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I am trying to create a MATLAB script to plot the Bending Moment Diagram (BMD) and Shear Force Diagram (SFD) as a function of spanwise distance, x, along a wing from the wing root (x=0) to the wingtip (x=b/2).

I will be considering the case where the lift generated by the wing is 2.5 times the weight of the wing (so n=2.5).

The three main forces I plan to consider in this analysis are: 1) The weight of the engine (Point load) 2) The weight of the wing (uniformly distributed load) 3) The lift generated by the wing (bell loading distribution)

My question is this: how can I set up an equation for the bending moment and shear force as a function of spanwise distance, x, despite a non-uniformly distributed load being considered in combination with a point load and a uniformly distributed load?

The classes I have taken at college have only covered BMD and SFD for uniformly distributed loads, so I am a bit confused as to how to go about setting up a numerical model for a non-uniform load.

Thanks a lot.

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  • $\begingroup$ Could you perhaps add a force body diagram to your question? And could you approximate the non-uniform distributed loads force equivalent via integrating, and the location via the centroid? $\endgroup$ – Nile River Mar 2 at 21:35
  • $\begingroup$ You can readily solve this analytically using superposition of your load cases. I can highly recommend Mechanics of Solids by Roger T. Fenner. The chapter on beam bending will have all you need and more. But feel free to use numerical methods if you just want an answer instead of fully understanding the underlying physics. $\endgroup$ – Sanchises Aug 3 at 19:08
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I would highly recommend to discretize your problem, for two reasons:

  1. You are using Matlab which is most suitable for a discrete approach anyways
  2. More complex load cases will make analytical continuous modelling difficult. This is why these kind of problems are typically solved numerically

So now the question how can we discretly regard this problem? For the wing bending moment, this is pretty straightforward. First of all, lets make a small sketch.

Sketch of the situation

The process of discretization is now to look at equally spaced points of the wing seperated by the distance Δd. I call them discretization points. I have labeled them in the following sketch as a vertical line numbered as 1, 2, 3 ... until point i.

Discretization

What you need to do now, is to calculate the force acting on each discrete point. This part in turn is divided into two parts:

  1. Calculating the exact shape of the different forces: Therefore force of motor weight, force of the wing structure and as a function of these two, the bell function of the lift
  2. Integrate the wing lift force and structural weight force from discretization point k-1 to point k.

Now you have the exact weight acting on each point k (simply the integration of the wing lift force and the structural weight force from point k-1 to point k). Calculating the bending moment is now straightforward. For example, the bending moment at point i-1 is just the force acting on point i times the distance from point i-1 to i:

$$ M_{i-1} = i \cdot \Delta d \cdot F_i $$

the bending moment at point i-2 is now therefore:

$$M_{i-2} = 2*\Delta d \cdot F_i + \Delta d \cdot F_{i-1}$$

and so forth and so on.

The shear force at these points is even simpler. It is just the sum of all forces at the different outboard. So for example at point i-2:

$$ F_{i-2} = F_i + F_{i-1} $$

You can see that this type of equations can be easily programmed in Matlab. If you program this a bit cleverly, you can even play around with different values of Δd, which enables you to see the effects of discretization.

Hope this helps. If you need more help with the code, feel free to ask.

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  • $\begingroup$ welcome to community. $\endgroup$ – Kolom Aug 3 at 19:39
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To include the point force from the engine mount you will need to use a Dirac delta and a Heaviside step function to add in the moment caused by the engine.

The Dirac delta multiplied by the engine weight will model the force, and once you integrate over the span once to obtain the moments it naturally will turn into the Heaviside step function.

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