Finding forces in members of frames

In summary, the conversation is about solving a problem involving finding reaction forces in member AFGH using three equilibrium equations. The problem is complicated as there are always three unknowns no matter which member is analyzed, making it unsolvable. The conversation also discusses the use of free body diagrams and the assumption that member GC is a two-force member. The expert suggests considering the horizontal forces on beam AE and using moments to relate the horizontal forces at point A and G to find the unknown force at CG. The conversation ends with the suggestion of using systems of equations to solve the problem.
  • #1
chunchunmaru

Homework Statement


I'm trying to solve for this problem below.How would you be able to get the force in member ID and GC? Find the reaction forces in member AFGH

Homework Equations


∑M = 0
∑[F][/y] = 0
∑[F][/x] = 0[/B]

The Attempt at a Solution


I dismembered all of its parts but no matter where member I analyze into there are always three unknowns which makes it impossible to solve using the three equilibrium equations. I got through the part where member GC is a two force member and the reaction forces at pin B and pin D are just equal to the tensions in the pulley, but after that no luck. Any ideas on how should I solve it? I know after solving the forces in the ABCDE member I would be able to get the reactions at the AFGH member but I seem to be lost in the problem.
 

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  • #2
chunchunmaru said:
no matter where member I analyze into there are always three unknowns which makes it impossible to solve
Please post an attempt, as per forum rules.
 
  • #3
My attempts are the free body diagrams. As you can see, the components have subscripts "x" and "y" to indicate their respective axial components.

The FBDs are labeled accordingly, pulley B for the pulley at point B , pulley E for the pulley at point E. I got the components of these first, which would just be the tension at the pulley. Which is 490N.

However,after solving the components at the pulleys I don't know where to go next because every member has atleast 3 unknowns which makes it unsolvable with just the three equations of equilibrium.

I tried solving the components at "FBD 4". For example, I tried getting the moment at point C but I would end up with the components Ay and Dy unknowns, therefore making it impossible to solve for the Ay and Dy components. I tried solving for the summation of X components but Ax, Dx, and the x component of force Fgc are unknowns and the same happens when solving for the summation of y components.

At FBD 2, I assumed that the member GC is a twi-force member to be able to simplify it's components but I cannot solve for its components without the values at FBD 4. At FBD 3, I tried solving it but without the value of the reactions at D I cannot solve for the reactions at point I.

Meanwhile, I created an FBD for the pins. At pin B, I assumed the the member AB exerts a vertical and horizontal component at pin B and member BC to exert a horizontal component as well. At pin E, I also assumed the member DE exerts a horizontal and vertical component at pin E.

I think after solving for the values at other FBDs. The FBD1, would be the last to be solved because without the value of the reactions at point A and G, the reactions at point H would not be solvable.
 

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  • #4
I think you are making it unnecessarily complicated by breaking it into too many pieces.
You should be able to write down immediately the x and y components of the forces the pulleys exert on the points B, E, and the force the rope exerts at point F.
A question worth asking yourself is what would happen if the angle bracket connecting C and G were removed. Would the system collapse?
 
  • #5
A question worth asking yourself is what would happen if the angle bracket connecting C and G were removed. Would the system collapse?[/QUOTE]

Would it mean that member CG is a zero force member?
 
  • #6
chunchunmaru said:
A question worth asking yourself is what would happen if the angle bracket connecting C and G were removed. Would the system collapse?

Would it mean that member CG is a zero force member?
Perhaps... what do you think CG is doing in the structure? Why is it there?
 
  • #7
Hmm I have an answer key to this problem but it states that there is a forc on the member GC.
 

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  • #8
chunchunmaru said:
Hmm I have an answer key to this problem but it states that there is a forc on the member GC.
Yes, I didn't say there was not a force. I just asked you to think about how the system would move if you took it away.
Never mind, let's try something else...

What can you say about the horizontal forces on beam AE?
 
  • #9
I think the horizontal forces on caused by the pins would just cancel out. Thus the remaining horizontal forces would be on point A,C and D. Is it correct?
 
  • #10
chunchunmaru said:
I think the horizontal forces on caused by the pins would just cancel out. Thus the remaining horizontal forces would be on point A,C and D. Is it correct?
Right. So you have an unknown force CG exerts at G, and an equal and opposite one it exerts at C. Consider its horizontal component.
What can you say about its relationship to the force the beam AE exerts on beam AH?
Take moments on AH about H. What do you find?
 
  • #11
If I would sum the moments at point H, the horizontal component of A and G would be the two unknowns. Would I be able to relate this equation to the sum of horizontal forces at the other member AE is it possible?
 
  • #12
chunchunmaru said:
the horizontal component of A and G would be the two unknowns.
Considering my post #10, can you get that down to one unknown?
 
  • #13
Is it possible?

Member A-H
*Considering that counter-clockwise moments are positive.
ΣM = 0
0 = (-Ax)(0.21)+(FGCx)(0.7)+(450)(0.8)
-360 = -0.21Ax+0.7FGCx

Member A-E
∑Fx = 0
0 = -Ax+FGCx+Dx
*I didn't include the horizontal components at B and E since they would just cancel.
I think it would be possible to make it at a one unknown if the horizontal component at D is not included, what should I do next? I was thinking of solving it in systems of equations but I noticed that the component at D is present so now I wouldn't be able to use systems of equations.
 
