Understanding Circular Motion: Common Misconceptions and Clarifications

In summary, my teacher said that the centrifugal force is a pseudo force that arises when we consider circular motion from a non-inertial reference frame. The only forces acting on a pendulum are its weight and the tension in the string.
  • #1
Delzac
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hi i hope that u are able to help me with these concept problems.

Q1. My teacher said that centrifugal force is aa imaginary force and that is does exist, is this true? i quote(from my teacher) " last time people thought that centrifugal force exist, but in actual fact it is a imaginary force which does not exist"



Q2. we know that the Earth is orbiting around the sun, circular motion requires that there be a centripetal acceleration towards the sun. If there is a acceleration towards the sun, shouldn't the Earth fly towards sun and collide together??


Q3. Say we have a eraser, and we put is on a spinning disc. when the rotation of the disk is slow, the eraser doesn't fly off because of friction. Now the problem arises that my teacher told me that frictional force is actually equal to centripetal force( magnitude and direction), but at any instant, the rubber's velocity is tangential to the radius, so shouldn't there be also a frictional force opposing this velocity in the apposite direction of the velocity? If this is the case, there there will be 2 frictional forces acting on the eraser instead of one.( The one which is Frictional force = centripetal force)

Q4. say we are pendulum, and we make is osscilate in a circular motion, should there be a outwards force? my teacher said that there isn't.( His explanation isn't very comprehensive)
 
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  • #2
Delzac said:
Q1. My teacher said that centrifugal force is aa imaginary force and that is does exist, is this true? i quote(from my teacher) " last time people thought that centrifugal force exist, but in actual fact it is a imaginary force which does not exist"
Yes, the centrifugal force is a pseudo forces and arises when we consider circular motion from a non-inertial reference frame (such as the frame of the object undergoing circular motion).
Delzac said:
Q2. we know that the Earth is orbiting around the sun, circular motion requires that there be a centripetal acceleration towards the sun. If there is a acceleration towards the sun, shouldn't the Earth fly towards sun and collide together??
Although, the Earth is always accelerating towards the sun, the velocity is always perpendicular to the acceleration hence the circular path. (Technically it is an elliptical orbit, but you get the idea). Just because an object is accelerating towards another object, doesn't mean that it must get any closer.
Delzac said:
Q3. Say we have a eraser, and we put is on a spinning disc. when the rotation of the disk is slow, the eraser doesn't fly off because of friction. Now the problem arises that my teacher told me that frictional force is actually equal to centripetal force( magnitude and direction), but at any instant, the rubber's velocity is tangential to the radius, so shouldn't there be also a frictional force opposing this velocity in the apposite direction of the velocity? If this is the case, there there will be 2 frictional forces acting on the eraser instead of one.( The one which is Frictional force = centripetal force)
You may want to reconsider this. Is the rubber accelerating tangentially? Or is it traveling at a constant speed?
Delzac said:
Q4. say we are pendulum, and we make is osscilate in a circular motion, should there be a outwards force? my teacher said that there isn't.( His explanation isn't very comprehensive)
No, there will never be an outward force (except the weight at the bottom of the oscillation). Ignoring drag, the only to forces acting on a pendulum is its weight and the tension in the string. Draw a free body diagram. Where would this other force originate?
 
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  • #3
For Qns 3. I meant that at any instant, the velocity of the eraser is tangent to the circle right?( refer to attachment althought it is quite blur)

Since the eraser is in circular motion, there is a centripetal acceleration right?( the "a" in the picture)

and because the eraser doesn't fly off the spinning disk, there is a frictinal force which is equal in direction and magnitude to the centripetal acceleration correct?( or so my notes says) my teacher told that only this frictional force is affecting the eraser.

Now the problem arises that, " any instant, the velocity of the eraser is tangent to the circle ". so naturally shouldn't there be also a frictional force opposing this velocity at that instant?? this in the end makes up 2 frictional force acting on the eraser, instead of the " my teacher told that ONLY this frictional force is affecting the eraser." mention above.

+ hope i explained clearly+
 

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  • #4
For Qns 4, let us replace the pendulum bob with a human, i am sure if i am in circular motion i will feel a outwards force...how can we explain this?
 
