Static equilibrium problem: Finding tension

In summary, when considering the diagonal component of a boom's weight as a reaction, it can be decomposed into horizontal and vertical components, and the vertical component can be used to calculate the weight of the boom. However, in order to find the correct solution, it is important to also decompose the weight counterpart of the reaction and use the torque method to solve the problem. It is recommended to double check all calculations and follow the guidelines given by your teachers for significant figures.
  • #1
archaic
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Homework Statement
The boom in the figure below weighs 3100 N and is attached to a frictionless pivot at its lower end. It is not uniform; the distance of its center of gravity from the pivot is 35.0 % of its length.
Relevant Equations
$$\sum\vec F=\vec0\\\sim\vec\tau=\vec0$$
yg.10.60.jpg
The diagonal component of the boom's weight is ##R=w\cos\frac{\pi}{6}=\frac{\sqrt 3}{2}w##, and, considering ##R## as a "reaction", we have ##R_x=R\cos\frac{\pi}{3}=\frac{\sqrt 3}{4}w## and ##R_y=R\sin\frac{\pi}{3}=\frac 34w##.
I will also have ##w_x=w\sin\frac{\pi}{6}\cos\frac{\pi}{6}=\frac{\sqrt 3}{4}w## and ##w_y=w\sin\frac{\pi}{6}\sin\frac{\pi}{6}=\frac 14w##.
$$\sum F_y=5000+w_y-R_y=5000+\frac 14w-\frac 34w=0\\w=10000\,N
\\\sum F_x=T-R_x-w_x=T-\frac{\sqrt3}{4}w-\frac{\sqrt 3}{4}w=0\\T=5000\sqrt3\,N$$
 
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  • #2
I messed up, probably because of ##R##. Let me consider the torques about the axis through the point of application of ##R## (in the image).
$$\sum\tau=0\Leftrightarrow lT\sin\frac{2\pi}{3}-5000l\sin\frac{5\pi}{6}-0.35\times5000l\sin\frac{5\pi}{6}=0\\T\sin\frac{2\pi}{3}-1.35\times5000\sin\frac{5\pi}{6}=0\\T=3375\,N$$
 
  • #3
At your picture the reaction R is directed along the boom Why? A priori you do not know its direction
 
  • #4
archaic said:
I messed up, probably because of ##R##. Let me consider the torques about the axis through the point of application of ##R## (in the image).
$$\sum\tau=0\Leftrightarrow lT\sin\frac{2\pi}{3}-5000l\sin\frac{5\pi}{6}-0.35\times5000l\sin\frac{5\pi}{6}=0\\T\sin\frac{2\pi}{3}-1.35\times5000\sin\frac{5\pi}{6}=0\\T=3375\,N$$
You seem to have used 5000N for both weights.

Wrt @wrobel 's point about the direction of R, consider moments about the top of the boom. If R acts along the boom then the weight of the boom is the only force with a torque about that axis.
 
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  • #5
wrobel said:
At your picture the reaction R is directed along the boom Why? A priori you do not know its direction
I didn't really consider reaction; I tried to come up with a force in the direction of ##T## so I decomposed the boom's weight in the way shown, but that makes a diagonal force that needs to be cancelled, hence me supposing ##R##.
The wrong step I did in summing up the forces was decomposing ##R## without decomposing its weight counterpart.
I need a vertical force to find the boom's weight, but I still don't see where it is.
...
 
  • #6
haruspex said:
You seem to have used 5000N for both weights.

Wrt @wrobel 's point about the direction of R, consider moments about the top of the boom. If R acts along the boom then the weight of the boom is the only force with a torque about that axis.
Hm, right. I can also find ##R_\perp=-\frac{13}{40l}w##. Don't see how that helps me, though.
 
  • #7
archaic said:
I need a vertical force to find the boom's weight, but I still don't see where it is.
...
The weight of the boom is given, 3100 N. And the force from the pivot does not act along the length of the boom: it has both vertical and horizontal components. No use to count with it. Solve the problem with the torque method.
 
  • #8
ehild said:
The weight of the boom is given, 3100 N. And the force from the pivot does not act along the length of the boom: it has both vertical and horizontal components. No use to count with it. Solve the problem with the torque method.
I forgot about it being given... Thank you.

$$\sum\tau=0\Leftrightarrow lT\sin\frac{\pi}{3}-5000l\sin\frac{\pi}{6}-0.35\times3100l\sin\frac{\pi}{6}=0\\T\sin\frac{\pi}{3}-6085\sin\frac{\pi}{6}=0\\T=\frac{6085}{\sqrt 3}\approx351.\times10^1\,N$$
I think this is good. Afraid of checking on the platform, though o_O . Anyone can confirm?
 
  • #9
archaic said:
I forgot about it being given... Thank you.

$$\sum\tau=0\Leftrightarrow lT\sin\frac{\pi}{3}-5000l\sin\frac{\pi}{6}-0.35\times3100l\sin\frac{\pi}{6}=0\\T\sin\frac{\pi}{3}-6085\sin\frac{\pi}{6}=0\\T=\frac{6085}{\sqrt 3}\approx351.\times10^1\,N$$
Correct, but why do you give it in 10 Newtons, instead of Newtons, , with two significant digits?
 
  • #10
ehild said:
Correct, but why do you give it in 10 Newtons, instead of Newtons, , with two significant digits?
Thank you. It is in three significant figures, since I'm taking ##35.0\%## as having that number of SFs.
 
  • #11
archaic said:
Thank you. It is in three significant figures, since I'm taking ##35.0\%## as having that number of SFs.
You are right! But even then, you can write it out as 3510 N , or 3.51x103 N
 
  • #12
ehild said:
You are right! But even then, you can write it out as 3510 N , or 3.51x103 N
Oh, the way I learned it from chemistry is that abc.x10n counts also as three significant figures.
 
  • #13
archaic said:
Oh, the way I learned it from chemistry is that abc.x10n counts also as three significant figures.
It is correct, only 101 looks strange. Do as it is required by your teachers
 
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  • #14
archaic said:
I didn't really consider reaction;
I see but this is not the reason to write wrong things
 
  • #15
archaic said:
Hm, right. I can also find ##R_\perp=-\frac{13}{40l}w##. Don't see how that helps me, though.
It doesn’t.. just illustrating that the reaction cannot be along the boom.
 
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  • #16
haruspex said:
It doesn’t.. just illustrating that the reaction cannot be along the boom.
Yes, I understood your point; "I can also..". Thank you!
 

1. What is static equilibrium?

Static equilibrium is a state in which all forces acting on an object are balanced, resulting in no net force and no acceleration.

2. How do you find tension in a static equilibrium problem?

To find tension in a static equilibrium problem, you need to use the equations of equilibrium. These include the sum of forces in the x-direction, the sum of forces in the y-direction, and the sum of moments about a point. By setting these equations equal to zero, you can solve for the tension.

3. What are the key principles to remember when solving a static equilibrium problem?

The key principles to remember are that the sum of forces and moments must equal zero for static equilibrium to be achieved, and that the direction of tension must be opposite to the direction of the force acting on the object.

4. What are some common mistakes to avoid when solving a static equilibrium problem?

Some common mistakes to avoid include not considering all forces and moments acting on the object, not setting up the equations of equilibrium correctly, and not paying attention to the direction of tension.

5. How can I check my answer to ensure it is correct in a static equilibrium problem?

You can check your answer by plugging it back into the equations of equilibrium and seeing if they still equal zero. Additionally, you can try solving the problem using a different method or approach to see if you get the same result.

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