How Do You Calculate Angular Momentum for a Particle in Non-Linear Motion?

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Homework Help Overview

The discussion revolves around calculating the angular momentum of a particle in non-linear motion, described by a position vector that includes time-dependent terms. Participants are tasked with finding the angular momentum about the origin and the force required to produce the motion, while verifying a relationship involving the time derivative of angular momentum.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the formulation of angular momentum using the cross product of position and momentum vectors, expressing uncertainty about the proper substitution of components and unit vectors. There are questions about the correct approach to differentiate the position vector to find velocity and subsequently acceleration.

Discussion Status

Some participants have provided clarifications regarding the cross product and the differentiation process. There is ongoing exploration of how to derive the force from the second derivative of the position vector, with some participants confirming their understanding of the components involved.

Contextual Notes

Participants are working under the constraints of homework rules, which may limit the amount of direct guidance provided. There is a focus on ensuring that assumptions about the components of vectors are checked and validated throughout the discussion.

karnten07
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Homework Statement



A particle of mass m follows a path given by

r = (Xo + at^2)x + bt^3 y + ct z

where o, a, b and c are constants, t is the time. x, y , z should have hats on them showing they are position vectors (unit vectors).

1. Find the angular momentum L of the particle about the origin.
2. Find the force F required to produce this motion and verify explicitly that dL/dt = r x F


Homework Equations






The Attempt at a Solution



L = r x p

p = mv

to get v differentiate r w.r.t time to get v = 2at.x + (3bt^2)y + cz

Subsitute into the equation:

L = ((Xo + at^2)x + bt^3y + ctz) x m(2at.x + (3bt^2)y + cz)

Now to perform the cross product, I am a bit unsure here. For the cross product i have this formula:

r x p = x(ry.pz - rz.py) - y(rx.pz - rz.px) + z(rx.py - ry.px)

where the x,y,z are unit vectors and the other x,y and z's are in subscript showing the particular component of each vector. So I am a bit confused because do i just subsitute the constants from my equations of r and p or do i include their respective unit vecotrs associated with each component? But if i did that i would get for example x x y = z so would make quite a difference.

Any thought guys, thanks
 
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karnten07 said:

Homework Statement



A particle of mass m follows a path given by

r = (Xo + at^2)x + bt^3 y + ct z

where o, a, b and c are constants, t is the time. x, y , z should have hats on them showing they are position vectors (unit vectors).

1. Find the angular momentum L of the particle about the origin.
2. Find the force F required to produce this motion and verify explicitly that dL/dt = r x F


Homework Equations






The Attempt at a Solution



L = r x p

p = mv

to get v differentiate r w.r.t time to get v = 2at.x + (3bt^2)y + cz

Subsitute into the equation:

L = ((Xo + at^2)x + bt^3y + ctz) x m(2at.x + (3bt^2)y + cz)

Now to perform the cross product, I am a bit unsure here. For the cross product i have this formula:

r x p = x(ry.pz - rz.py) - y(rx.pz - rz.px) + z(rx.py - ry.px)
to be more clear, this is

[tex] \vec{ r} \times \vec{ p} = (r_y p_z - r_z p_y) \hat{i} - (r_x p_z - r_z p_x) \hat{j} + (r_x p_y - r_y p_x) \hat{k}[/tex]
where the x,y,z are unit vectors and the other x,y and z's are in subscript showing the particular component of each vector. So I am a bit confused because do i just subsitute the constants from my equations of r and p or do i include their respective unit vecotrs associated with each component? But if i did that i would get for example x x y = z so would make quite a difference.

Any thought guys, thanks
In the equation above, r_x, p_y, etc are the components of your vectors [itex]\vec{r}, \vec{p}[/itex].
 
nrqed said:
to be more clear, this is

[tex] \vec{ r} \times \vec{ p} = (r_y p_z - r_z p_y) \hat{i} - (r_x p_z - r_z p_x) \hat{j} + (r_x p_y - r_y p_x) \hat{k}[/tex]

In the equation above, r_x, p_y, etc are the components of your vectors [itex]\vec{r}, \vec{p}[/itex].

Ok thankyou for explaining, i thought i was overthinking it. So i think that i get my value of L from r x p as:

x(mc(Xo + at^2 - 3bt^3)) - y(mc(Xo - at^2)) + z(mb(Xo + t^2(a+3-2at^2))

How do i find the Force required to produce this motion?

Edit: do i just take the double derivative of r to get the acceleration and use F = ma. Then by taking the derivative of L i can show that my F multiplied by r should equal this derivative?
 
Last edited:
karnten07 said:
Ok thankyou for explaining, i thought i was overthinking it. So i think that i get my value of L from r x p as:

x(mc(Xo + at^2 - 3bt^3)) - y(mc(Xo - at^2)) + z(mb(Xo + t^2(a+3-2at^2))

How do i find the Force required to produce this motion?

the force vector is simply the second derivative with respect to time of you rposition vector.
 
nrqed said:
the force vector is simply the second derivative with respect to time of you rposition vector.

I need to multiply it by m after differentiating it twice to get F right?
 
nrqed said:
the force vector is simply the second derivative with respect to time of you rposition vector.

Okay, I am taking the secomd derivative of r, but a bit sure on my math. I have

v = 2atx + 3bt^2 y + cz

for a I am getting it = 2ax + 6bt y

but i wasn't sure if the z component completely disappeared or if the cz become just z - sorry I am a bit rusty on this stuff. Anyone?
 
karnten07 said:
Okay, I am taking the secomd derivative of r, but a bit sure on my math. I have

v = 2atx + 3bt^2 y + cz

for a I am getting it = 2ax + 6bt y

but i wasn't sure if the z component completely disappeared or if the cz become just z - sorry I am a bit rusty on this stuff. Anyone?

The z component of a is zero . (if you want, the derivative of [itex]c \hat{k}[/itex] is zero. )
 
nrqed said:
The z component of a is zero . (if you want, the derivative of [itex]c \hatk}[/itex] is zero. )

Thankyou, i had convinced myself of that also after a while. Just had to check.
 

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