How Do Forces and Angles Affect Angular Acceleration in a Pulley System?

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Homework Help Overview

The discussion revolves around a pulley system involving two blocks, one on a slope and the other hanging, with the goal of determining the acceleration of the blocks. The participants are exploring the effects of forces, angles, and friction on the system's dynamics.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants are attempting to set up equations for the forces acting on each block, considering tension, gravitational components, and friction. There are questions about the correct representation of forces, particularly regarding the components of gravity acting on the inclined block and the role of tension in the system.

Discussion Status

Some participants are providing clarifications on the components of forces acting on the blocks, particularly in relation to the incline. There is an ongoing exploration of the relationships between tension, friction, and gravitational forces, with some participants expressing confusion about the correct formulations and assumptions.

Contextual Notes

Participants are discussing the implications of an ideal pulley and the effects of angles on force components. There is a mention of a coefficient of friction and the need to consider the normal force in relation to the incline.

parttime
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there are two blocks on a trapizoid one on the top and one on the side with the slope a wire that goes throu a pully connects the two. determin the the acceleration of the two blocks.
block one =m1 block two = m2 pully =m with radius r Ufriction =.36
what i have so far is
sum of forces(along x axis) on block one is t (for tension) - ufm1g=m1a(acceleration)
sum of forces (along yaxis) on block two is tsin(thata) +ufm2gsin-mg=m2a

is this correct
 
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This is not angular acceleration by the way. You might want to check that sum of the y forces again, because you must remember that (I'm assuming block 2 is on an incline) that there is a component of gravity which is pulling the block downwards and is certainly not equal to m*g. Break the force exerted due to gravity up into components vertical and horizontal to the incline.
 
for the sum of forces along y sin 30 mg for the force of gravity i just can't get the tension not sure if it is just t or tcos30
 
so would it be t -sin30*m*g + ufcos30*m*g?
also is the tension a and b both positve because the are going in the same direction or would tension b be negitive can't make sense of it
 

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parttime said:
for the sum of forces along y sin 30 mg for the force of gravity i just can't get the tension not sure if it is just t or tcos30

Remember what an ideal pulley does... it merely changes the direction of a force, therefore you would not break it up into components based on its angle relative to the rope's orientation on the other side of the pulley. You're getting closer to the answer though; your picture has not been authenticated yet so I can't give you great answers.
 
thanks for the help finally got it to give me the correct answer since i had it from the book just couldn't get it to come out . this is what i have
sum forces x = t1 - uf*m1*g =m1 *a
sum forces y =t2 +uf*m2*g*cos()-m2*g*sin() =m2*-a
that i don't understand is why for the y the weight is mgsin and the friction is mgcos (that is assuming i am doning it right when i plug in values i get the right answer for the sum)
 
parttime said:
that i don't understand is why for the y the weight is mgsin and the friction is mgcos (that is assuming i am doning it right when i plug in values i get the right answer for the sum)

The easiest way to prove it to yourself is to take it to extremes. It's not that the *weight* is mg*sin(theta) it's that the *component of gravity pulling the block downward* is mg*sin(theta). This is the force that acts opposed to the tension in the rope and the friction force at the surface. Consider the situation where theta = 0. Does it make sense that there would be no part of gravity that is able to pull a block down a flat, horizontal surface?

Now, think about what determines friction force at a contact point on a surface. It's the coefficient of friction multiplied by the normal force at that point, right? What is the component of gravity that is perpendicular to the incline? Take the angle to extremes again. What if theta was 90 degrees (and therefore mg*cos(theta) = 0, that is, the surface of the plane is vertical. Does it make sense then that gravity would produce no potential for a friction force because that force runs parallel to the surface at that inclination?
 

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