Mechanics: Moments of force in a rigid beam

Click For Summary
SUMMARY

The discussion focuses on calculating the forces at points A and B on a rigid beam subjected to multiple forces, specifically addressing the conditions for equilibrium. The moment equations derived indicate that the force at B, denoted as |FB|, is approximately -5.92 N, indicating it acts in the negative x-direction. The moment about point A is calculated using the cross product of position and force vectors, confirming that the beam remains in static equilibrium under the applied loads.

PREREQUISITES
  • Understanding of static equilibrium principles in mechanics
  • Familiarity with vector cross products and moment calculations
  • Knowledge of trigonometric functions for force resolution
  • Ability to interpret free-body diagrams for rigid bodies
NEXT STEPS
  • Study the application of the equilibrium equations in rigid body mechanics
  • Learn about the implications of negative forces in structural analysis
  • Explore advanced topics in moment of force calculations using MATLAB or Python
  • Investigate the effects of varying load conditions on beam stability
USEFUL FOR

Students and professionals in mechanical engineering, civil engineering, and physics who are involved in structural analysis and design of beams under various loading conditions.

JohanM
Messages
9
Reaction score
0

Homework Statement


Consider the rigid beam below, which is loaded by five forces shown. The forces at A and B act to keep the total force on the bar equal to zero and the sum of the moments about point A equal to zero.
a) Find the forces at A and B that satisfy the conditions stated above.
b) Find the sum of the moments about point B.
2ylp4k1.png

Homework Equations


\vec{M} = \vec{r} \times \vec{F}


The Attempt at a Solution


For part A, I figured that I can calculate the magnitude of FB by adding all of the moments about point A and separating |Fb|

Force C: creates 0 moment about point A since its direction is towards A (theta=180)

Force D:

\vec{r} = \left\langle 1000,-200 \right\rangle
\vec{F} = \langle 25 cos(20^\circ), 25 sin(20^\circ) \rangle

\vec{M}=\left| \begin{array}{ccc}\hat{i}&\hat{j}\\1000&-200 \\ 25 cos(20^\circ)&25 sin(20^\circ) \end{array} \right| \approx 3852.04 \hat{k}

Force B:

\vec{r} = \left\langle 1000,-650 \right\rangle
\vec{F} = \langle |\vec{F_{B}}|, 0 \rangle

\vec{M}=\left| \begin{array}{ccc}\hat{i}&\hat{j}\\1000&-650 \\ |\vec{F_{B}}|&0\end{array} \right| = 650 |\vec{F_{B}}| \hat{k}


\sum \vec{M}=O\hat{k}+3852.04...\hat{k}+650|\vec{F_{B}}|\hat{k}=0

|\vec{F_{B}}| \approx -5.92

Before I go any further I just want to make sure that I am approaching this correctly... Does it make sense that FB points in the negative x-direction?

Thanks,
Johan
 
Last edited:
Physics news on Phys.org
I think so, if the drawing is roughly to scale the 25kN force tends to rotate the beam counter clockwise therefore for the beam not to move the force at B must tend to rotate the beam clockwise and can only do so if the force at B acts to the left.
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
2K
Replies
12
Views
2K
  • · Replies 25 ·
Replies
25
Views
2K
Replies
3
Views
2K
Replies
3
Views
1K
Replies
1
Views
3K
  • · Replies 4 ·
Replies
4
Views
1K
Replies
2
Views
1K
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K