Finding tension in tarzan swing

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Homework Help Overview

The problem involves determining the tension in a rope as Tarzan swings across a river on a vine, starting from rest. The discussion centers around the forces acting on Tarzan at the bottom of the swing and the application of energy conservation principles.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss drawing free body diagrams and applying Newton's second law to analyze the forces acting on Tarzan. There are attempts to use conservation of energy to relate initial and final states of motion. Some participants question the assumptions made regarding the forces, particularly the relationship between tension and weight.

Discussion Status

Multiple interpretations of the problem are being explored, with some participants providing corrections and clarifications regarding the application of energy conservation and the net forces acting on Tarzan. Guidance has been offered on considering the net force and the implications of circular motion.

Contextual Notes

There are discussions about the assumptions made regarding height references in energy equations and the necessity of accounting for acceleration due to circular motion. Some participants note the importance of recognizing that tension must exceed Tarzan's weight at the bottom of the swing.

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Tarzan (mass m) is trying to swing across a river on a long vine (length L) Assume that he starts from rest. Determine the tension in the rope at the bottom of the arc as a function of the angle theta, the arc angle between his starting point and ending point and whatever other variables necessary. Hints: Draw Free body diagrams for Tarzan when the rope is vertical.

I drew the free body diagram. It has tension pointing up and gravity pointing down. However, I don't know what to do.
 
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vu10758 said:
It has tension pointing up and gravity pointing down.
So far, so good. What does Newton's 2nd law tell you? Hint: What's the acceleration?
 
vu10758 said:
Tarzan (mass m) is trying to swing across a river on a long vine (length L) Assume that he starts from rest. Determine the tension in the rope at the bottom of the arc as a function of the angle theta, the arc angle between his starting point and ending point and whatever other variables necessary. Hints: Draw Free body diagrams for Tarzan when the rope is vertical.

I drew the free body diagram. It has tension pointing up and gravity pointing down. However, I don't know what to do.

You mean, tension pointing in the direction of the rope, right?
Use the fact that energy is conserved.

Btw, I'm sure I saw a few more 'Tarzan' problems in the last few days, so using the search option might be useful. :smile:
 
Using the law of conservation of energy

K_i + U_i + W_other = K_f + U_f

(1/2)m(v_i)^2 + mgLcos(theta) = (1/2)m(v_f)^2 + mgL

I let the height equals zero at the top

v_i is zero since it starts from rest

mgLcos(theta) = (1/2)m(v_f)^2 + mgL

the masses cancel

gLcos(theta) = (1/2)(v_f)^2 + gL
gLcos(theta) - gL = (1/2)(v_f)^2
2(gLcos(theta) - gL) = (v_f)^2

I know the the motion is circular so I know

F = m(v^2)/r

In this case, v is v_f and r is L

F = m(v^2)/L

I want to solve for the force of tension which is in the same direction as the centripetal force in this case

so

F = m(2gLcos(theta) - gL) / L
F = mL(2gcos(theta) - g)/L
F = m (2gcos(theta) - g)
F = mg (2cos(theta) - 1)

T = mg(2cos(theta) - 1)

Is this correct?
 
Just a few corrections:
vu10758 said:
Using the law of conservation of energy

K_i + U_i + W_other = K_f + U_f

(1/2)m(v_i)^2 + mgLcos(theta) = (1/2)m(v_f)^2 + mgL

I let the height equals zero at the top
If you let the height = 0 at the top (top of the vine, I presume), then the initial and final heights will be negative, since they are below the top:
(1/2)m(v_i)^2 - mgLcos(theta) = (1/2)m(v_f)^2 - mgL

The main thing is that Tarzan drops: his final height is lower than the initial.

v_i is zero since it starts from rest

mgLcos(theta) = (1/2)m(v_f)^2 + mgL

the masses cancel

gLcos(theta) = (1/2)(v_f)^2 + gL
gLcos(theta) - gL = (1/2)(v_f)^2
2(gLcos(theta) - gL) = (v_f)^2
Realize that the left hand side of this is negative--the correction above will fix that.


I know the the motion is circular so I know

F = m(v^2)/r

In this case, v is v_f and r is L

F = m(v^2)/L

I want to solve for the force of tension which is in the same direction as the centripetal force in this case

so

F = m(2gLcos(theta) - gL) / L
F = mL(2gcos(theta) - g)/L
F = m (2gcos(theta) - g)
F = mg (2cos(theta) - 1)

T = mg(2cos(theta) - 1)
Right approach, but realize that the tension is not the only force acting on Tarzan. (Use the net force in the above equations.)
 
how about making tarzan's weight equal and opposite to the tension in the rope?
 
billiards said:
how about making tarzan's weight equal and opposite to the tension in the rope?
That will not do. When Tarzan swings on the rope he is traveling on a circular path, which means he is accelerating. There must be a net force acting upwards when he is at the bottom of the swing. The tension must be greater than his weight.

Tarzan will feel like his weight is the tension in the rope, because he has to pull that hard to hold on. But what he feels is not his true weight.
 
Last edited:
billiards said:
how about making tarzan's weight equal and opposite to the tension in the rope?
Huh? You're supposed to solve for the tension, not just assume it to be something. (The tension doesn't equal Tarzan's weight--if it did, he'd be in equilibrium.)
 

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