Measuring Torque: Ideas & Solutions for Lab Projects

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To measure torque on a closed loop in a magnetic field without specialized devices, one suggestion is to use a spring with a known spring constant attached to the loop. By measuring the elongation of the spring, the torque can be estimated using the formula for potential energy. The discussion highlights the challenge of treating torque as constant during large angle rotations, emphasizing that torque may vary and complicate calculations. It is recommended to connect the spring directly to the loop to avoid energy loss through intermediaries. The spring's potential energy is considered the primary contributor to the loop's rotational energy in this setup.
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Hello everyone.
I'm working on a physics lab project and I've reached a barrier.
I need to measure the torque on a closed loop in a magetic field and I can't reach a way to do so. Of course, excluding all the torque measuring devices and such which I believe we don't have at the lab.

Any ideas on how to measure it?Thank you.
 
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I think you can use a spring with a known spring constant(which should be chosen in accordance with the range of torque being applied to the loop, you should have at least a very rough estimate of the amount of torque). Then you attach the loop to one end of the spring and fix the other end. Then you measure the elongation of the spring. Now you calculate \frac 1 2 k \delta x^2 which should be approximately equal to \int_{\theta_i}^{\theta_f} \tau d\theta. If the rotation angle is small, I think you can take the torque to be constant and that gives you the amount of torque.
 
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Interesting.
I can estimate what the torque should be by calculations so I believe that shouldn't be a problem. Just a question: how can I deal with the integral on the torque that you've given with large angles? Why can't I treat tge torque as a constant in both cases (small and large)?
 
Take the interval (a,b) where b=a+H. Now I want to calculate the integral \int_a^b f(x) dx(f being any function). Now I substitute x=a+\frac H 2 +h \Rightarrow dx=dh.
<br /> \int_{-\frac H 2}^{\frac H 2} f(a+\frac H 2+h) dh=\int_{-\frac H 2}^{\frac H 2} [\sum_{n=0}^\infty \frac{ f^{(n)}(a+\frac H 2)}{n!} h^n] dh=\int_{-\frac H 2}^{\frac H 2} [f(a+\frac H 2)+O(h)] dh=f(a+\frac H 2)H+O(H^3) \\ \Rightarrow f(a+\frac H 2)=\frac{1}{H} \int_a^b f(x)dx+O(H^2)<br />
So by taking \frac{1}{\theta_f-\theta_i}\int_{\theta_i}^{\theta_f} \tau d\theta, to be the torque at \theta=\frac{\theta_f+\theta_i}{2}, you have an error of the order (\theta_f-\theta_i)^2.
All of this is because the torque may not be constant during the rotation and how it changes is unknown to us. You may think its actually constant from some calculations but that only makes the approximation better because in reality, things aren't as clean as on the paper!
 
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Thanks. I'll make sure to go over it as when I get home (I'm on my phone).
Just a couple more questions if I may.
1. Did you mean to connect the spring directly to the loop or by a string or something?
2. Aren't there other things that contribute to the work in the system (except for the spring)?
 
MMS said:
1. Did you mean to connect the spring directly to the loop or by a string or something?
Connect them directly! Otherwise those things in between, will get some energy and that worsens the approximation.

MMS said:
2. Aren't there other things that contribute to the work in the system (except for the spring)?
I think the spring's potential energy is, to a good approximation, the only thing that gets the loop's rotational energy.
 
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