Solving a Moment Equation: Understanding the Relationship with AD

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Homework Help Overview

The discussion revolves around understanding a moment equation involving vectors and their relationships in a mechanical system. The original poster presents a scenario with a dot product equation involving moments and questions how different vectors relate to the resultant moment about a point D.

Discussion Character

  • Conceptual clarification, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants explore the implications of the moment equations and the role of various vectors, particularly questioning the necessity of certain terms and the relationships between the forces and moments. There is a focus on understanding why specific vectors are used and how they contribute to the equilibrium condition.

Discussion Status

The conversation is ongoing, with participants seeking clarification on the relationships between the vectors involved in the moment equation. Some guidance has been offered regarding the equilibrium condition and the use of dot products to eliminate terms, but confusion remains about the interpretation of the vectors and their roles in the equation.

Contextual Notes

Participants express uncertainty about the assumptions regarding the directions of forces and moments, particularly concerning the resultant force at point A and its relationship to the vector rDA. There is also a discussion about the order of terms in cross products and their implications for the moment calculations.

goldfish9776
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Homework Statement


Inq this question, I am given that the u dot ( rb x tb + re x w) =0.
I knew that the rb x tb give a resultant moment pointed inside the book , which is parallel to AB... Then it cross with r AD, we will get the resultant moment.
But when re x w , I will gt the moment pointed in dx direction... How can it be related to AD?

Homework Equations

The Attempt at a Solution

 

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I don't understand your question.
##\vec{r_b}\times \vec{T_B}## is the moment of the tension about D, while ##\vec {r_E}\times\vec W## is the moment of W about D.
To these we could add the moment of the forces at A about D and end up with 0, for equilibrium. However, that moment is orthogonal to ##\vec u##, so if we take the dot product with ##\vec u## that moment disappears, leaving the given equation.
 
haruspex said:
I don't understand your question.
##\vec{r_b}\times \vec{T_B}## is the moment of the tension about D, while ##\vec {r_E}\times\vec W## is the moment of W about D.
To these we could add the moment of the forces at A about D and end up with 0, for equilibrium. However, that moment is orthogonal to ##\vec u##, so if we take the dot product with ##\vec u## that moment disappears, leaving the given equation.
what do u mean by we could add the moment of the forces at A about D here ? I'm confused...forces at A are not taken into calculation here ...
 
goldfish9776 said:
what do u mean by we could add the moment of the forces at A about D here ? I'm confused...forces at A are not taken into calculation here ...
you mean by doing u dot ( rb x tb + re x w) , it means the moment of the forces at A about D
 
goldfish9776 said:
what do u mean by we could add the moment of the forces at A about D here ? I'm confused...forces at A are not taken into calculation here ...
I mean that the full "sum of moments about D = 0" equation looks like :
moment of the tension about D + moment of W about D + moment of the forces at A about D = 0

If we then take the dot product of that with u then the last of those three terms vanishes, leaving:
u.(moment of the tension about D + moment of W about D) = 0
 
haruspex said:
I mean that the full "sum of moments about D = 0" equation looks like :
moment of the tension about D + moment of W about D + moment of the forces at A about D = 0

If we then take the dot product of that with u then the last of those three terms vanishes, leaving:
u.(moment of the tension about D + moment of W about D) = 0
why vector rDA is used here? why not rE ? this is weird becoz , moment of the tension about D + moment of W about D only pass thru rE ...
 
goldfish9776 said:
why vector rDA is used here? why not rE ? this is weird becoz , moment of the tension about D + moment of W about D only pass thru rE ...
I don't understand either of those points.
Where is rDA being used that you think is wrong? It would be used for the forces at A, yes, but rDA is in the same direction as u, so when we take the dot product of u with (rDA x forces at A) we get 0.
What do you mean about moments "passing through" rE? Forces pass through points, moments turn about points. All the moments being calculated here are about D.
 
haruspex said:
I mean that the full "sum of moments about D = 0" equation looks like :
moment of the tension about D + moment of W about D + moment of the forces at A about D = 0

If we then take the dot product of that with u then the last of those three terms vanishes, leaving:
u.(moment of the tension about D + moment of W about D) = 0
for them , why u is necessary ? aren't them have the vector rB and rE already ?
 
goldfish9776 said:
for them , why u is necessary ? aren't them have the vector rB and rE already ?
Taking the dot product with u is done to eliminate the forces at A from the equation.
 
