Confused on whether this counts as an external torque

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SUMMARY

The discussion centers on the application of torque and angular momentum in a physics problem involving a mass m and a radial force from a string. The formula a = v^2/r is highlighted, along with the relationship Mg = mv^2/r, indicating two unknowns: velocity (v) and radius (r). Participants clarify that the tension in the string does not create torque about the center of rotation due to the radial nature of the force, leading to the conclusion that the conservation of angular momentum holds true in this scenario despite the presence of external torque.

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laser
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Homework Statement
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Relevant Equations
Tension in this case is Mg, which is equal to centripetal force, mv^2/r
1701686067504.png

For part (d), there is the formula a = v^2/r I can use. Note that Mg = mv^2/r, we have two unknowns, v and r. I can solve this if conservation of angular momentum is true, i.e. mvr = constant. I am not convinced I can use this however, because is increasing M torque?

My idea is that it is an external torque, because by the right hand rule, torque points along the axis which M is acting on.

How can I solve this problem?

(This problem comes from a past exam paper, which the physics department will not provide help with)
 
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laser said:
because is increasing M torque?
What torque? The force from the string on the mass m is radial.
 
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Damn, you're right. I kind of forgot their configuration. Thanks!
 
Orodruin said:
What torque? The force from the string on the mass m is radial.
One more doubt: The conservation of angular momentum is valid if there are no external torques. Even though this torque is not interfering with the motion of the object rotating in a circle, there is still an external torque being applied to the system (radially). Why can we still say the conservation of angular momentum is constant? Is it only constant in the plane that m rotates in?
 
laser said:
Even though this torque is not interfering with the motion of the object rotating in a circle, there is still an external torque being applied to the system (radially).
There is no torque
.
Consider a force F and some point P (which can be anywhere).

Let d be the perpendicular (shortest) distance between F's line-of-action and P.

The magnitude of the torque (about P) is Fd.

But if P lies on the force's line-of-action, then d=0. In this case, the torque about P is Fd = Fx0 = 0.

In the current question, the tension acting on the mass is radial - it acts through the centre of rotation: so d=0 making the torque (about the centre of rotation) zero.

Consider trying to open a screw-top cap on bottle using a radial force! There is zero torque about the centre of rotation and the cap doesn't turn. You need a tangential force (or component of force) to create a torque.
 
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