Proof related to angular momentum

AI Thread Summary
To prove that the angular momentum of a system of particles remains the same about all origins when the total linear momentum is zero, start with the definition of total angular momentum, which is the sum of the cross products of position vectors and momenta for each particle. When shifting the origin, the new position vector can be expressed as the original position vector minus a constant vector. This leads to the conclusion that the change in angular momentum due to the shift is zero, as the term involving the total linear momentum vanishes when it is zero. The proof is confirmed by recognizing that the angular momentum remains invariant under the shift of origin. Thus, the angular momentum is consistent across different reference points when linear momentum is zero.
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Homework Statement


Show that if the total linear momentum of system of particles is zero, the angular momentum of the system is same about all origins.


Homework Equations





The Attempt at a Solution


I really don't know where to begin with this. I am not good at these kind of proofs. I need a few hints on how to approach such problems.

Any help is appreciated. Thanks!
 
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You want to prove a general result. So, start with the most general definition of the total angular momentum of a system of particles. See what happens to this expression if you shift the origin.
 
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Start by writing up what you know, namely the expression for the total linear momentum (which you know is zero) and the total angular momentum for some arbitrary points a and b. You then may want to look at how each relative vector from point b to a particle relates to the relative vector from point a to same particle?
 
TSny said:
You want to prove a general result. So, start with the most general definition of the total angular momentum of a system of particles. See what happens to this expression if you shift the origin.

Angular momentum for a particle is defined as
$$\vec{L}=\vec{r}\times \vec{p}$$
where ##\vec{r}## is the radius vector of the particle from some fixed point (origin) and ##\vec{p}## is the momentum of particle.

For a system of particle,
$$\vec{L}=\sum_i \vec{r_i} \times \vec{p_i}$$
where i denotes the ith particle.

Shifting the origin, the new position vector for the ith particle is
$$\vec{r_i'}=\vec{r_i}-\vec{R}$$
Hence,
$$\vec{L'}=\sum_i \vec{r_i'}\times \vec{p_i}=\sum_i(\vec{r_i}-\vec{R})\times p_i$$
$$\Rightarrow \vec{L'}=\vec{L}-\sum_i \vec{R}\times \vec{p_i}$$
The second term is zero, hence proved.

Is this the correct way? Did I use the right words?

Thank you TSny! :)
 
Pranav-Arora said:
Angular momentum for a particle is defined as
$$\vec{L}=\vec{r}\times \vec{p}$$
where ##\vec{r}## is the radius vector of the particle from some fixed point (origin) and ##\vec{p}## is the momentum of particle.

For a system of particle,
$$\vec{L}=\sum_i \vec{r_i} \times \vec{p_i}$$
where i denotes the ith particle.

Shifting the origin, the new position vector for the ith particle is
$$\vec{r_i'}=\vec{r_i}-\vec{R}$$
Hence,
$$\vec{L'}=\sum_i \vec{r_i'}\times \vec{p_i}=\sum_i(\vec{r_i}-\vec{R})\times p_i$$
$$\Rightarrow \vec{L'}=\vec{L}-\sum_i \vec{R}\times \vec{p_i}$$
The second term is zero, hence proved.

Is this the correct way? Did I use the right words?

Thank you TSny! :)

Looks right to me. The final result is more obvious if you write out explicitly that $$\sum_i \vec{R}\times \vec{p_i} = \vec{R}\times \sum_i \vec{p_i}$$
 
TSny said:
Looks right to me. The final result is more obvious if you write out explicitly that $$\sum_i \vec{R}\times \vec{p_i} = \vec{R}\times \sum_i \vec{p_i}$$

Got it, thanks a lot TSny! :smile:
 
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