  • #10
haruspex said:
Taking the dot product with u is done to eliminate the forces at A from the equation.
That's only for force a right? Why tb and w also need to multiply u ?
 
  • #11
goldfish9776 said:
That's only for force a right? Why tb and w also need to multiply u ?
We have an equation. We cannot multiply some terms of the equation by something and not other terms.
 
  • #12
haruspex said:
We have an equation. We cannot multiply some terms of the equation by something and not other terms.
i still don't understand . why shouldn't thtotal moment about D = rB x tB + rE x W + (resultant force at A) x rDA ?
 
  • #13
goldfish9776 said:
i still don't understand . why shouldn't thtotal moment about D = rB x tB + rE x W + (resultant force at A) x rDA ?
It does (except that you have the arguments of the last cross product in the wrong order; the distance vector should be on the left). But since the system is in equilibrium that total moment is zero. Write that as an equation. Now take the dot product of each side of that equation with u. What do you get?
 
  • #14
haruspex said:
It does (except that you have the arguments of the last cross product in the wrong order; the distance vector should be on the left). But since the system is in equilibrium that total moment is zero. Write that as an equation. Now take the dot product of each side of that equation with u. What do you get?
sorry , i mean D = rB x tB + rE x W + rDA x (resultant force at A) ... why shouldn't the equation look like this ?
 
  • #15
goldfish9776 said:
sorry , i mean D = rB x tB + rE x W + rDA x (resultant force at A) ... why shouldn't the equation look like this ?
I just answered that question. That equation is quite correct, but we need to move beyond it.
Step 1: since the system is in equilibrium, total moment about D is zero:
rB x tB + rE x W + rDA x (resultant force at A) = 0.
Step 2:
We want to eliminate the unknown (resultant force at A). We can do that by taking the dot product of both sides of the equation with u:
u.(rB x tB + rE x W + rDA x (resultant force at A)) = 0
u.rB x tB + u.rE x W + u.rDA x (resultant force at A) = u.0 = 0
Now, u.rDA x (resultant force at A) = 0
(can you see why?)
 
  • #16
haruspex said:
I just answered that question. That equation is quite correct, but we need to move beyond it.
Step 1: since the system is in equilibrium, total moment about D is zero:
rB x tB + rE x W + rDA x (resultant force at A) = 0.
Step 2:
We want to eliminate the unknown (resultant force at A). We can do that by taking the dot product of both sides of the equation with u:
u.(rB x tB + rE x W + rDA x (resultant force at A)) = 0
u.rB x tB + u.rE x W + u.rDA x (resultant force at A) = u.0 = 0
Now, u.rDA x (resultant force at A) = 0
(can you see why?)
we already know that the resultant force at A should be parallel to rDA , right , this will bring the rDA x (resultant force at A) = 0 ? So, why would we have to do one more step(step 2 ) ?
 
  • #17
goldfish9776 said:
we already know that the resultant force at A should be parallel to rDA , right
No. Why do you think that?
 
  • #18
haruspex said:
No. Why do you think that?
the resultant force of Az and Ay should be in perpendicular to Az and Ay(so, it's Ax) , right ? so it's Az . Az x rDA = o , since they are parallel to each other .
 
  • #19
goldfish9776 said:
the resultant force of Az and Ay should be in perpendicular to Az and Ay(so, it's Ax) , right ? so it's Az . Az x rDA = o , since they are parallel to each other .
Eh?!
The resultant of adding a force in the z direction and a force in the y direction will be somewhere in the YZ plane. It will certainly not be perpendicular to either. Even if it were perpendicular to both, as you claim, that would put it in the X direction, not the Z direction. And even if it were in either the X or Z direction that would not make it parallel to DA.
 
