Newton's 3rd Law - Firefighter slides down a pole

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Homework Help Overview

The problem involves a firefighter sliding down a vertical pole, with a focus on the forces acting on both the firefighter and the pole. It relates to Newton's Third Law and the application of Newton's Second Law in a dynamics context.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the identification of forces acting on both the firefighter and the pole, including weight and frictional forces. There is an exploration of free-body diagrams to clarify the situation. Some participants question the application of Newton's Second Law and its relationship to Newton's Third Law.

Discussion Status

Participants are actively engaging with the problem, sharing insights about the forces involved and how they relate to each other. There is recognition of the need to understand action-reaction pairs and the role of friction in the interaction between the firefighter and the pole. Some guidance has been provided regarding the use of free-body diagrams and the application of the laws of motion.

Contextual Notes

There is mention of confusion regarding the language used to describe forces and the implications of Newton's laws. Participants are also considering the assumptions made about friction and its role in the problem.

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Homework Statement


A firefighter who weighs 712 N slides down a vertical pole with an acceleration 3 m/s2, directed downward. What are the (a) magnitude and (b) direction (up or down) of the vertical force on the firefighter from the pole and the (c) magnitude and (d) direction (up or down) of the vertical force on the pole from the firefighter?


Homework Equations


Newton's Second Law: Fnet = ma
Newton's Third Law: F1 + F2 = 0

The Attempt at a Solution



I know that the magnitude of the force on the pole from the firefighter will be the same as the force on the firefighter from the pole, but I'm having trouble implementing this to Newton's Second and Third Laws.

(a)

Let \textit{F}_{P} be the vertical force on the firefighter from the pole.
Let \textit{W}_{F} be the weight of the firefighter.
Let \textit{m}_{F} be the mass of the firefighter.

\textit{m}_{F} = \frac{W_F}{9.8}\textit{ = 72.6531 kg}

\sum\textit{F}_{y} = \textit{F}_{P}\textit{ - W}_{F}\textit{ = m}_{F}\textit{ a}_{y}\textit{ = }\textit{(72.6531 kg)(-3}\frac{m}{s^2}\textit{) + (712 N) = }\textit{494.0408 N}

This answer is correct according to the text.

(b) Up, to resist the net downward acceleration.

Also correct according to the text.

(c) Now this is where I don't know how to implement the equations properly and visualize the diagram for forces.

First, I tried identifying all the forces on the body of interest; the pole. Since in part (a) I identified all the forces acting on the firefighter, I chose to identify all the forces acting on the pole.

With this, I reasoned that \textit{W}{_F} acts on the pole in the downward direction, while the frictional force \textit{F}{_f} acts upward on the pole.

Since the net acceleration of the body (the pole) was 0, I put \sum\textit{F}{_y}\textit{ = F}{_f}\textit{ - W}{_F = 0}

This is wrong according to the text, but I also feel that I'm missing a key idea for this problem. I just don't know what :/
 
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steve , have you drawn free body diagram for the firefighter and the pole separately ?
it does helps to understand the situation. its better than imagining in your mind.

now remember in Newton's third law, the action and reaction always act on different bodies. also all forces in nature come in action-reaction pairs. so W_Fdoesn't act on the pole. that's wrong kind of language. W_F is force exerted by the Earth on the man and one should ask instantly , what is its reaction according to third law ? well, that is force exerted by the man on the earth. these two forces form action-reaction pair. now what you found in part a is force exerted on the man by the pole. so its reaction is the force exerted by the man on the pole and by Newton's third law , their magnitudes are equal... does it help
 
IssacNewton said:
steve , have you drawn free body diagram for the firefighter and the pole separately ?
it does helps to understand the situation. its better than imagining in your mind.

Yes I did also draw a free-body diagram to go along with this problem.

IssacNewton said:
now remember in Newton's third law, the action and reaction always act on different bodies. also all forces in nature come in action-reaction pairs. so W_Fdoesn't act on the pole. that's wrong kind of language. W_F is force exerted by the Earth on the man and one should ask instantly , what is its reaction according to third law ? well, that is force exerted by the man on the earth. these two forces form action-reaction pair. now what you found in part a is force exerted on the man by the pole. so its reaction is the force exerted by the man on the pole and by Newton's third law , their magnitudes are equal... does it help

Well I did already know the answer to part (c) because of Newton's Third Law but I didn't know if it had anything to do with the free-body diagram and the affecting forces.

I guess what I'm confused about is figuring how to apply Newton's Second Law in finding (c).

Or is it that you CAN'T just use Newton's Second Law to find (c)?
 
yes you can use second law, but the intermediate step would be Newton's third law anyway.
 
Wait. Does the firefighter also exert a frictional force on the pole?

I always assumed friction to be be made from only one body to another interacting body. Not both bodies.
 
the force of interaction between the man and the pole would be, yes , frictional force.
frictional force is just one type of force... since its interactive force, you need two bodies
to interact
 
IssacNewton said:
the force of interaction between the man and the pole would be, yes , frictional force.
frictional force is just one type of force... since its interactive force, you need two bodies
to interact

Ahh I see. Okay, so since there's a frictional force exerted by both the pole and firefighter, you'd have to reuse the force found in (a) to use Newton's Second Law in part (c) correct?
 
yes, correct... but we can directly use third law... since every force has its reaction paired with it (unless its pseudo force, which doesn't have reaction pair... that's why its called 'pseudo' force...), and in part a), you found one of these pairs, part c) is asking for the reaction associated with the force in part a)...
 
IssacNewton said:
yes, correct... but we can directly use third law... since every force has its reaction paired with it (unless its pseudo force, which doesn't have reaction pair... that's why its called 'pseudo' force...), and in part a), you found one of these pairs, part c) is asking for the reaction associated with the force in part a)...

Okay thanks much :]
 

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