Another centripetal force problem

In summary, the tension in the rope must match the centripetal force in order for the man to follow his circular path. However, the tension is not constant throughout the swing and may vary depending on the position of the man. To solve this problem, both the centripetal force equation and trigonometry can be used to find the tension at different points in the swing. At the bottom of the swing, the tension must be equal to the sum of the centripetal force and the weight of the man.
  • #1
BrainMan
279
2
A stuntman swings from the end of a 4 m long rope along the arc of a circle. If his mass is 70 kg, find the tension in the rope required to make him follow his circular path at (a) the beginning of his motion, assuming he starts when the rope is horizontal, (b) at a height of 1.5 above the bottom of the circular arc, and (c) at the bottom of the arc.

(Equation) Fc = mv^2/r
KE= 1/2mv^2
PE = mgy

(Attempt at solution)
Find the total energy of the system
4 m (9.8)(70 kg) = 2744 J
Find the kinetic energy at 1.5 m to find the velocity
70(9.8)(1.5) = 1029
2744 - 1029 = 1715 J
1/2mv^2 = 1715
V= 7 m/s
Find the centripetal force using Fc= mv^2/r
70(49/4)
Fc = 857.5
The correct answer is 1.29 x 10^3 N
 
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  • #2
You were asked to find the tension in the rope; you found the centripetal force. They're not the same thing. I suggest you draw a free-body diagram to try figure this problem out.
 
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  • #3
vela said:
You were asked to find the tension in the rope; you found the centripetal force. They're not the same thing. I suggest you draw a free-body diagram to try figure this problem out.

What makes them different? The tension in the rope must match the centripetal force in order for the man to move in a circle.
 
  • #4
BrainMan said:
The tension in the rope must match the centripetal force in order for the man to move in a circle.
That's not true. You should drop the notion of centripetal force and instead think in terms of a centripetal acceleration: objects that follow a circular path of radius ##r## experience a centripetal acceleration of magnitude ##v^2/r##. When you plug this into Newton's second law (for the radial direction), you get
$$\sum F_\text{r} = ma = m\frac{v^2}{r}.$$ You're getting the lefthand side of the equation wrong. Did you draw a free-body diagram yet?
 
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  • #5
BrainMan said:
What makes them different? The tension in the rope must match the centripetal force in order for the man to move in a circle.

The tension in the rope must cause the net centripetal force, but that does not mean that the tension in the force must match the centripetal force. (Because there are other forces involved.)

(If you're stuck, draw a FBD)
 
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  • #6
vela said:
That's not true. You should drop the notion of centripetal force and instead think in terms of a centripetal acceleration: objects that follow a circular path of radius ##r## experience a centripetal acceleration of magnitude ##v^2/r##. When you plug this into Newton's second law (for the radial direction), you get
$$\sum F_\text{r} = ma = m\frac{v^2}{r}.$$ You're getting the lefthand side of the equation wrong. Did you draw a free-body diagram yet?

Here is my free-body diagram. The T stands for tension, CF for centripetal force, TF for tangential velocity, and w for weight.
 

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  • #7
BrainMan said:
Here is my free-body diagram. The T stands for tension, CF for centripetal force, TF for tangential velocity, and w for weight.

Do you see it now?
 
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  • #8
dauto said:
Do you see it now?

No I don't. What should I be seeing?
 
  • #9
BrainMan said:
No I don't. What should I be seeing?

Ok, so we have a weight swinging around on a rope in circular motion. Let's look at the time when the rope is at the bottom of it's swing (so it's completely vertical) just to simplify things.


Suppose, like you said, that the tension in the rope is equal to the centripetal force.


What would be the net force on the weight (or person)? The tesnison is directed upwards (towards the center of the circle) but gravity is directed downwards, so what would be the Net Force on the weight? Would that Net Force be equal to the centripetal force?


For an object to move in a circle there must be a NET force equal to [itex]\frac{mv^2}{2}[/itex]

If the tension was equal to [itex]\frac{mv^2}{2}[/itex] then would the Net Force be equal to [itex]\frac{mv^2}{2}[/itex]?

What must the tension be in order for the Net Force to equal [itex]\frac{mv^2}{2}[/itex]?

(Hint: The tension is not constant throughout the swing)
 
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  • #10
Nathanael said:
Ok, so we have a weight swinging around on a rope in circular motion. Let's look at the time when the rope is at the bottom of it's swing (so it's completely vertical) just to simplify things.


Suppose, like you said, that the tension in the rope is equal to the centripetal force.


What would be the net force on the weight (or person)? The tesnison is directed upwards (towards the center of the circle) but gravity is directed downwards, so what would be the Net Force on the weight? Would that Net Force be equal to the centripetal force?


