How Do You Calculate Jerk in Uniform Circular Motion?

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SUMMARY

The discussion focuses on calculating the jerk of an object in uniform circular motion (UCM), specifically its direction and magnitude. The formula for jerk is defined as j = d(a)/dt, where the acceleration vector's perpendicular component is derived from the parameterized position function r(t) = R(cos(ωt) i + sin(ωt) j). Participants clarify that the jerk components are j_x = Rω³sin(ωt) and j_y = -Rω³cos(ωt), while also emphasizing the need to express these in terms of linear velocity (v) and radius (r). The conversation highlights the relationship between angular and linear quantities, particularly v = ωr and a = αr.

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  • Understanding of uniform circular motion (UCM)
  • Familiarity with differentiation in calculus
  • Knowledge of angular velocity (ω) and linear velocity (v)
  • Basic concepts of jerk and acceleration in physics
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Homework Statement


The question asks to calculate the jerk of an object (both its direction and magnitude) in uniform circular motion.

Homework Equations


j=d(a)/dt

The Attempt at a Solution


I know that the direction is opposite the velocity vector (I did this by drawing a circle and taking a limit of average acceleration as t approaches 0). I also know that the parallel component of jerk is 0 because the parallel component of acceleration in UCM is 0. I am stuck on the magnitude of the perpendicular component. I know that
\vec{a}_{\perp} = \frac{v^2}{2}(-r) (the r is a unit vector)... can I just take the derivative of this? wouldn't that be 0? because v^2/r is a constant and there is no t. i am suck.
 
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Perhaps start with a parameterized version of the motion?

##r(t) = R (cos(\omega t) \vec{i} + sin(\omega t) \vec{j})##

Should be easy enough to differentiate repeatedly...
 
gneill said:
Perhaps start with a parameterized version of the motion?

##r(t) = R (cos(\omega t) \vec{i} + sin(\omega t) \vec{j})##

Should be easy enough to differentiate repeatedly...
where did you get that parameterized version?
 
It's just a conversion from polar form to rectangular form of a circle. x = R cos(θ), y = R sin(θ), where θ = ωt to make it time dependent.
 
gneill said:
It's just a conversion from polar form to rectangular form of a circle. x = R cos(θ), y = R sin(θ), where θ = ωt to make it time dependent.
ok so, j_x = Rw^3sin(wt) and j_y = -Rw^3cos(wt) right?

the problem is however that my prof wanted us to express it interms of v and r. i don't really know how to convert from w to r... we haven't really talked about w yet.
 
It seems strange that you'd be learning about a concept like jerk without having covered the basics of rotational motion.

##v = \omega r~~ ; ~~a = \alpha r## are the basic relationships between angular and linear velocities and accelerations. You would profit from taking the magnitudes of each of the vectors along the differentiation path: position → velocity → acceleration → jerk. For example, the magnitude of the velocity vector is v = ω R.
 
gneill said:
It seems strange that you'd be learning about a concept like jerk without having covered the basics of rotational motion.

##v = \omega r~~ ; ~~a = \alpha r## are the basic relationships between angular and linear velocities and accelerations. You would profit from taking the magnitudes of each of the vectors along the differentiation path: position → velocity → acceleration → jerk. For example, the magnitude of the velocity vector is v = ω R.
yeah, it was just one problem out of a list of 10 or so. our teacher kinda talked about w in the last 5 minutes of class on friday, but we haven't touched rotations yet... we haven't even begun f=ma (school just started)
 
toesockshoe said:
the problem is however that my prof wanted us to express it interms of v and r. i don't really know how to convert from w to r... we haven't really talked about w yet.

toesockshoe said:
our teacher kinda talked about w in the last 5 minutes of class on friday,

Did your teacher mention that v2/r = rw2?

Most classes have reading assignments in addition to classroom lectures, so maybe it's discussed in more depth there.
 
Mister T said:
Did your teacher mention that v2/r = rw2?

Most classes have reading assignments in addition to classroom lectures, so maybe it's discussed in more depth there.
he wrote on the board that v=ds/dt = r d(theta)/dt ... and d(theta)/dt is the same as w. that is all he talked/wrote about w. so sorry Mister T... it was hidden in my notes... i guess he did write an equation relating the 2.
 
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toesockshoe said:
ok so, j_x = Rw^3sin(wt) and j_y = -Rw^3cos(wt) right?

Right. So looking at the x-components and the y-components of the position vector and the acceleration vector, what can you conclude about the direction of those two vectors?

Now make the same comparison of the velocity vector and the jerk vector.

Can you find the magnitude of these vectors from their components?

These should lead you to being able to describe the magnitude and direction of the jerk vector, which is what your teacher is asking you to do.
 

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