Undergrad Why is the first term zero in the Virial Theorem derivation?

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The discussion centers on the derivation of the Virial Theorem, specifically addressing why the first term in the equation goes to zero. Participants clarify that due to Newton's Third Law, the forces between pairs of particles cancel each other out, leading to the first term being zero. The symmetry in the forces, where the force from particle i to j is equal in magnitude and opposite in direction to the force from j to i, is crucial to this cancellation. However, the second term does not go to zero because the vector difference between the positions of the particles changes sign when the indices are exchanged. This understanding highlights the importance of both symmetry and directionality in the derivation.
rexregisanimi
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Hello everyone! I am reviewing the derivation of the Virial Theorem from an introductory Astrophysics book (Carroll and Ostlie's) and found a step I couldn't follow. I've attached a photo of the step.

Can anyone explain how Newton's Third Law brings about eqn 2.41? I don't see how that first term in the right side previous to eqn 2.41 goes to zero. What symmetry is being referenced?

1482184447251.jpg
 
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Consider the ##ij##-th term
$$
\mathbf F_{ij} \cdot (\mathbf r_i + \mathbf r_j)
$$
and the ##ji##-th term
$$
\mathbf F_{ji} \cdot (\mathbf r_j + \mathbf r_i) = -\mathbf F_{ij} \cdot (\mathbf r_i + \mathbf r_j)
$$
The two terms has equal magnitude but opposite sign, so they will cancel. The same is true for other pair of terms connected by interchanging the indices.
 
So, in other words, the top triangular part of the F_ij matrix cancels with the bottom triangular part because of the Third Law; this leaves the diagonals only which are zero because a particle will not exert a force on itself. Is that correct?
 
You actually don't sum the vector F_ij, instead you are summing over the component of F_ij along the position vector of the central point in the line connecting the two particles.
 
Thank you for your replies.

Why then isn't the second term zero? If we're just concerned about those values, shouldn't both terms go to zero?
 
rexregisanimi said:
Thank you for your replies.

Why then isn't the second term zero? If we're just concerned about those values, shouldn't both terms go to zero?
When you exchange the indices, the vector ##\mathbf r_i - \mathbf r_j## also changes sign.
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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