Newton's Third Law - Using pulleys and slopes

In summary, a 5.9 kg box on a frictionless 40 degree slope is connected via a massless string over a massless, frictionless pulley to a hanging 2.1 kg weight. When the box is held in place, the tension in the string is 20.61N. When the box is released, it will slide downwards on the slope and the tension in the string can be found using the equations -m1*g*sinθ+T=m1(-a) and m2*g*T=m2(a), where a is the same for both equations. The solution can be found by eliminating T and solving for a.
  • #1
tastypotato
3
0

Homework Statement


A 5.9 kg box is on a frictionless 40 degree slope and is connected via a massless string over a massless, frictionless pulley to a hanging 2.1 kg weight.

A.
What is the tension in the string if the 5.9 kg box is held in place, so that it cannot move?

B.
If the box is then released, which way will it move on the slope?

C.
What is the tension in the string once the box begins to move?

Homework Equations


Fnet=m*a


The Attempt at a Solution


A. The mass of the second box times the gravity will give me the solution to part A -> m2*(9.81)=20.61N
B. If the box is released then it will slide downwards on the slope because there is more mass in m1
C. This is where I'm stuck. My professor wrote down this equation for us to follow.

-m1*g*sin[tex]\theta[/tex]+T=m1(-a)
and
m2*g*T=m2(a)

but I don't know where to go from here.
 
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  • #2
Hi tastypotato! :smile:

(have a theta: θ :wink:)
tastypotato said:
A 5.9 kg box is on a frictionless 40 degree slope and is connected via a massless string over a massless, frictionless pulley to a hanging 2.1 kg weight.

B.
If the box is then released, which way will it move on the slope?

C.
What is the tension in the string once the box begins to move?

B. If the box is released then it will slide downwards on the slope because there is more mass in m1

Sorry, but that's the wrong reason … "more mass" doesn't clinch it … what matter is the equation your professor wrote down for you …
C. …
-m1*g*sin[tex]\theta[/tex]+T=m1(-a)
and
m2*g*T=m2(a)

(and btw, this is https://www.physicsforums.com/library.php?do=view_item&itemid=26", not third)

These two equations are the Ftotal = ma equations for m1 and m2 separately

(you have to do them separately) …

the first one is of the components in the direction of the slope, and the second is for the vertical components …

a is the same in both equations because the string has fixed length, so if m1 goes distance x up the slope, m2 goes distance vertically down …

so i] can you prove those two equations are correct?

ii] eliminate T, and find a :smile:
 
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  • #3


I would like to clarify that Newton's Third Law states that for every action, there is an equal and opposite reaction. In this scenario, the action is the force exerted by the hanging weight on the string and the reaction is the tension in the string. Therefore, the tension in the string will be the same for both boxes regardless of their masses.

To solve part C, we can use the equation F=ma. In this case, the force acting on the 5.9 kg box is its weight (m1*g) and the tension in the string (T). This results in the equation m1*g-T=m1*a. Similarly, for the 2.1 kg box, the force acting on it is its weight (m2*g) and the tension in the string (T). This results in the equation m2*g+T=m2*a. Since the acceleration for both boxes will be the same (as they are connected by a string), we can equate the two equations and solve for T. This results in T=(m1-m2)*g/2. Therefore, the tension in the string once the box begins to move is 11.7 N.

It is important to note that in this scenario, the box will not slide down the slope as there is no net force acting on it (since the tension in the string balances out its weight). It will remain in place until the tension in the string is released or changed.
 

What is Newton's Third Law?

Newton's Third Law states that for every action, there is an equal and opposite reaction. This means that when one object exerts a force on another object, the second object will exert an equal and opposite force back on the first object.

How is Newton's Third Law applied to pulleys?

In pulley systems, the forces acting on the pulley and the object attached to it follow Newton's Third Law. For example, when a person pulls down on one side of a pulley, the pulley will pull up on the other side with an equal force. This allows for easier lifting of heavy objects by distributing the force needed to lift the object.

How does Newton's Third Law apply to slopes?

On a slope, the force of gravity pulling an object down the slope is countered by the normal force from the surface of the slope pushing back on the object. According to Newton's Third Law, these forces are equal and opposite, allowing the object to remain at rest or in motion at a constant speed.

Can Newton's Third Law be observed in everyday life?

Yes, Newton's Third Law can be observed in many everyday situations. For example, when walking, you push against the ground with your feet and the ground pushes back with an equal force, allowing you to move forward. Another example is when you sit on a chair, the force of your weight pushing down is balanced by the normal force of the chair pushing up.

How does Newton's Third Law contribute to the laws of motion?

Newton's Third Law is one of the three laws of motion, along with the first and second laws. It describes the relationship between forces and motion, stating that forces always occur in pairs and are equal in strength but opposite in direction. This law helps us understand how objects move and interact with each other in the physical world.

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