Free body diagrams with tension

In summary, the difference between T and t is that t is the force of tension and T is the force of gravity. T-mg is the force of tension on top of a mass and mg-t is the force of gravity on bottom of the mass.
  • #1
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My question is for free body diagrams with tension on top and mass hanging from the bottom. Why is it "T-mg" sometimes and "mg-t" other times. How do I know which one to use? I was doing gravitation questions where "T-mg=Fc" sometimes and "mg-t=Fc" other times.
 
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  • #2
the net centripetal force is in the direction of the centripetal acceleration... if the thing is at the top, the centripetal acceleration is downward, and thus the gravitational force is winning (it must be in order to make the net force point down), so the gravitational force is greater and comes before tension...
 
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  • #3
hmm I am still kinda confused on this one..
 
  • #4
So are we. What is the difference between T and t? You haven't described the problem at all well.
 
  • #5
T is tension... he's referring to one of those ferris wheel problems asking what is the force of tension on the carriage while it is at the top/bottom of the revolution... I messed up on my answer because I thought you would get the gist so I didn't worry about the details... Fc=mv^2/r ... now let's say the mass is at the bottom of the revolution like you said, now let's find the net force. The force of tension and the force of gravity are in opposite directions (tension up, towards the center, and gravity down) so you know to subtract... but which to subtract from which... You want the net force to be positive, so if they tell you both forces just put the bigger one first... but let's say you're solving for tension. How do you know if tension is bigger and you should write T-mg=mv^2/r or gravity is bigger and you should write mg-T=mv^2/r.. if you don't know how big tension is... well the way to find out is to look at which direction the centripetal force needs to be pointing... the centripetal net force should always point to the center, so if the mass is at the bottom like we assumed you know that the net centripetal force should be pointing... up... well since the net force must point up (and must be positive), you know that the force of tension must be greater than the force of gravity... thus you use T-mg... that's your answer... using mg-T in this case would give you a) a negative net force or b) a net force pointing away from the center ...thats bad

btw, disregard my post above, if the mass is at the top of the revolution, both the force of gravity and force of tension would be pointing down and the net force would just be T+mg
 
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  • #6
oo, i get it now. thanks a bunch for writing the explanation!
 

Related to Free body diagrams with tension

1. What is a free body diagram?

A free body diagram is a visual representation of the forces acting on an object. It includes all external forces, such as weight, tension, and normal force, and is used to analyze the motion of an object.

2. How do you draw a free body diagram with tension?

To draw a free body diagram with tension, start by identifying the object and all external forces acting on it. Then, draw the object as a dot or box and draw arrows representing the direction and magnitude of each force, including tension. Make sure the arrows are proportional to the magnitude of the force.

3. What is tension in a free body diagram?

Tension is a pulling force that is exerted by a string, rope, or cable on an object. It is represented by an arrow pointing away from the object and is equal in magnitude to the force applied by the string on the object.

4. How do you calculate tension in a free body diagram?

To calculate tension in a free body diagram, you can use Newton's second law, which states that the sum of all forces acting on an object is equal to its mass multiplied by its acceleration. You can set up equations for each direction (horizontal and vertical) and solve for the tension force.

5. Why are free body diagrams with tension important?

Free body diagrams with tension are important because they allow us to understand the forces acting on an object and predict its motion. They are also useful for solving problems involving tension, such as determining the maximum weight a rope can hold before breaking.

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