly we get:
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\begin{align*}
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M_{P_y} = M_y\sin\theta\\
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M_{Q_y} = M_y\cos\theta\\
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\end{align}
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Therefore:
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\begin{align*}
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M_P = M_{P_x} + M_{P_y} = M_x\cos\theta + M_y\sin\theta \\
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M_Q = M_{Q_x} + M_{Q_y} = -M_x\sin\theta + M_y\cos\theta \\
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\end{align*}
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## Bending Stress at Position (P, Q)
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![](./images/vimscrot-2023-02-02T15:02:36,806587572+00:00.png)
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$$\sigma = \frac{M_PQ}{I_P} - \frac{M_QP}{I_Q}$$
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Note the -ve sign, as a positive stress results in a -ve moment about the y-axis.
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## Position of the Neutral Axis
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![](./images/vimscrot-2023-02-02T15:09:13,105535645+00:00.png)
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The neutral axis is where $\sigma = 0$:
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\begin{align*}
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\frac{M_PQ}{I_P} &= \frac{M_QP}{I_Q} \\
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\frac Q P &= \frac{M_QI_P}{M_PI_Q} \\
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\\
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\alpha &= \arctan\frac{Q}{P}
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\end{align*}
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The maximum stress is located in cross section point which is furthest from the neutral axis.
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## Procedure for Solving for Bending Stress and Neutral Axis Position in Asymmetrical Bending Problems
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1. [Determine the principal axes](#Principal-Axes-and-Principal-2nd-Moments-of-Area) of the section (about which $I_{xy}= 0$)
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2. [Resolve bending moments onto these axes](#resolving-onto-principal-axes)
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3. [Determine angle of neutral axis](#position-of-neutral-axis)
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4. Evaluate bending stress at any poisition in the section, such as extremes away from neutral axis, which give maximum bending stress
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# Worked Example
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- [Worked Example 1 (PDF)](./worked_examples/MMME2053 AB WE1 Slides.pdf)
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- [Worked Example 2 (PDF)](./worked_examples/MMME2053 AB WE2 Slides.pdf)
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