Calculating Deflection of Clamped Rods

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Discussion Overview

The discussion centers on calculating the deflection of a clamped rod when a force is applied at a certain point along its length. Participants explore the relationship between the applied force, the length of the rod, and the resulting deflection, delving into the mathematical formulation of the problem.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Conceptual clarification

Main Points Raised

  • One participant inquires about the formula for deflection in terms of the applied force and the position along the rod, suggesting a proportional relationship.
  • Another participant presents a mathematical expression for curvature and deflection, involving moment of inertia, elastic modulus, and applied force.
  • Questions arise regarding the definitions of moment of inertia (I_{xx} and I_{yy}) and the meaning of curvature, with a request for clarification on the variable z.
  • A correction is made regarding the moment of inertia notation, and further explanation is provided about the implications of asymmetrical sections in beam theory.
  • Participants discuss the relationship between the moment and the position along the rod, noting that the moment is maximum at the clamped end and decreases towards the point of force application.
  • Clarification is provided on the integration constants needed for solving the deflection equations based on initial conditions.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the mathematical concepts involved, and while some clarifications are made, no consensus is reached on the complete formula for deflection or the implications of different moment of inertia values.

Contextual Notes

Some assumptions about the geometry of the rod and the nature of the applied force remain unaddressed, and the discussion does not resolve the complexities of integrating the equations for deflection.

alexbib
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Here's a lil question:

If you have a rod of which an end is clamped to a table and you apply a force somewhere on the rod, what will the deflection be (in terms of difference in the height of the other end of the rod? For sure it will be proportional to the force and to some power of the length at which it is applied. What would be the complete formula, solved for deflection?
 
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For symmetrical beams with [tex]I_{xy} = 0[/tex], the curvature, [tex]v^{''}[/tex] is given by:

[tex]v^{''} = -{\frac{M_y}{EI_{xx}}}[/tex]

The deflection is thus:
[tex]v(L) = -\int_{0}^{L}\int_{0}^{L}{\frac{M_y}{EI_{xx}}}\cdot{dz}\cdot{dz}[/tex]

where L is the length of the rod, z is the axial length along the rod, F is the applied force, [tex]I_{xx}[/tex] is the moment of inertia about the horizontal axis, E is the elastic modulus of the material and [tex]M_y[/tex] for a point load at the end is [tex]M_y = {F}\cdot{(L - z)}[/tex].
 
Last edited:
Thx a lot for answering. [tex]I_{yy}[/tex] is the moment of inertia along the horizontal axis you say? Then what is the [tex]I_{xx}[/tex]found in the formula? The moment of inertia along another axis?

What do you mean by "For symmetrical beams with[tex]I_{xy} = 0[/tex]"?

Also, I'm not sure I fully understand what z is...
Sorry for being a newb lol.

Finally how is the curvature expressed. Is it a scalar quantity? What is its unit?

Thanks a lot,

Alex
 
Oops, I made a typo. [tex]I_{yy}[/tex] should be [tex]I_{xx}[/tex]. Sorry for the confusion caused (has now been edited). If you wanted to calculate [tex]u^{''}[/tex] which is the horizontal deflection due to an asymmetric section and/or horizontal load, then [tex]I_{yy}[/tex] is the moment of inertia about the vertical Y-axis.

Non-symmetrical section beams (e.g. L-section, as opposed to I or T-section) will have non-zero [tex]I_{xy}[/tex].

z is a variable, L is the total length (fixed). So z varies from 0 to L.

For the moment, don't worry about curvature. Use the integral equation to get the deflections you want. But since you asked, curvature has units m-1. It is a scalar quantity.
 
Ok, thanks. So [tex]M_y[/tex] would be the torque, attaining it's maximum value when z=0, when the force is applied derectly at the free end?
 
Actually, M was an abbreviation for "moment". But torque will do :smile:

Yup, the moment is maximum at the root of the rod where it is supported and goes to zero the closer you get to where you apply the load - the moment arm gets shorter as you go closer to the applied force.

BTW, you solve the integration constants based on the initial conditions. E.g. the slope at a rigid, unhinged support @ z=0 is 0, initial tip deflection @ z=L is 0, etc.
 
Alright, thanks for the help!
 

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