- 42,775
- 10,484
Yes.dahoa said:You are saying R1 and R2, R2 and R3 are separate problems?
Yes.dahoa said:You are saying R1 and R2, R2 and R3 are separate problems?
I think its because, there will be more unknowns than the number of static equilibrium equations that can be applied.If both ends of a beam are fixed, you have to find two reaction meoments(one at each end) and two reaction vertical forces(one at each end).But you have only two static equilibrium equations.(summation of vertical forces=0 and summation of moment about any point=0).dahoa said:If the ends are fully moment connected (100% fixed).. why can't you determine the reaction forces and moments?
No, there's more to it than that.Mohankpvk said:I think its because, there will be more unknowns than the number of static equilibrium equations that can be applied.If both ends of a beam are fixed, you have to find two reaction meoments(one at each end) and two reaction vertical forces(one at each end).But you have only two static equilibrium equations.(summation of vertical forces=0 and summation of moment about any point=0).
Try applying the procedure I posted at #22 and #34.dahoa said:anyway.. I have been trying to derive these for a month but couldn't... in the following:
View attachment 228381
How is R1=R3=5P/16 and R2= 11P/8 exactly derived?
Yes.I agree with the point that they are not totally indeterminate.haruspex said:No, there's more to it than that.
Consider the simplest case: no load applied, weightless beam, ends at same height and fixed horizontally.
If this is statically indeterminate then there must be a nontrivial solution, i.e., one in which the end supports apply equal and opposite nonzero vertical forces. Correspondingly there will be nonzero torques so that equilibrium is maintained.
For a theoretical rigid beam that would all be possible, but this field of study considers beams to be flexible. The beam undergoes a deflection y=y(x).
Suppose the supports give a force F up at the left and down at the right, and anticlockwise torques T, T' respectively.
Taking moments at offset x from the left:
ky"=-T+Fx
Integrating, and using y(0)=0:
ky'=-Tx+Fx2/2
Integrating, and using y'(0)=0:
ky=-Tx2/2+Fx3/6
Now we use the same constraints at the right hand end (x=L):
0=-TL+FL2/2
0=-TL2/2+FL3/6
When the smoke clears:
T=F=0.
So it is not indeterminate after all.
(I was wrong to agree to that earlier without checking.)
I'd put it a little differently: you have to use the information about the slopes at the ends.Mohankpvk said:Yes.I agree with the point that they are not totally indeterminate.
But I think they are called statically indeterminate because we can't find the reactions just by using the static equilibrium equations.
We have to exploit the cocept of deflection(deflection at the ends=0)to solve for the reactions.
I can't see it, but maybe you can. For me, it's easier to just solve the doggone thing already.dahoa said:My thoughts before was that fixing the end can redistribute the moments and loads. But can't one make a general statement without computng for anything that fixing the ends versus just pinned can always produce more reactions for the fixed ends?
My reasoning is that making something stiffer can attract more load.
It is easy to see that this cannot be a general rule.dahoa said:fixing the 2 ends lessen the moments at the center a bit..
haruspex said:It is easy to see that this cannot be a general rule.
Suppose you have some arrangement where the ends are only pinned. There will be some gradient to the beam at each end. Now fix the ends at that gradient. Clearly nothing changes: no torque at the ends and no change to the verical reactions or moments anywhere.
Now consider fixing the gradients a little differently, up or down. If going one way increases a moment or reaction at some point then going the other way probably reduces it.
However, it may that what you say is the usual consequence for the typical arrangement: ends fixed horizontally with downward loads along the beam.
Yes, of course, but the point of my previous post is that :dahoa said:But fixing the ends can change the deflections.
haruspex said:Yes, of course, but the point of my previous post is that :
a) it does not necessarily change anything
b) depending on how the ends are fixed, the deflections, moments etc. can be increased or decreased.
Consider a beam with a central weight, pinned at each end. Now changed the left-hand support to fixed at the horizontal. That will shift some of the vertical reaction from the right-hand support to the left-hand.dahoa said:If we have a single beam with 2 pinned or fixed supports.. it won't change the reactions
haruspex said:Consider a beam with a central weight, pinned at each end. Now changed the left-hand support to fixed at the horizontal. That will shift some of the vertical reaction from the right-hand support to the left-hand.
I have shown you how to compute them.dahoa said:we just don't know how to compute the increase in the reactions
haruspex said:I have shown you how to compute them.
But you seem to be looking for a simple rule of thumb, and that may or may not exist.
You mean "statically indeterminate", which means that you cannot deduce the reactions from the usual equilibrium equations alone, i.e. an external view of the torques and forces on the beam as a whole.dahoa said:statistically indeterminate.. meaning uncomputable
haruspex said:You mean "statically indeterminate", which means that you cannot deduce the reactions from the usual equilibrium equations alone, i.e. an external view of the torques and forces on the beam as a whole.
But you can often solve these questions when you take into account the known constraints on the shape of the beam. E.g. if it is a fixed support at one end then the torque is an extra unknown, but if you know it is fixing the slope there at a certain angle then that gives you an extra equation too.
As I already explained, if there is a fixed support part the way along the beam you can treat it as two separate problems.dahoa said:if you can compute all the reactions for 3 fixed supports beam
Not sure how they would be using "torsion". In everyday English it can mean either torque (i.e. an applied twisting load) or the twist that results from it.dahoa said:"Torque" and "Slope" were not mentioned.. only Torsion and Deflections
haruspex said:Not sure how they would be using "torsion". In everyday English it can mean either torque (i.e. an applied twisting load) or the twist that results from it.
If the deflection is given by some function y=y(x) then the slope at some point is the first derivative, y'(x), and the twist the second derivative, y"(x).
If the upward force density on the beam is f(x) and the anticlockwise torque density t(x) [could use the Dirac delta function to represent point loads and torques] then the basic equation is:
ky"(x)=∫z=0z=x(f(z)(x-z)-t(z)).dz
The reasoning is this: if at the beam element dz the locally applied force is f(z) then that is distance (x-z) from the point x, so exerts a clockwise torque f(z).(x-z)dz about the point x, and this leads to an upward curvature in y. Similarly for the applied torque t(z).dz, but in that case the effect at x is just t(z).dz, not depending on the distance x-z.
No. The moment is the cause, and only depends on the load distribution. The deflection is the result, and depends on both the load and the properties of the beam.dahoa said:. Is deflection just like the concept of moments where it can occur without any material properties
haruspex said:No. The moment is the cause, and only depends on the load distribution. The deflection is the result, and depends on both the load and the properties of the beam.
Ok, I can see why you are getting confused.dahoa said:Well in the following derivations of 11P/8 and 5P/16 in the 3 supports pinned case.. there is no material properties of the beam so how did he derive using the deflection that has no material properties?
haruspex said:Ok, I can see why you are getting confused.
If all the forces and moments acting on the beam are known then the deflection depends on those and the properties of the beam.
In these problems, only some of the applied forces are known initially. The remaining reactions will depend on how the beam reacts to those.
If the beam is known to be uniform then we can figure out the shape of the deflection without knowing its extent. Halving the EI will simply double all the deflections. This allows us to calculate all the reactions without knowing the extent of the deflection.