  • #5
Delzac said:
For Qns 4, let us replace the pendulum bob with a human, i am sure if i am in circular motion i will feel a outwards force...how can we explain this?

You have to make clear about which reference frame you are talking. You are feeling a force pointing outwards because your reference frame is moving with you.
 
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  • #6
And i still can't get Qns 2. If acceleration is towards the sun, a simple equation [tex]F=ma[/tex] will show that a force is exerted on the Earth by the sun(towards the direction of the sun), so can't it collide with it?( i just need a better explanation, if there is one :) )
 
  • #7
Delzac said:
And i still can't get Qns 2. If acceleration is towards the sun, a simple equation [tex]F=ma[/tex] will show that a force is exerted on the Earth by the sun(towards the direction of the sun), so can't it collide with it?( i just need a better explanation, if there is one :) )

The force you are describing will lead to a change of direction of your tangential velocity.

The applet on this website might be helpful to visualize to process: http://highered.mcgraw-hill.com/sites/0078458137/student_view0/chapter6/circular_motion_applet.html

There's a vertical scrollbar on the left that will change the circle to an ellipse.
 
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  • #8
Then this force is from the tangential velocity(at an instant) in orbit i guess... but still u can treat it like projectile motion( sort of?) then Earth while moving horizontally can also move inwards. ( treating horizontal and vertical velocity as seprated things? as in projectile motion)
 
  • #9
nazzard said:
You have to make clear about which reference frame you are talking. You are feeling a force pointing outwards because your reference frame is moving with you.


what do u mean? i dun quite understand how different reference frame affect what force u are feeling.
 
  • #10
Delzac said:
what do u mean? i dun quite understand how different reference frame affect what force u are feeling.

The important difference is: Is it an inertial reference frame or a non-inertial reference frame. In the latter case the reference frame is accelerated and fictitious forces are acting on you.

Edit: I've edited post #7 to include a link to an applet that might be helpful.
 
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  • #11
Delzac said:
i dun quite understand how different reference frame affect what force u are feeling.
It doesn't, of course. Different reference frames just change the way you describe what's going on; they don't change what's going on.

If you stick to an inertial frame, then you only need to deal with real forces, not pseudoforces.
 
  • #12
Delzac said:
For Qns 3. I meant that at any instant, the velocity of the eraser is tangent to the circle right?( refer to attachment althought it is quite blur)

Since the eraser is in circular motion, there is a centripetal acceleration right?( the "a" in the picture)

and because the eraser doesn't fly off the spinning disk, there is a frictinal force which is equal in direction and magnitude to the centripetal acceleration correct?( or so my notes says) my teacher told that only this frictional force is affecting the eraser.
This is all good.
Delzac said:
Now the problem arises that, " any instant, the velocity of the eraser is tangent to the circle ". so naturally shouldn't there be also a frictional force opposing this velocity at that instant?? this in the end makes up 2 frictional force acting on the eraser, instead of the " my teacher told that ONLY this frictional force is affecting the eraser." mention above.

+ hope i explained clearly+
This is not so good. You have said it yourself, velocity. Just because the velocity is in that direction doesn't mean there is a force. Forces create accelerations. Is there any force acting tangentially to the eraser? Is the eraser traveling at a constant speed? Remember Newton's first law. Remember that the eraser is traveling at the same velocity as the disc.
 
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  • #13
Doc Al said:
It doesn't, of course. Different reference frames just change the way you describe what's going on; they don't change what's going on.

If you stick to an inertial frame, then you only need to deal with real forces, not pseudoforces.
Just add to what the Doc said. A good way to get your head round this is to imagine a child on a round-a-bout. When you are watching a child going around on a round-a-bout what you see is the child holding on, 'pulling towards the centre of the circle'; this is the centripetal force. You are viewing this from an inertial (non-accelerating) reference frame. Now imagine you yourself are on the round-a-bout, you feel yourself being 'pulled' off the round-a-bout; this is the centrifugal force because you are in a non-inertial reference frame. Do you follow?
 