For an object to move in a circle there must be a NET force equal to [itex]\frac{mv^2}{2}[/itex]

If the tension was equal to [itex]\frac{mv^2}{2}[/itex] then would the Net Force be equal to [itex]\frac{mv^2}{2}[/itex]?

What must the tension be in order for the Net Force to equal [itex]\frac{mv^2}{2}[/itex]?

(Hint: The tension is not constant throughout the swing)

So the centripetal force doesn't have to be the same as the tension because the tension is reliant on the weight and the acceleration due to gravity while the centripetal force relies on the mass, the velocity , and the radius. So do I even have to use centripetal force to solve this problem? Can I just use trigonometry and the weight vector to find the tension?
 
  • #11
BrainMan said:
So the centripetal force doesn't have to be the same as the tension because the tension is reliant on the weight
I don't think this is a good interpretation.

BrainMan said:
So do I even have to use centripetal force to solve this problem? Can I just use trigonometry and the weight vector to find the tension?

You do need the centripetal force still. You'll need both methods.

If you're at the bottom of the swing (completely vertical) then you have the equation:

[itex]F_{centripetal}=F_{net}=F_{tension}-F_{gravity}[/itex]

Therefore:
[itex]F_t=F_c+F_g=\frac{mv^2}{2}+mg[/itex]


The bottom of the swing is the easiest place to analyze it (because no angles are involved)


I'll let you figure it out for other parts of the swing (that do involve angles) but do you understand the logical principle I'm applying?

The logic is that the only two forces are gravity and tension and they must combine to give a Net Force of [itex]\frac{mv^2}{2}[/itex] (towards the center)
 
  • #12
Nathanael said:
I don't think this is a good interpretation.



You do need the centripetal force still. You'll need both methods.

If you're at the bottom of the swing (completely vertical) then you have the equation:

[itex]F_{centripetal}=F_{net}=F_{tension}-F_{gravity}[/itex]

Therefore:
[itex]F_t=F_c+F_g=\frac{mv^2}{2}+mg[/itex]


The bottom of the swing is the easiest place to analyze it (because no angles are involved)


I'll let you figure it out for other parts of the swing (that do involve angles) but do you understand the logical principle I'm applying?

The logic is that the only two forces are gravity and tension and they must combine to give a Net Force of [itex]\frac{mv^2}{2}[/itex] (towards the center)
OK I see it now. Thanks!
 
  • #13
BrainMan said:
OK I see it now. Thanks!

No problem
 
  • #14
Nathanael said:
I don't think this is a good interpretation.



You do need the centripetal force still. You'll need both methods.

If you're at the bottom of the swing (completely vertical) then you have the equation:

[itex]F_{centripetal}=F_{net}=F_{tension}-F_{gravity}[/itex]

Therefore:
[itex]F_t=F_c+F_g=\frac{mv^2}{2}+mg[/itex]


The bottom of the swing is the easiest place to analyze it (because no angles are involved)


I'll let you figure it out for other parts of the swing (that do involve angles) but do you understand the logical principle I'm applying?

The logic is that the only two forces are gravity and tension and they must combine to give a Net Force of [itex]\frac{mv^2}{2}[/itex] (towards the center)
Alright now I am having trouble with the angle. I know that at 1.5 m above the ground the force of gravity is perpendicular to the ground and in order to find the amount of that force that effects the tension I have to use trigonometry. So T = 1/2mv2 + mg sin θ (or cos θ). The problem I have is that I don't know whether to use sin or cosine or how to find the angle. Do I use radians to find the angle?
 
  • #15
BrainMan said:
Alright now I am having trouble with the angle. I know that at 1.5 m above the ground the force of gravity is perpendicular to the ground and in order to find the amount of that force that effects the tension I have to use trigonometry. So T = 1/2mv2 + mg sin θ (or cos θ). The problem I have is that I don't know whether to use sin or cosine or how to find the angle. Do I use radians to find the angle?

First step is to find the angle. How? Draw a picture.


Can you find the θ in my picture? (Maybe I shouldn't have labeled the 2.5m side haha)


If you're stuck on whether to use cosine or sine and whatnot or something else I want to see you draw a picture to try to figure it out
 

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  • #16
Nathanael said:
First step is to find the angle. How? Draw a picture.Can you find the θ in my picture? (Maybe I shouldn't have labeled the 2.5m side haha)If you're stuck on whether to use cosine or sine and whatnot or something else I want to see you draw a picture to try to figure it out

ImageUploadedByPhysics Forums1402688824.676259.jpg


I found theta by doing the inverse cos of 2.5/4 = .89566. I found out whether to use sin or cos by drawing the picture. So
T = 70(7)/2 + mg/ cos .89566
T = 1715 + 686 / cos .89567
T = 2812.59
This is not the correct answer
Ignore the caption under the photo
 
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  • #17
Don't you want g (or mg) to be the hypotenuse? Because you're trying to break up the force of gravity into it's components (specifically it's tangent and perpendicular components)

Your drawing is wrong, gravity should be the hypotenuse.EDIT:
Can you explain your calculations?

