Man climbs rope ladder attached to balloon with acceleration relative to ladder

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Homework Help Overview

The problem involves a balloon, a rope ladder, and a man climbing the ladder, focusing on the accelerations of the center of mass of the system and the balloon. The context is rooted in dynamics and the application of Newton's laws, particularly regarding systems with multiple interacting masses.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of Newton's Second Law and the concept of center of mass. There is an exploration of how to relate the accelerations of the man, balloon, and the center of mass, with some participants questioning the clarity of the expressions provided in the problem.

Discussion Status

Some participants have offered hints and guidance regarding the relationship between the accelerations of the man and the balloon. There is an ongoing exploration of the expressions for acceleration, with participants clarifying their understanding of the system dynamics and the role of relative acceleration.

Contextual Notes

Participants note the ambiguity in the phrasing of questions and expressions, which has led to clarifications and deeper exploration of the problem's assumptions and definitions.

txy
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Homework Statement



There is a balloon of mass Mb. A rope ladder of negligible mass is hung from it. A man of mass m stands on the rope ladder. A buoyant force F acts on the balloon, causing the man-balloon-ladder system to accelerate upwards. Now, the man climbs up the rope ladder towards the balloon with an acceleration of am relative to the rope ladder. Find the acceleration relative to the ground of
  1. the center of mass of the man-balloon-ladder system;
  2. the balloon.
The acceleration due to gravity is g.


Homework Equations



I think it's just intelligent application of Newton's Second Law of motion and concepts of the center of mass.


The Attempt at a Solution



My book provided the answers, but did not state clearly which expression belongs to which acceleration.
There is a \frac{F - m a_{m}}{M_{b} + m} - g
and a \frac{F}{M_{b} + m} - g .

I think the second expression is for the acceleration of the center of mass. If I consider the whole system, I get
F - (M_{b} + m) g = (M_{b} + m) a_{c}, where a_{c} is the acceleration of the center of mass.

I'm not sure how to obtain the second acceleration expression.
 
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txy said:
I think the second expression is for the acceleration of the center of mass. If I consider the whole system, I get
F - (M_{b} + m) g = (M_{b} + m) a_{c}, where a_{c} is the acceleration of the center of mass.
Right.

I'm not sure how to obtain the second acceleration expression.
Hint: If the acceleration of the balloon with respect to the ground is "a", what's the acceleration of the man with respect to the ground? Use those results to express the acceleration of the center of mass in terms of "a" and am.
 
Oops I didn't phrase my question properly. I should have written "I'm not sure how to obtain the other acceleration expression." to avoid ambiguity. Thankfully you understood what I meant.

Why haven't I thought of finding the acceleration of man with respect to the ground before?

If a = acceleration of balloon with respect to ground,
then
acceleration of man with respect to ground = a + am .

So net force on center of mass = net force on whole system = vector sum of net forces on individual objects in the system.
So
(M_{b} + m) a_{c} = M_{b} a + m(a + a_{m}) = (M_{b} + m) a + m a_{m}
And so
a = a_{c} - (\frac{m}{M_{b} + m}) a_{m}
Then I sub in the expression for ac that I've obtained earlier and I'll get the expression given in the answer.

At first I wasn't sure about how the acceleration of center of mass is like the "weighted average" of the accelerations of the individual objects in the system. Now I understand. I hope my steps above are correct. Thanks a lot for pointing me in the right direction, with regards to the relative acceleration thing.
 
Last edited:
Perfectly correct.
 

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