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  • #14
Thx i understand now :)
 
  • #15
Hi again, sry to dig up an old post again but i want to clarify something. :P

U guys mention that when the acceleration is perpendicular to velocity, the object will not move towards the direction of the accelration, but move in circular motion right?

Say i have a rock obiting around a planet(going in circles). in circular motion, the rock should not fall into the planet right? but sometimes, or often the case is that the rock do fall into the planet sooner of later isn't? y does this happen, shoudn't it be in circular motion(meaning it will circle the planet forvever)?

hope u understand what i am driving at :P
 
  • #16
Delzac said:
Hi again, sry to dig up an old post again but i want to clarify something. :P

U guys mention that when the acceleration is perpendicular to velocity, the object will not move towards the direction of the accelration, but move in circular motion right?

Say i have a rock obiting around a planet(going in circles). in circular motion, the rock should not fall into the planet right? but sometimes, or often the case is that the rock do fall into the planet sooner of later isn't? y does this happen, shoudn't it be in circular motion(meaning it will circle the planet forvever)?

hope u understand what i am driving at :P
If the rock is close enough to the planet that it is affected by noticable friction from the atmosphere, then there will be a component of acceleration (due to the friction force) not perpendicular to the velocity vector. That will slow the rock and cause it to eventually fall to the planet. If, however, the rock is far enough away or the planet has no atmosphere so that there is no friction, the rock will circle the planet forever.
 
  • #17
Maybe try thinking about a swinging bucket of water in a vertical plane. There is a minimum velocity such that the water will stay in the bucket. If you spin it slower, the water will spill out. If you maintain the minimum velocity, the water stays in, and at the instance at the top of the motion, the only force is gravity, which provides the centrifical force normal to the velocity.
 
  • #18
HallsofIvy said that it is due to friction of the atmosphere but civil_dude said that it is the minimum velocity so whcih is it, friction or velocity or both?
 
  • #19
Both are correct, they are just talking about different aspects of the same thing. In either case it's true that as long as the force remains perpendicular to the velocity, the rock will remain in a circular orbit.

Of course to get that rock in orbit in the first place requires a certain speed. As you know, if you throw a rock it just falls to the ground following a parabolic trajectory. The force starts out perpendicular to the velocity, but doesn't stay perpendicular. It will only stay perpendicular if the rock is moving fast enough. (Of course if the rock is moving too fast, it will have an elliptical orbit around the Earth's center--assuming it doesn't just crash into the surface at some point. Faster still and it will "escape" the Earth's gravity, never to return.)

Once the rock is in a circular orbit, as long as no other forces act it will stay there. The gravitational force and the velocity are perfectly matched to remain perpendicular. But if you add in the effect of atmospheric friction, as Halls' explained, the net force is no longer perpendicular to the velocity.
 
  • #20
thx for the explanation! :)
 

FAQ: Understanding Circular Motion: Common Misconceptions and Clarifications

What is circular motion?

Circular motion is the movement of an object along a circular path around a fixed point. This type of motion is characterized by a constant speed and a continuously changing direction.

What are some common problems with circular motion?

Some common problems with circular motion include centripetal force, centrifugal force, and the concept of angular velocity. Other problems may involve calculating the radius or period of a circular motion, or analyzing the forces acting on an object in circular motion.

What is centripetal force and how does it affect circular motion?

Centripetal force is the force that causes an object to move in a circular path. It is directed towards the center of the circle and is necessary to keep an object in circular motion. Without centripetal force, an object would continue moving in a straight line tangent to the circle.

How do you calculate the radius of circular motion?

The radius of circular motion can be calculated using the equation r = v^2/a, where r is the radius, v is the velocity, and a is the centripetal acceleration. Alternatively, if the period of the circular motion is known, the radius can be calculated using the equation r = (T/2π)^2, where T is the period.

What is the difference between centripetal force and centrifugal force?

Centripetal force and centrifugal force are often confused, but they are not the same. Centripetal force is the inward force that keeps an object in circular motion, while centrifugal force is the outward force that appears to push an object away from the center of the circle. Centrifugal force is a fictitious force that only exists in a rotating reference frame and does not actually act on the object in circular motion.

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