Minimizing the maximum bending moment

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Discussion Overview

The discussion revolves around minimizing the maximum bending moment in a beam subjected to a uniformly distributed load. Participants explore the implications of varying the distance between supports and the resulting effects on the bending moment, engaging in a problem-solving context related to structural mechanics.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation

Main Points Raised

  • One participant assumes a uniform force distribution and derives expressions for shear force and bending moment across different segments of the beam.
  • Another participant suggests that the answer in the back of the book might be a specific value of "a" related to the beam length.
  • A participant indicates that moving the supports affects the maximum moment, suggesting a need to find an optimal value for "a" to minimize this moment.
  • One participant claims to have solved the problem, providing a formula for "a" in terms of the beam length.
  • Another participant confirms the solution and provides a simplification of the derived formula for "a".

Areas of Agreement / Disagreement

Participants express differing views on the assumptions regarding the uniform distribution of load and the derived values for "a". While some participants agree on the final expression for "a", the initial assumptions and methods of derivation remain contested.

Contextual Notes

The discussion includes various mathematical steps and simplifications that may depend on specific assumptions about the load distribution and beam configuration. Some expressions and derivations are not universally accepted, indicating potential gaps in consensus.

gpavanb
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Homework Statement



Refer to the attachment provided

Homework Equations



Just taking force and moment equilibium of whatever component I choose.

The Attempt at a Solution



I assumed a uniform force distribution.
Set the origin at the leftmost end. For 0< x < \frac{L-a}{2}
The shear force acting is +qx and the bending moment is \frac{-qx^{2}}{2}
Note that the situation is symmetrical w.r.t the centre of the beam.
Now for \frac{L-a}{2}< x < L/2
The relevant force equilibrium equation is
-qx+\frac{qL}{2}+V=0 \Rightarrow V=qx-\frac{qL}{2}
The bending moment can be similarly found and is given by
\frac{qLx}{2}-\frac{qx^{2}}{2}-\frac{qL(L-a)}{4}

Thus the maxima of the above two moments are
\frac{q(L-a)^{2}}{8} and \frac{qL(L-a)}{4}

Both of which give a=L is when it is minimized. That isn't the answer at the back of the book!

I don't think we should take it as a uniform distribution.
 

Attachments

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gpavanb: It is a uniformly-distributed load. Is the answer in the back of the book by any chance a = 0.5858*L?
 
Spot On!
 
How did you get it?
 
If you move the supports too far apart, the midspan moment increases. If you move the supports too close together, the moment somewhere else increases. You want to figure out, at what value of "a" is the maximum moment in the beam as small as possible.
 
That was a vague hint. I got the problem in the mean time though. It was fairly straightforward.a=\frac{1}{(1+\frac{1}{\sqrt{2}})}L
 
Excellent work, gpavanb, which can be simplified to a = (2 - 2^0.5)*L, by multiplying the numerator and denominator of your answer by the complement, (2^0.5 - 1)/(2^0.5 - 1), which is 1, shown in line 4, below.

a = L/{1 + [1/(2^0.5)]}
= L/{[(2^0.5)/(2^0.5)] + [1/(2^0.5)]}
= (2^0.5)*L/(2^0.5 + 1)
= [(2^0.5)*L/(2^0.5 + 1)]*[(2^0.5 - 1)/(2^0.5 - 1)]
= (2^0.5)(2^0.5 - 1)*L/[(2^0.5 + 1)(2^0.5 - 1)]
= (2 - 2^0.5)*L/(2 + 2^0.5 - 2^0.5 - 1)
= (2 - 2^0.5)*L/(2 - 1)
= (2 - 2^0.5)*L
 

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