Angular Momentum of a 3kg Particle at t=5s

AI Thread Summary
To find the angular momentum of a 3kg particle at t=5s, the position function is evaluated, yielding specific coordinates in meters. The discussion highlights the importance of ensuring correct units, clarifying that "ms" should be interpreted as "m/s." The particle's velocity is constant, simplifying the calculation of angular momentum, which involves the cross product of the position vector and the momentum vector. Participants emphasize the correct placement of components in the cross product matrix and confirm that taking the derivative of the position function provides the velocity vector. Understanding these steps is crucial for accurately calculating the angular momentum about the origin.
Nickluvn
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Homework Statement



A 3kg particle has its position as a function of time given by
(−3m + 1 ms t)xˆ + (4m + 2 ms t)yˆ − 3 ms tzˆ . What is the particle’s angular momentum about the origin at t=5s?

Homework Equations



m1v1+m2v2=m1v1f + m2v2f

The Attempt at a Solution



I plugged in the value for t = 5s

gave me (-3m + 5 ms)x^ + ( 4m + 10 ms)y^-15 ms z^

what i am unsure about is the usage of the cross product.
 
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Nickluvn said:

Homework Statement



A 3kg particle has its position as a function of time given by
(−3m + 1 ms t)xˆ + (4m + 2 ms t)yˆ − 3 ms tzˆ . What is the particle’s angular momentum about the origin at t=5s?

Homework Equations



m1v1+m2v2=m1v1f + m2v2f

The Attempt at a Solution



I plugged in the value for t = 5s
So far so good. On way to approach this problem is to first find the particle's position r at t = 5 sec.
gave me (-3m + 5 ms)x^ + ( 4m + 10 ms)y^-15 ms z^
You lost me on your units.

Are you sure the position isn't actually given as:

\vec r = (-3 \ [\mathrm{m}] + (1 \ [\mathrm{m/s}])t ) \hat x \ \<br /> + \ \ (4 \ [\mathrm{m}] + (2 \ [\mathrm{m/s}])t ) \hat y \ \<br /> + \ \ (-3 \ [\mathrm{m/s}]})t \hat z \ \ ?

That would make all the units come out be meters. I really don't know what units of ms are (something doesn't look right there).

Once you have the position at time t = 5 sec, the next thing is to find the particle's velocity at time t = 5 sec. (It's easy in this case since the particle is traveling at a constant velocity.)

what i am unsure about is the usage of the cross product.
Once you have the particle's position (about the origin) and velocity at time t = 5 sec, find the angular momentum about the origin.

\vec L = \vec r \times m \vec v = \left| <br /> \begin{array}{ccc} <br /> \hat x &amp; \hat y &amp; \hat z \\<br /> r_x &amp; r_y &amp; r_z \\<br /> mv_x &amp; mv_y &amp; mv_z<br /> \end{array} \right|
 
My bad it should be m/s. Thanks again man this helped me alot, I am just confused on the placement of R in the matrix you provided.

Velocity because it is constant would mean that we would take the derivative of the function given and then plug in a value for t?
 
Nickluvn said:
My bad it should be m/s. Thanks again man this helped me alot, I am just confused on the placement of R in the matrix you provided.
The r components go in the middle. It's the definition of the cross product.

<br /> \vec A \times \vec B = \left| <br /> \begin{array}{ccc} <br /> \hat x &amp; \hat y &amp; \hat z \\<br /> A_x &amp; A_y &amp; A_z \\<br /> B_x &amp; B_y &amp; B_z<br /> \end{array} \right| <br />

That's true for any vectors, A and B. (Excuse my mismatching notation. I'm using either boldface or the upper arrow to indicate vectors.)

And by the way, it's not just a matrix. It's the determinant of a matrix. Do an Internet search on "determinant of a matrix" if you're not sure where to go from here.
Velocity because it is constant would mean that we would take the derivative of the function given and then plug in a value for t?
Yes, that will work fine! :approve:

All I'm saying it it turns out to be pretty simple in this case (The variable t goes away in each component in this particular case, leaving a constant velocity independent of t). But yes, taking the derivative of r with respect to t will give you the velocity vector v.
 
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