Finding torque by integration of weight

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The discussion revolves around calculating torque by integrating the weight of a rod along its length. The initial attempt led to an incorrect expression for torque, prompting confusion about the integration process. Key insights included the need to define a linear density and correctly express the mass element in terms of the variable of integration. Clarification was provided on distinguishing between mass and mass-per-unit-length, which helped resolve the misunderstanding. Ultimately, the participant successfully completed the problem after applying these concepts.
Cooojan

Homework Statement



Hi. I ve got a problem, where I have to show torque by integrating the weight of the rod over the whole it's length.

Homework Equations


[/B]
Result, what I am suppose to get is:

## \tau_{rod} = \frac{mgb}2 ##

The Attempt at a Solution


[/B]
When I try to integrate, I am only getting:

## \tau_{rod} = \frac{mgb^2}2~~~~ ##

I'm sure I'm doing some silly mistake. But why can't I do this:

## \frac{d \tau_{rod}}{db} = mg~b~~~~~~⇒~~~~~~ \int \,d \tau_{rod}= mg \int b\,db~~~~~~⇒~~~~~~ \tau_{rod} = \frac{mgb^2}2~~~~##??

I only get the right answer by doing this:

## \frac{d \tau_{rod}b}{db} = mg~b~~~~~~⇒~~~~~~ \int \,d \tau_{rod}b= mg \int b\,db~~~~~~##

but I don't really understand why should I be doing anything like that, and this seems to me like completely wrong approach.

Im sorry if this seems very stupid :/
 

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If you have mass element ##dm## at distance ##x## from the the pivot, then the element contributes torque ##d\tau = dm~x##. The next thing you have to do is add up (integrate) all such elements over the length of the rod. Note that both ##dm## and ##x## are variables. You need to invent a linear density and cast ##dm## in terms of ##dx##.
 
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Cooojan said:
I'm sure I'm doing some silly mistake
b is the whole length of the rod. That is a bound on the integral, but not the variable of integration. Create a separate variable for that to avoid confusion.
In particular, you may find you are confusing mass with mass-per-unit-length.
 
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kuruman said:
If you have mass element ##dm## at distance ##x## from the the pivot, then the element contributes torque ##d\tau = dm~x##. The next thing you have to do is add up (integrate) all such elements over the length of the rod. Note that both ##dm## and ##x## are variables. You need to invent a linear density and cast ##dm## in terms of ##dx##.

I'm so cofused right now xDD
 
haruspex said:
b is the whole length of the rod. That is a bound on the integral, but not the variable of integration. Create a separate variable for that to avoid confusion.
In particular, you may find you are confusing mass with mass-per-unit-length.

True! Thank you guys. I feel like my head is about to explode )))))
 
Is that suppose to be an obvious solution to this? Because I feel so dumb right now xD
Are there any video tutorials on this kind of problems, because I can't find any simmilar ones. Even tho it should be a common kind of problem, I guess... I've really been sitting with this problem for too long now... And this is just a first part of the exercise ://///
 
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OK! I think I got this now... Please confirm if I am doing the right thing...

lin.density = ##\frac mb##

##dF=g \int_0^b \,dm##

## g \int_0^b \,dm = \frac {mg}{b} \int_0^b \,dx##

## g \int_0^b \,dm =g~dm= dF##

##g~dm~x = d\tau##

##d\tau=\frac{gm}{b}\int_ 0^b x\,dx##

##d\tau=\frac{gm}{b}[\frac{x^2}{2}]_0^b##

##\tau=\frac{gmb^2}{2b}=\frac{gmb}{2}##
 
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Cooojan said:
##F=g \int m'\,dm##
Imagine cutting up the rod into length elements ##dx##. If ##m'## is the linear density, then what is mass element ##dm##? If I give you length ##dx##, how much mass is in that length?

Also, we are not looking for a force, we are looking for a torque. Please reread post #2.
 
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kuruman said:
Imagine cutting up the rod into length elements ##dx##. If ##m'## is the linear density, then what is mass element ##dm##? If I give you length ##dx##, how much mass is in that length?

Also, we are not looking for a force, we are looking for a torque. Please reread post #2.

Since we don't deal with volume here, but only length, so lin.density should be ##=\frac mb##..
And as I understand, the mass per length ##dx## must be ##\frac{m}{dx}##.. And torque is just the the force time radius times ##sin\theta##,
so in this case, I thought I could multiply both sides with that particular ##x##, to get that particular ##\tau##

Im sorry if that's annoying...
 
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  • #10
Cooojan said:
Since we don't deal with volume here, but only length, so lin.density should be ## \frac {m}{b}##.
That is correct.
Cooojan said:
And as I understand, the mass per length ##dx## must be ##\frac{m}{dx}##
Incorrect. We already decided what the linear density is. Linear density is also known as mass per length. Units might be kg/m.

Perhaps you can clarify these ideas in your head if you answer this "real-life" situation: Given a salami of length b = 1.0 m and mass m = 2 kg, what is the mass, dm, of a slice of length dx = 3×10-3m?
 
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  • #11
It all suddenly became very clear, when u put it in salami terms...
Especially as I started getting seriously hungry, after breaking my head with this one.
That is one great salami, with fantastics mass of ##dm## per ##dx## unit length.
Thank you very much :)
 
  • #12
Cooojan said:
t all suddenly became very clear, when u put it in salami terms...
I'm glad. Can you finish the problem now?
 
  • #13
yes)) it's done :)
 

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