Two forces held by pulley's on an inclined plane.

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Homework Help Overview

The problem involves two masses connected by a pulley on an inclined plane, with angles of 60 degrees and 20 degrees. The left-hand mass is given as 2.1 kg, and the goal is to determine the right-hand mass needed for the system to accelerate downslope at 0.64 m/s².

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the equations of motion for both masses and the role of tension in the system. There are attempts to isolate the right-hand mass, with some participants expressing frustration over algebraic manipulation. Questions arise regarding the assumptions about the pulley and the setup of the problem.

Discussion Status

Participants are actively engaging with the problem, sharing their attempts and questioning each other's reasoning. Some guidance has been offered regarding the algebraic steps needed to isolate the right-hand mass, though there is no consensus on the correct approach yet.

Contextual Notes

There is an ongoing discussion about the assumptions made regarding the pulley and the forces acting on the system. Participants are also addressing potential errors in their calculations and the implications of negative values in their results.

NemoMnemosyne
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Homework Statement



Suppose the angles on an inclined plane are 60*(left-hand side) and 20* (right-hand side). If the left-hand mass is 2.1 kg, what should the right-hand mass be so that it accelerates downslope at 0.64 m/s/s?

Homework Equations



F=ma

The Attempt at a Solution



a=.64
Ml (left-side) = 2.1kg
Mr (right-side) = ?
θl = 60*
θr = 20*

Ml -> F = Mla -> T - Mlgsinθl = Mla
Mr -> F = Mra -> Mrgsinθr - T = Mra

I understand that since acceleration is the same then Mla + Mra = (Ml + Mr)a

I also know that T = Mla + Mlgsinθl

So I tried to sub in for T -> Mrgsinθr - Mla + Mlgsinθl = Mra but this doesn't make any sense to me. No matter how I look at it I can't seem to isolate Mr by itself. This is causing me considerable frustration.
 
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I'm assuming the pulley is negligible? I would suggest drawing a picture and displaying the forces acting on the system.
 
Liquidxlax said:
I'm assuming the pulley is negligible? I would suggest drawing a picture and displaying the forces acting on the system.

Yes the pulley is negligible, as is the rope. I drew a picture and free-body diagram and labeled all the forces accordingly.

I think my issue here is figuring out how to do the algebra correctly to end up with the Mass of the right-hand side by itself so I can solve the problem. Anywhere in my steps that you see an error?
 
Have you tried:
Mrgsinθr - Mla + Mlgsinθl = Mra
\large M_r = \frac{M_l(a+g\sin{\theta_l})}{g\sin{\theta_r}+a}?
 
danielakkerma said:
Have you tried:

\large M_r = \frac{M_l(a+g\sin{\theta_l})}{g\sin{\theta_r}+a}?

You think I could get you to run through how you managed to get that? I still just can't see how you managed to get Mr by itself. I can tell there's some factoring in there somewhere but I guess I'm just not making the right calculations.
 
It's very simple, and there's no secret to it.
It always helps to arrange the needed elements on one side, and the rest, the known ones on the other.
So we would get,
<br /> \LARGE<br /> M_rg\sin{\theta_r} + M_ra = M_lgsin{\theta_l}+M_la<br />
All that's left is to extract M_r by removing it as a common factor/coefficient, and dividng by the remainder, namely, g sin(theta_r)+a.
Hope that's clear enough,
Daniel
P.S
I might help if you pointed exactly which step you don't follow...
 
danielakkerma said:
It's very simple, and there's no secret to it.
It always helps to arrange the needed elements on one side, and the rest, the known ones on the other.
So we would get,
<br /> \LARGE<br /> M_rg\sin{\theta_r} + M_ra = M_lgsin{\theta_l}+M_la<br />
All that's left is to extract M_r by removing it as a common factor/coefficient, and dividng by the remainder, namely, g sin(theta_r)+a.
Hope that's clear enough,
Daniel
P.S
I might help if you pointed exactly which step you don't follow...

I seem to be having trouble figuring out how you get a positives on both sides of the equation above. I managed to get there but I had a negative the left side of it, (right-hand side of the problem).

I'll write down all my steps...

<br /> \LARGE<br /> T - M_lgsin{\theta_l} = M_la<br />
<br /> \LARGE<br /> M_rgsin{\theta_r} - T = M_ra<br />
Adding both equations, the tensions cancel leaving...

<br /> \LARGE<br /> M_rgsin{\theta_r} - M_lgsin{\theta_l} = M_la + M_ra<br />

I subtracted the M_ra from the right-side of the equation, and added M_lgsin(theta_l) to get

<br /> \LARGE<br /> M_rgsin{\theta_r} - M_ra = M_lgsin{\theta_l} + M_la<br />

I just don't see how you ended up with the equation you posted, with positives on both sides.
 
Hi,
You're positively right! there's a minus there, but that shouldn't matter. Anyway, can you extract m_r now?
 
danielakkerma said:
Hi,
You're positively right! there's a minus there, but that shouldn't matter. Anyway, can you extract m_r now?

Yes I can. I ended up getting...

<br /> \LARGE<br /> M_r(gsin{\theta_r} - a) = M_lgsin{\theta_l} + M_la<br />

If divide by the
<br /> gsin{\theta_r} - a<br />

the answer still comes out negative for me. Am I right in thinking that if I reversed the order of...
<br /> gsin{\theta_r} - a<br />

it would make it positive like so...

<br /> a + gsin{\theta_r}<br />
 
  • #10
It can't possibly be negative!
With your given data, g*sin(theta_r) is larger(much!) than a.
Check your arithmatics...
 

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