Acceleration for Masses on a slope/plane connected by a string

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Homework Help Overview

The discussion revolves around finding the acceleration of two masses connected by a string over a pulley, with one mass on a slope. Participants are analyzing the forces acting on the masses and the equations governing their motion.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to apply Newton's second law and considers both x and y components of forces. Some participants question the validity of adding these components directly to find net force.
  • There is a discussion about whether components are necessary for solving the problem, with suggestions to focus on the forces acting on the masses without breaking them into components.
  • Participants explore the implications of the pulley system on the direction of forces and how that affects the overall analysis.

Discussion Status

Some participants have offered guidance on how to approach the problem, emphasizing the need to consider the system as a whole. There is an ongoing debate about the correct application of vector addition in the context of forces.

Contextual Notes

Participants are navigating through the assumptions regarding the forces acting on the masses, particularly the role of friction and the direction of acceleration. There is also mention of the ideal conditions assumed for the string and pulley.

AJKing
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euyPI.jpg


I think I've solved this, I'm looking for an answer check.

Homework Statement



Given the picture above, find the acceleration of the block and the tension in the string. Assume the string preforms ideally and the pulley is frictionless.

Homework Equations



Fnet = ƩFx + ƩFy = ma

The Attempt at a Solution



Looking at M2, the horizontal forces are the tension in the string and the force of friction.
Ff = mg*0.47 = 10.6N

Looking at M1, the horizontal forces are the tension in the string in the opposite direction and the horizontal portion of the force pulling M1 down the hill.
F = -mg*sinθ = -18.7N
Fx = 18.7N*cosθ = - 16.66N

An ideal string transfers the forces equally, so we may ignore the string and consider the masses to be one system.
ƩFx = -16.66N+10.6N = -6.06N
ƩFy = -18.7N*sinθ = -8.49N
Fnet = √((-6.06)2+(-8.49)2) = -10.4N 27° below horizontal

-10.4N = ma = (m1+m2)a
a = -10.4N/(4.2+2.3)kg = -1.60m/s2 27° below horizontal----

There are 2 forces on m1, the tension in the string and the force of gravity down the slope.
the sum of those forces must equal -10.4N
(-10.4 + 18.7)N = 8.3N = Ts

Is this all correct?
 
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Sadly, I don't think you did this exactly right.

AJKing said:
Fnet = ƩFx + ƩFy = ma

This equation is never true. You cannot add x and y components to get a net force.

Secondly, no y-components of force are necessary in this problem. No components at all. Just the forces by themselves.

The only reason you'd need components here is to find the force pulling the 4.2kg block down the slope. You did trig for that and came up with mgsinθ, which is correct. Once you found that though, you went further and found the x-component of that force, which you don't do.

It might sound confusing because the 4.2kg object is being pulled in a different direction than the 2.3kg object, but remember that a pulley simply changes the direction of forces. Therefore, you could think of this as both objects being pulled in the same direction. So no components are necessary.

Now you need to figure out the acceleration of the system before you do much else, so simply add the force of gravity parallel to the slope that you found with mgsinθ and the force of friction of the 2.3kg object. Once you do that, it's easy to come up with the acceleration of the two blocks, but don't forget to add the two masses together.

After that, then find the tension in the rope. You only need to consider the 2.3kg block when doing this. How much force does it take to move a 2.3kg object accelerating at x m/s/s? And that's your tension.

Once again, no components are involved here.

Hope this helps
 
howie8594 said:
a pulley simply changes the direction of forces. Therefore, you could think of this as both objects being pulled in the same direction. So no components are necessary.

Ah, that makes sense. I'll find more questions like this to check my understanding.
Thanks for the response

howie8594 said:
This equation is never true. You cannot add x and y components to get a net force.

You most certainly can!
But I did write it lazily: this is what I meant and I'm certain it's true.
If I'm wrong I'd really appreciate the correction.

\vec{F}_{net} = \Sigma\vec{F}_{x} + \Sigma\vec{F}_{y} = m\vec{a}
 
I actually don't know what that means, but if it means you get an x component of force and a y component of force, then do pythagorean's theorum to get a resultant force, then that would be correct.

I was saying that if for instance, you add x components together and get 10 N, and then add y components and get 13 N, the resultant net force is not 23 N.

I'm sure that's what you meant.
 
howie8594 said:
I actually don't know what that means, but if it means you get an x component of force and a y component of force, then do pythagorean's theorum to get a resultant force, then that would be correct.

I was saying that if for instance, you add x components together and get 10 N, and then add y components and get 13 N, the resultant net force is not 23 N.

I'm sure that's what you meant.

Ok, we're both correct on that front then, I was a little shocked :P.
The arrows indicate vector addition which requires the pythagorean theorum in this case
 

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