Tension in a pendulum (probably just me being stupid)

AI Thread Summary
The discussion revolves around analyzing the forces acting on a pendulum bob at a specific angle of 30 degrees from the horizontal. Participants clarify that the tension in the string is not solely the centripetal force but also includes a component of gravitational force acting at that angle. The tension must account for both the centripetal force required to keep the bob moving in a circular path and the gravitational force component acting perpendicular to the tension. The conversation emphasizes the importance of understanding vector components in physics, particularly in resolving forces acting on the pendulum. Ultimately, the participants arrive at a clearer understanding of how to calculate the tension and its relationship with gravitational forces at the given position.
downwithsocks
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Homework Statement


A pendulum consisting of a small heavy ball of mass m at the end of a string of length l is released from a horizontal position. When the ball is at point P, the string forms an angle 30 degrees with the horizontal.
a. Free body diagram (all set on that)
b. Determine the speed of the ball at P.
c. Determine the tension in the string when the ball is at P.
d. Determine the tangential acceleration of the ball at P.


Homework Equations


PEi + KEi = PEf + KEf
a = v^2 / r
Fc = mv^2 / r


The Attempt at a Solution


a. was just drawing a free body diagram, easy. For b., PE = KE, mglsin(30) = .5mv^2, v^2 = gl, v = sqrt(gl).

For c., is it just that the tension is equal to the centripetal force? In that case, Ft = Fc = mv^2/r = mv^2/l = mg? It just seems strange that it's the same as the force due to gravity at this point.
 
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Still need some help
 
Yeah, I am 100 per cent positive that the centripetal force is equal to the tension.

Concerning your remark, it is just a coincidence that Fc appears to be equal to mg, but note that this only happens when the angle is 30 degrees.
 
Centripetal force is not just tension, it also includes the relevant component of gravity at P.
 
aim1732 said:
Centripetal force is not just tension, it also includes the relevant component of gravity at P.

Ops yeah you're totally right, my bad. Those are the two forces acting in that very moment; both gravity component at that angle and F_c.
 
aim1732 said:
Centripetal force is not just tension, it also includes the relevant component of gravity at P.

Isn't gravity just acting straight down, and the centripetal force is the center-pointing force, the force pulling it in and causing it to "rotate" rather than just fall?
 
downwithsocks said:
Isn't gravity just acting straight down, and the centripetal force is the center-pointing force, the force pulling it in and causing it to "rotate" rather than just fall?

No, think of it this way: when the pendulum bob reaches the lowest point (90º from the horizontal) it is clear that gravity will play an important role to the tension at that point, so it is at point P.
 
Redsummers said:
No, think of it this way: when the pendulum bob reaches the lowest point (90º from the horizontal) it is clear that gravity will play an important role to the tension at that point, so it is at point P.

But isn't that because at that point ALL of the force due to gravity is canceled by the tension force (the centripetal force) whereas at point P it's only a component?
 
downwithsocks said:
But isn't that because at that point ALL of the force due to gravity is canceled by the tension force (the centripetal force) whereas at point P it's only a component?

No, If you draw the FBD you will see how the part of the gravitational force opposite to the tension must cancel the force of the tension in the string when the pendulum is at rest. But if we have an additional component, such as the centripetal force, the tension must be greater to provide sufficient stability, not letting the bob to break apart. That lead us to think that:

T = F_c + mg\cdot cos\theta
 
  • #10
Redsummers said:
No, If you draw the FBD you will see how the part of the gravitational force opposite to the tension must cancel the force of the tension in the string when the pendulum is at rest. But if we have an additional component, such as the centripetal force, the tension must be greater to provide sufficient stability, not letting the bob to break apart. That lead us to think that:

T = F_c + mg\cdot cos\theta

I just don't get what you mean by part of the gravitational force. The gravitational force is just straight down, no? The tension is the one with components isn't it? At rest, Fg = Ft obviously. Fc isn't an additional component is it? I thought it was CAUSED by an already present force...ie tension?
 
  • #11
Do you have a knowledge of vectors?
 
  • #12
Yes, but I tend to be kind of shaky with them except in basic addition and subtraction.
 
  • #13
Then you would have learned vector resolution too - breaking the vector into mutually perpendicular independent components? Try this with gravity with one component along the direction of motion of pendulum and one perpendicular to it. What do you get?
 
  • #14
A translated version of the tension FBD, so I set Ft equal to mgsin30? I understand that the math behind this works I guess, I just don't quite "see" it, I would have never thought to do that...anyways...

Fc = Ft - Fgsin30 = mv^2/r
mgl/l + .5mg = Ft
Ft = 3mg/2?
 
  • #15
Well, not equal, since mv^2/r isn't 0, but you get the idea...I'm a little tired.
 
  • #16
Relax. These things become clearer with time. But I think you have the answer. Just keep in mind that the second law is a vector law and valid along directions.
 
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