What is the angle between the acceleration and velocity when rotating?

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Homework Help Overview

The discussion revolves around determining the angle between acceleration and velocity in a rotational motion context, specifically after one complete rotation (2π radians). The original poster attempts to calculate angular acceleration and subsequently tangential and radial accelerations, leading to a proposed angle.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the calculations related to angular acceleration and its implications on tangential and radial accelerations. There are questions about the correctness of the proposed angle and the necessity of diagrams to clarify the situation. Some participants explore the relationship between angular speed and linear speed, as well as the direction of tangential acceleration.

Discussion Status

The conversation is ongoing, with participants providing insights and corrections to each other's reasoning. There is a recognition of the need for diagrams and a suggestion to approach the problem using vector notation to find the angle between the acceleration and velocity vectors.

Contextual Notes

Participants mention the absence of a solution manual and the potential for sign errors in calculations. The discussion includes considerations of angular velocity and acceleration, with some uncertainty about the correct interpretation of the angles involved.

bolzano95
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Homework Statement
A body is circulating on a fixed circumference with radius R=1m. It moves with an angular velocity ##ω = \frac {k} {\sqrt{φ}}##.
Relevant Equations
Relevant equations are listed below in solving process.
CamScanner 02-11-2021 17.41_1.jpg
##ω = \frac {k} {\sqrt{φ}}##
What is the angle between acceleration and velocity after 1spin (2π radians)?

First I decided to find out what is the angular acceleration:
##α = \frac {dω} {dt} = \frac {dω} {dt} \frac {dφ} {dφ} = \frac {dω} {dφ} ω \implies ##after integrating ##\implies α = - \frac {k^2} {2φ^2}##
## a_t= αR = - \frac {k^2} {2φ^2} R##
## a_r= ω^2R= \frac {k^2} {φ} R##
## a= \sqrt{a_t^2+a_r^2}=...##

Because ##\vec{v}## is parallel to ##\vec{a_t}## we can use ## tanθ = |\frac {a_r} {a_t}|\implies## after evaluating for ##φ=2π \implies θ=85,45°##

Is this correct?
 
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Did you draw a diagram?
 
I did. I'm just not sure about the result. Unfortunately I have no solution manual.
 
bolzano95 said:
I did. I'm just not sure about the result. Unfortunately I have no solution manual.
You're almost right, but you need to draw a diagram.
 
bolzano95 said:
I did. I'm just not sure about the result. Unfortunately I have no solution manual.
Perhaps you can post the diagram that you drew?
 
Posted above in the solving process.
 
It helps. Is the angular speed increasing or decreasing as this thing goes around?
 
If you look at the equation ##ω = \frac {k} {\sqrt{φ}}## I would say the angular speed is decreasing.
 
bolzano95 said:
If you look at the equation ##ω = \frac {k} {\sqrt{φ}}## I would say the angular speed is decreasing.
Right which means that the linear speed is also decreasing. What is the direction of the tangential acceleration for that to happen?
 
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  • #10
bolzano95 said:
If you look at the equation ##ω = \frac {k} {\sqrt{φ}}## I would say the angular speed is decreasing.
Yes, and ##\alpha## was negative in your calculations.
 
  • #11
If I increase the angle, then the angular velocity decreases but is still positive. So the velocity vector is OK as drawn.
The angular velocity is decreasing so I need a negative angular acceleration and if it is negative then is directed in the clockwise direction of circulation. The tangential acceleration is then parallel to the velocity but has an opposite direction.
The correct solution then is $$ ψ=π-θ= 94,55^\circ$$
 
  • #12
bolzano95 said:
If I increase the angle, then the angular velocity decreases but is still positive. So the velocity vector is OK as drawn.
The angular velocity is decreasing so I need a negative angular acceleration and if it is negative then is directed in the clockwise direction of circulation. The tangential acceleration is then parallel to the velocity but has an opposite direction.
The correct solution then is $$ ψ=π-θ= 94,55^\circ$$
Flipping the angle from π - θ to π + θ will not give you the correct answer if θ is incorrect.
At this point I would suggest another line of attack that will give you the angle without a diagram. It's what I did. Write the linear acceleration vector ##\vec a## and linear velocity vector ##\vec v## in unit vector notation (polar coordinates) and then consider that the cosine of the angle ##\psi## between them is given by $$\cos\psi = \frac{\vec a \cdot \vec v}{av}.$$
 
  • #13
bolzano95 said:
If I increase the angle, then the angular velocity decreases but is still positive. So the velocity vector is OK as drawn.
The angular velocity is decreasing so I need a negative angular acceleration and if it is negative then is directed in the clockwise direction of circulation. The tangential acceleration is then parallel to the velocity but has an opposite direction.
The correct solution then is $$ ψ=π-θ= 94,55^\circ$$
I get the same.
 
  • #14
haruspex said:
I get the same.
I too get the same now. I had a sign error in my solution.
 

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