Proving Magnitude of Centre of Mass Vector Equation

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Homework Help Overview

The discussion revolves around proving the magnitude of the center of mass vector equation, specifically the relationship involving the position vector for the center of mass from an arbitrary origin. The original poster presents an equation and expresses difficulty in deriving the required result from the definition of the center of mass.

Discussion Character

  • Exploratory, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss working backwards from the definitions and relationships involved in the equation. There are mentions of summation rules and concepts that some participants feel are outdated. One participant outlines a method involving squaring the center of mass equation and manipulating terms related to the position vectors.

Discussion Status

The discussion is active, with participants exploring various approaches to the problem. One participant has provided a detailed breakdown of the mathematical reasoning, while others are engaging with the concepts and expressing their uncertainties about summation techniques.

Contextual Notes

Some participants indicate a lack of familiarity with certain mathematical concepts, such as summation rules and number theory, which may affect their ability to follow the discussion fully.

Reshma
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Prove that the magnitude of R of the position vector for the centre of mass from an arbitrary origin is given by the equation:
M^2R^2 = M\sum m_ir_i^2 - {1\over 2}\sum m_i m_j r_{ij}^2

Well the centre of mass is given by:
\vec R = \frac{\sum m_i r_i}{M}

But squaring this doesn't seem to produce the result I require. I need more help.
 
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I'm not too sure about this but I think it should work if you start working backwards - from the definition of rij2, then multiply by -0.5mimj and then sum over the indices. My summation rules are a bit rusty. :redface:
 
Last edited:
Work backwards? I will try that. My summation concepts are pretty outdated too. Got to relocate my high school number theory text.
 
This is quite straightforward. Let's start with:

M\vec{R} = \sum_i m_i \vec{r}_i

Square it:

M^2 R^2 = \sum_{i,j} m_i m_j \vec{r}_i \cdot \vec{r}_j \qquad (1)

Then consider \vec{r}_{i j} \equiv \vec{r}_i - \vec{r}_j \Longleftrightarrow r^2_{ij} = (\vec{r}_i - \vec{r}_j)^2 = r^2_i - 2 \vec{r}_i \cdot \vec{r}_j + r^2_j \Longleftrightarrow \vec{r}_i \cdot \vec{r}_j = \frac{1}{2}(r^2_i+r^2_j-r^2_{ij})

Insert the last relationship in (1) and you'll obtain:

M^2 R^2 = \frac{1}{2} \sum_{i,j} m_i m_j (r^2_i+r^2_j-r^2_{ij}) = \frac{1}{2} \sum_{i,j} m_i m_j (r^2_i+r^2_j) - \frac{1}{2} \sum_i m_i m_j r^2_{ij} \qquad (2)

Now, consider the first term of (2)'s rhs:

\frac{1}{2} \sum_{i,j} m_i m_j (r^2_i+r^2_j) = \frac{1}{2}\sum_i m_i \left[\sum_j m_j (r^2_i + r^2_j) \right] = \frac{1}{2} \sum_i m_i \left[\sum_j m_j r^2_i + \sum_j m_j r^2_j \right] \qquad (3)

But \sum_j m_j r^2_i = M r^2_i so:

\frac{1}{2} \sum_i m_i \left[\sum_j m_j r^2_i + \sum_j m_j r^2_j \right] = \frac{1}{2} \sum_i m_i \left[ M r^2_i + \sum_j m_j r^2_j \right] = \frac{1}{2} \left[ M \sum_i m_i r^2_i + \sum_i m_i \sum_j m_j r^2_j \right] = \frac{1}{2} \left[ M \sum_i m_i r^2_i + M \sum_j m_j r^2_j \right] =

= \frac{1}{2} M \left[ \sum_i m_i r^2_i + \sum_j m_j r^2_j \right]

Because "j" is a summed index, you can call it "i" so (3) becomes:

\frac{1}{2} \sum_{i,j} m_i m_j (r^2_i+r^2_j) = \frac{1}{2} M \left[ \sum_i m_i r^2_i + \sum_i m_i r^2_i \right] = M \sum_i m_i r^2_i \qquad (3)

Finally, just insert rhs of (3) in (2) and that's it :smile:
 
Last edited:
Very nicely done, Emanuel. :approve:
 
Bravo, Emanuel! :smile:
 

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