  • #20
haruspex said:
I just answered that question. That equation is quite correct, but we need to move beyond it.
Step 1: since the system is in equilibrium, total moment about D is zero:
rB x tB + rE x W + rDA x (resultant force at A) = 0.
Step 2:
We want to eliminate the unknown (resultant force at A). We can do that by taking the dot product of both sides of the equation with u:
u.(rB x tB + rE x W + rDA x (resultant force at A)) = 0
u.rB x tB + u.rE x W + u.rDA x (resultant force at A) = u.0 = 0
Now, u.rDA x (resultant force at A) = 0
(can you see why?)

yes , becoz u=rDA , they are parallel to each other
 
  • #21
haruspex said:
Eh?!
The resultant of adding a force in the z direction and a force in the y direction will be somewhere in the YZ plane. It will certainly not be perpendicular to either. Even if it were perpendicular to both, as you claim, that would put it in the X direction, not the Z direction. And even if it were in either the X or Z direction that would not make it parallel to DA.
I have mixed up the direction of torque and resultant force.
 
  • #22
haruspex said:
I mean that the full "sum of moments about D = 0" equation looks like :
moment of the tension about D + moment of W about D + moment of the forces at A about D = 0

If we then take the dot product of that with u then the last of those three terms vanishes, leaving:
u.(moment of the tension about D + moment of W about D) = 0
Can you explain why uDA. Moment of forces about D will =0 ?
 
  • #23
goldfish9776 said:
yes , becoz u=rDA , they are parallel to each other
Yes, because u and rDA are parallel.
 
  • #24
haruspex said:
I just answered that question. That equation is quite correct, but we need to move beyond it.
Step 1: since the system is in equilibrium, total moment about D is zero:
rB x tB + rE x W + rDA x (resultant force at A) = 0.
Step 2:
We want to eliminate the unknown (resultant force at A). We can do that by taking the dot product of both sides of the equation with u:
u.(rB x tB + rE x W + rDA x (resultant force at A)) = 0
u.rB x tB + u.rE x W + u.rDA x (resultant force at A) = u.0 = 0
Now, u.rDA x (resultant force at A) = 0
(can you see why?)
do u mean rDA x (resultant force at A) = 0 ? why it will become 0 ? rDA and resultant force at A are not parallel to each other ?
 
  • #25
goldfish9776 said:
do u mean rDA x (resultant force at A) = 0 ? why it will become 0 ? rDA and resultant force at A are not parallel to each other ?
No, that cross product is not zero. The dot product of u with it is zero.
If you have a triple product a.(b x c) and a is parallel to either b or c then the triple product is zero. The reason is clear: b x c is perpendicular to b and c; if a is parallel to b then a is perpendicular to b x c.
 
  • #26
haruspex said:
No, that cross product is not zero. The dot product of u with it is zero.
If you have a triple product a.(b x c) and a is parallel to either b or c then the triple product is zero. The reason is clear: b x c is perpendicular to b and c; if a is parallel to b then a is perpendicular to b x c.
since the rE x W and rb xTB are not perpendicular to u , so it,s not = 0 ?
how do u knw that a is parallel to b then a is perpendicular to b x c ??
 
  • #27
goldfish9776 said:
how do u knw that a is parallel to b then a is perpendicular to b x c ??
The cross product of two vectors (if nonzero) is always perpendicular to the two vectors.
If a is parallel to b then it must be perpendicular to b x c.
 
  • #28
haruspex said:
The cross product of two vectors (if nonzero) is always perpendicular to the two vectors.
If a is parallel to b then it must be perpendicular to b x c.
how do u knw that the rE x W and rb xTB are not perpendicular to u ?
 
  • #29
goldfish9776 said:
how do u knw that the rE x W and rb xTB are not perpendicular to u ?
Why would that matter? Nothing in the algebra assumes those are not zero.
 
  • #30
haruspex said:
Why would that matter? Nothing in the algebra assumes those are not zero.
because when rE x W and rb xTB are not perpendicular to u , then i can't say that u . (rE x W) and u .(rb xTB ) = 0
 

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