Velocity and Acceleration of a particle around a circle

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Homework Help Overview

The discussion revolves around a particle moving with constant speed around a circular path. The original poster describes the particle's position and velocity at specific points on the circle and seeks to determine its velocity and acceleration at another point. The context involves concepts from circular motion and vector calculus.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the derivatives of position vectors and the implications of unit vectors in Cartesian coordinates. Questions arise regarding the correct coordinates for the left side of the circle and how to determine the direction of motion based on velocity vectors. There is also exploration of the relationship between velocity and acceleration in circular motion.

Discussion Status

Participants are actively engaging with the problem, questioning assumptions about the particle's position and direction of motion. Some guidance has been offered regarding the nature of acceleration in circular motion and the relationship between velocity and acceleration, though no consensus has been reached on the specific equations or methods to derive them.

Contextual Notes

There are discussions about potential errors in the coordinates provided for the particle's position and the implications of these errors on the analysis. The conversation also touches on the derivation of acceleration in circular motion, indicating a need for clarity on the underlying principles.

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Homework Statement


A particle moves with constant speed around a circle. When it is at the top of the circle, its coordinates are x=0 and y=2 and its velocity is 4(m/s) i. When it reaches the left hand of the circle, where its coordinates are now x=2 and y=0, what is its velocity and acceleration respectively?

Homework Equations


[/B]
I know that a position vector consists of r= R (cos theta i + sin theta j), also velocity is the first derivative of the position vector and acceleration is the second derivative of the position vector.

How do I take a derivative of position vectors i j k, or do i just leave them as they are?

The Attempt at a Solution



Ive tried taking derivatives to arrive at an answer with the proper position vectors but can't seem to get it right.
 
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droidofthevoid said:

Homework Statement


A particle moves with constant speed around a circle. When it is at the top of the circle, its coordinates are x=0 and y=2 and its velocity is 4(m/s) i. When it reaches the left hand of the circle, where its coordinates are now x=2 and y=0, what is its velocity and acceleration respectively?[/B]

Homework Equations



I know that a position vector consists of r= R (cos theta i + sin theta j), also velocity is the first derivative of the position vector and acceleration is the second derivative of the position vector.

How do I take a derivative of position vectors i j k, or do i just leave them as they are?[/B]

The Attempt at a Solution



Ive tried taking derivatives to arrive at an answer with the proper position vectors but can't seem to get it right.

One of the simple things about cartesian coordinates is that the unit vectors i, j and k are independent of position and time. Hence, they do not affect derivatives with respect to time or x, y and z.

The first step in this question is to find ##\textbf{r}(t)##: the position vector of the particle as it moves in time. Can you do that?
 
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droidofthevoid said:

Homework Statement


A particle moves with constant speed around a circle. When it is at the top of the circle, its coordinates are x=0 and y=2 and its velocity is 4(m/s) i. When it reaches the left hand of the circle, where its coordinates are now x=2 and y=0, what is its velocity and acceleration respectively?[/B]

Shouldn't the left hand of the circle be x = -2, y = 0? Do you know how to tell from the velocity at x = 0, y = 2 whether the particle is traveling clockwise or counter-clockwise?
 
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PeroK said:
One of the simple things about cartesian coordinates is that the unit vectors i, j and k are independent of position and time. Hence, they do not affect derivatives with respect to time or x, y and z.

The first step in this question is to find ##\textbf{r}(t)##: the position vector of the particle as it moves in time. Can you do that?

I believe I had done it correctly, I got r(t) = 0i + 2j
 
Chestermiller said:
Shouldn't the left hand of the circle be x = -2, y = 0? Do you know how to tell from the velocity at x = 0, y = 2 whether the particle is traveling clockwise or counter-clockwise?
Yes, that is correct and an error on my part. well, if the velocity at r(t)= 0 i +2j is 4(m/s)i, then I would assume it is going in the clockwise direction because of the i vector. if it had been -4(m/s)i, then it would be in the counter clockwise direction.
 
droidofthevoid said:
Yes, that is correct and an error on my part. well, if the velocity at r(t)= 0 i +2j is 4(m/s)i, then I would assume it is going in the clockwise direction because of the i vector. if it had been -4(m/s)i, then it would be in the counter clockwise direction.
Right. So if it is going clockwise, what is its velocity at -2,0 (the left hand side of the circle)? What is its acceleration at this point?
 
well, I found an equation of a= (v^2)/2 i, which gave an acceleration of a = 8 m/s i. I don't understand how this equation was derived. Although, now that I have actually thought about this, the acceleration vector around a curve or a circle always points toward the center of the circle and the velocity vector is always tangent to the point on the curve, so I understand how the acceleration vector is i and the velocity vector is j for x=-2,y=0. The only problem I have is the equation I came across.

I know that velocity is the derivative of the r vector with respect to time and acceleration is the derivative of the velocity with respect to time, but where does a = (v^2)/2 come from?
 
droidofthevoid said:
well, I found an equation of a= (v^2)/2 i, which gave an acceleration of a = 8 m/s i. I don't understand how this equation was derived. Although, now that I have actually thought about this, the acceleration vector around a curve or a circle always points toward the center of the circle and the velocity vector is always tangent to the point on the curve, so I understand how the acceleration vector is i and the velocity vector is j for x=-2,y=0. The only problem I have is the equation I came across.

I know that velocity is the derivative of the r vector with respect to time and acceleration is the derivative of the velocity with respect to time, but where does a = (v^2)/2 come from?
What a great question! As you said, the acceleration is the derivative of the velocity with respect to time, and the velocity has both magnitude and direction. So the equation for the acceleration a = v^2/r in this circular motion with constant velocity is related to how the direction of the velocity vector is changing with time. There are different ways of deriving this equation, so it depends on which method is used in your textbook.

Chet
 

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