Also in your drawing you put 0.89566 degrees, but it would actually be radians (I don't think this effected your math though)Why didn't your calculation involve the centripetal equation?
 
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  • #18
Nathanael said:
Don't you want g (or mg) to be the hypotenuse? Because you're trying to break up the force of gravity into it's components (specifically it's tangent and perpendicular components)

Your drawing is wrong, gravity should be the hypotenuse.EDIT:
Can you explain your calculations?

Also in your drawing you put 0.89566 degrees, but it would actually be radians (I don't think this effected your math though)

I thought the force of gravity always was a straight line down?
 
  • #19
BrainMan said:
I thought the force of gravity always was a straight line down?

It is, but you can sill make it the hypotenuse. Look at the drawing I've attatched, that is how it should be.


But why didn't your calculations involve the centripetal force equation?
 

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  • #20
Nathanael said:
It is, but you can sill make it the hypotenuse. Look at the drawing I've attatched, that is how it should be.But why didn't your calculations involve the centripetal force equation?

Ok I did that but I'm still not getting the right answer. I did
Mg cos .88566 = 428.75
Then I plugged that into the equation
Mv^2/r + 428.76 = T
70(7)/2 + 428.75 = 2143.75
Which is not the right answer
I got the velocity 7 from an earlier calculation attempt.
 
  • #21
BrainMan said:
Ok I did that but I'm still not getting the right answer. I did
Mg cos .88566 = 428.75
Then I plugged that into the equation
Mv^2/r + 428.76 = T
70(7)/2 + 428.75 = 2143.75
Which is not the right answer
I got the velocity 7 from an earlier calculation attempt.
You run the risk of accumulating rounding errors by substituting in numbers too soon. Keep everything symbolic until the final step. This also helps simplify the process by finding cancellations of terms, helps others follow your logic and helps you spot algebraic errors. It's a very good habit to get into.
In the present case, you would have avoided taking any square roots, since it's the value of v2 that you need. You would also have avoided figuring out the angle since the information provided gives you the trig function of it that you need (cos).
If you still don't get the right answer, please repost your working in purely symbolic form.
 
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  • #22
haruspex said:
You run the risk of accumulating rounding errors by substituting in numbers too soon. Keep everything symbolic until the final step. This also helps simplify the process by finding cancellations of terms, helps others follow your logic and helps you spot algebraic errors. It's a very good habit to get into.

In the present case, you would have avoided taking any square roots, since it's the value of v2 that you need. You would also have avoided figuring out the angle since the information provided gives you the trig function of it that you need (cos).

If you still don't get the right answer, please repost your working in purely symbolic form.

I don't think it has to do with my rounding. My answer is double the correct answer..
 
  • #23
Edit:
nevermind
 
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  • #24
Nathanael said:
Doesn't it equal 673.75? Is that the correct answer?
The answer is 1.29 x 10^3
 
  • #25
BrainMan said:
The answer is 1.29 x 10^3

I was just thrown off because you put 70(7)/2 instead of 70(7^2)/2

Honestly I don't know why your answer is wrong, I'll let you know if I think of anything
 
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  • #26
BrainMan said:
I don't think it has to do with my rounding. My answer is double the correct answer..

I didn't say rounding was the primary cause of your error, it's just one contribution.
Your main error is here:
Mv^2/r + 428.76 = T
70(7)/2 + 428.75 = 2143.75
Passing over the missing power of 2 on the 7 (just a typo), r is not 2.
 
  • #27
haruspex said:
Your main error is here:

Passing over the missing power of 2 on the 7 (just a typo), r is not 2.

hahah of course I (and you, brainman) was mixing up the centripetal equation with kinetic energy equation

You had it all right, you (and I) just made a silly mistake :)
 
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  • #28
Alright thanks guys! That problem was pretty tough.
 

1. What is a centripetal force?

A centripetal force is a force that acts on an object moving in a circular path, pulling it towards the center of the circle.

2. How is centripetal force calculated?

Centripetal force is calculated using the equation F = mv^2/r, where F is the force, m is the mass of the object, v is the velocity, and r is the radius of the circular path.

3. What are some real-life examples of centripetal force?

Some examples of centripetal force include a car turning around a curve, a satellite orbiting around the Earth, and a merry-go-round spinning.

4. How does centripetal force affect the motion of an object?

Centripetal force causes an object to continuously change direction and move in a circular path, rather than a straight line.

5. What are the differences between centripetal force and centrifugal force?

While centripetal force pulls an object towards the center of a circle, centrifugal force is the apparent outward force experienced by an object moving in a circular path. Centrifugal force is not a real force, but rather a result of inertia and the object's tendency to continue moving in a straight line.

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