Pulley, two objects, frictionless plane; find acceleration and cable tension

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Homework Help Overview

The problem involves two boxes connected by a cable over a pulley, with one box hanging and the other on a frictionless inclined plane. The objective is to determine the acceleration of the boxes and the tension in the cable, given that both boxes are initially at rest.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the forces acting on each box, including gravity and cable tension. They explore the setup of equations based on Newton's second law and the components of forces acting parallel to the incline.

Discussion Status

Several participants have provided equations based on their understanding of the forces involved. There is ongoing exploration of the relationships between the variables, with some participants questioning the necessity of including the normal force in their calculations. Guidance has been offered regarding the setup of equations and the consideration of signs in the equations.

Contextual Notes

Participants are navigating through the complexity of the problem, with some expressing feelings of being overwhelmed by the number of equations and components involved. There is an emphasis on ensuring clarity in the setup of equations and the interpretation of forces.

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Homework Statement



A box of mass m1 is hanging from a cable of negligible mass, The cable rounds a pulley, where it is connected to a second box of mass m2 on a frictionless plane. The angle of the inclined plane is \theta as measured from the flat ground. Both boxes are initially at rest. Find the acceleration of the boxes and the tension in the cable.

ramp.jpg


Homework Equations



\overline{F}=m\overline{a}

\overline{n}+\overline{F}g=m\overline{a}

The Attempt at a Solution



Object A had mass m1 and object B has mass m2.

I know that gravity and the cable tension are both affecting object A, and the cable tension, gravity, and a normal force from the plane are affecting object B. Therefore, I have:

Object A: TA + FgA = m1a
Object B: TB +FgB + n = m2a

(where T, F, and a are all vectors)

I tried drawing free-body diagrams, and I just get lost drawing all of the equations...I know I need to make component vectors, but there is a lot to the problem, and I'm feeling a little overwhelmed.

Is this stuff correct so far? Thanks.
 
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What forces act on A? What forces act on B? (For B, all you care about are forces parallel to the incline.)
 
Gravity and the cable tension are the forces acting on A.

Gravity, the cable tension, and the normal force (the plane) act on force B.
 
emr13 said:
Gravity and the cable tension are the forces acting on A.
Good. Set up an equation with Newton's 2nd law.

Gravity, the cable tension, and the normal force (the plane) act on force B.
What are their components parallel to the incline? Set up an equation with Newton's 2nd law.

You'll get two equations with two unknowns. Careful with signs. (If one block goes up, the other must go down.)
 
Assuming A is heavier than B...

for A, I get m1g - T = m1a

The parallel forces for object B are Fgx and the T force... so I guess for B I get
T-m2gsin\theta = m2a.

Am I ignoring the normal force because the object doesn't move in that direction so it doesn't affect the acceleration?

If the above equations are right, then I can get the following equation for acceleration by making T= m2a + m2gsin(theta), and substituting it in for the T in object A's equation:

a=m1g-m2gsin(theta) over m1+m2

(sorry, formatting wouldn't work right for some reason)
 
emr13 said:
Assuming A is heavier than B...

for A, I get m1g - T = m1a

The parallel forces for object B are Fgx and the T force... so I guess for B I get
T-m2gsin\theta = m2a.
Excellent.

Am I ignoring the normal force because the object doesn't move in that direction so it doesn't affect the acceleration?
Right. You can consider the normal force if you like, but since the acceleration in that direction is zero, you'll just end up with N = m2gcosθ. You don't need it.

If the above equations are right, then I can get the following equation for acceleration by making T= m2a + m2gsin\theta, and substituting it in for the T in object A's equation:

a=m1g-m2gsin\theta
m1+m2
There are several ways to combine the two equations; that way is perfectly fine. I assume you meant to write:
a = (m1g - m2gsinθ)/(m1 + m2)

Another way is simply to add the two equations. That way the T from one cancels the -T from the other.
 
Yes, that it what I meant for the acceleration.

To find the cable tension, I substituted acceleration back into one of the equations and got:

T=m1g - m12g+m2gsinθ/m1+m2

that looks really gross...is it still correct?

And thank you so much for all your help.
 
emr13 said:
Yes, that it what I meant for the acceleration.

To find the cable tension, I substituted acceleration back into one of the equations and got:

T=m1g - m12g+m2gsinθ/m1+m2

that looks really gross...is it still correct?
It looks a bit off to me, but it may be formatting again. In any case, your approach is correct. If you do it over more carefully, you can simplify it a bit so it doesn't look quite so ugly. (Hint: Express everything over m1 + m2.)
 
What about this?

T=(m1m2g(1+sinθ)) / (m1+m2)
 
  • #10
emr13 said:
What about this?

T=(m1m2g(1+sinθ)) / (m1+m2)
Looks good! :approve:
 
  • #11
Awesome. Thank you so, so much.
 

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