  • #14
chunchunmaru said:
Is it possible?

Member A-H
*Considering that counter-clockwise moments are positive.
ΣM = 0
0 = (-Ax)(0.21)+(FGCx)(0.7)+(450)(0.8)
-360 = -0.21Ax+0.7FGCx

Member A-E
∑Fx = 0
0 = -Ax+FGCx+Dx
*I didn't include the horizontal components at B and E since they would just cancel.
I think it would be possible to make it at a one unknown if the horizontal component at D is not included, what should I do next? I was thinking of solving it in systems of equations but I noticed that the component at D is present so now I wouldn't be able to use systems of equations.

I tried to solve it with neglecting the D component and I got the wrong answer for the other component reactions. It seems that D has indeed a horizontal component, how would I be able to get the value? I imagine taking moments but I think it would not be correct.
 
  • #15
chunchunmaru said:
0 = (-Ax)(0.21)+(FGCx)(0.7)+(450)(0.8)
A few mistakes there.
Check the 0.21, the 450 and the 0.8.
chunchunmaru said:
I tried to solve it with neglecting the D component
Since DI is freely jointed at I, there can be no horizontal force at D.
 
  • #16
haruspex said:
A few mistakes there. Check the 0.21, the 450 and the 0.8.

Ah yes, I got it now.

haruspex said:
Since DI is freely jointed at I, there can be no horizontal force at D.

How is it possible for D to not have a horizontal component? I was thinking that D should have a horizontal one since it's support at point I may have a horizontal component?

I just tried it and I'm so happy it's correct.I noticed that the way we have approached this problem was a littble bit of short because with the way my professor taught me, we were always asked to first dismember all the parts first even before analyzing the whole structure itself in able to be able to do the structural analysis. May I ask is the method that we have just did applicable to any frames and trusses problem?
 
  • #17
chunchunmaru said:
How is it possible for D to not have a horizontal component?
It is freely jointed at I. If there were a horizontal component at D that would have a moment about I that is not balanced by any other force or torque.
Also, since it is freely jointed at D, there is no torque exerted by DI on the horizontal beam.
chunchunmaru said:
we were always asked to first dismember all the parts first
Yes, that is a good methodical approach, but it can be overkill.
In the present problem I would resolve it into the main components (the four structural beams) and see what I can write down about them. It is reasonably obvious how the rope, pulleys and pins mediate the forces between them. If that is not obvious, then I would analyse those smaller components.
 
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  • #18
haruspex said:
It is freely jointed at I. If there were a horizontal component at D that would have a moment about I that is not balanced by any other force or torque.
Also, since it is freely jointed at D, there is no torque exerted by DI on the horizontal beam.
So a proof of it not having a component is if I sum moments at point I at member DI,
ΣM = 0
0 = Dx(2.1)
Dx=0
Is it safe to analyze zero force members like this?

haruspex said:
Yes, that is a good methodical approach, but it can be overkill.
In the present problem I would resolve it into the main components (the four structural beams) and see what I can write down about them. It is reasonably obvious how the rope, pulleys and pins mediate the forces between them. If that is not obvious, then I would analyse those smaller components.

So for this problem the four FBDs I drew were enough? even without the pulley and pin FBDs?
 
  • #19
Thanks your approach kind off gave me a new way to solve frames. Hoping I would be able to use it for solving
 
  • #20
chunchunmaru said:
ΣM = 0
0 = Dx(2.1)
Dx=0
Is it safe to analyze zero force members like this?
Yes.
chunchunmaru said:
So for this problem the four FBDs I drew were enough? even without the pulley and pin FBDs?
As long as you are comfortable with that. If you are not sure what forces those will exert on the joints then by all means do separate diagrams for them.
For pulleys, I find the clearest approach is to regard all parts of the rope that are in contact with the pulley wheel as part of the pulley.
 
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FAQ: Finding forces in members of frames

What is a frame?

A frame is a structural system made up of interconnected members, such as beams and columns, that work together to support loads and resist forces.

What are external and internal forces in frames?

External forces are the loads acting on a frame from outside sources, such as the weight of a building or wind. Internal forces are the forces that develop within the frame members in response to external loads.

How do you find forces in members of frames?

To find forces in members of frames, you must first draw a free body diagram of the frame and identify all external and internal forces. Then, apply the equations of equilibrium to solve for the unknown forces in each member.

What are the different types of forces that can act on a frame?

The different types of forces that can act on a frame include tension, compression, shear, and bending. Tension and compression forces act along the length of a member, shear forces act perpendicular to the length of a member, and bending forces cause a member to bend or deform.

How can you ensure a frame is structurally stable?

To ensure a frame is structurally stable, you must make sure that all external forces are balanced and that the frame members are strong enough to resist the internal forces. This can be achieved by properly designing and constructing the frame according to engineering principles and standards.

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