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10:07 AM
Hi @JohnRennie. I wanted to ask something.
 
10:23 AM
@Abcd Morning :-)
 
@JohnRennie Finding the force due to the ring (and then using newton's third law) and considering the sphere as a point mass helps
But then, directly finding the force on the ring due to the sphere which can be treated as a point mass doesn't help. (without using Newton's third law. )
 
Isn't it just a matter of calculating the force on an element of the ring then integrating round the ring?
 
yes, but how? i wasn't getting the right answer using that.
 
Give me a moment and I'll draw a diagram ...
 
No
I have a diagram.
Let me send
Here @JohnRennie ^
let's treat the sphere as a point of mass M placed at its centre, using shell theorem.
 
10:32 AM
 
Ok
 
Ha. Just beat me to it :-)
 
yeah :).
1 min ago, by Abcd
let's treat the sphere as a point of mass M placed at its centre, using shell theorem.
 
If we consider an element of the ring subtending an angle $d\theta$ then its mass is $md\theta/2\pi$, so the force is $dF = \frac{GM md\theta}{4a^2 2\pi}$
 
@JohnRennie where does it subtend $d\theta$?
 
10:38 AM
That's the top view of the ring so we are looking down on the ring and the sphere is below it.
We consider a small element of the ring subtending an angle $d\theta$ measured from the centre of the ring.
 
ok
now integration gives: $F = \dfrac{GMm}{4a^2}$?
 
No, because force is a vector. You can't just sum the magnitudes of the $dF$ s
 
right.
we need $\hat{j}$ components of force, from symmetry.
 
If we go back to the side view, there will be a component of the force that acts horizontally inwards towards the centre of the ring. When we integrate this component will sum to zero.
 
yes
 
10:45 AM
So we just integrate the vertical component, which I guess is what you mean by the $j$ component.
 
yes
Oh, then we'll have to use another angle.
Then, after that cosine rule.
Wait, i/m slightly uncertain.
 
It's just going to add a factor of $1/\sqrt{3}$
 
What about $\theta$ @JohnRennie? Were's it.
 
Theta is the angle measured from the centre of the ring to the edge of the ring. It integrates from 0 to $2\pi$ to go round the ring.
 
Ok.
 
10:50 AM
$dF_v = \frac{GM md\theta}{4a^2 2\pi} \cos\phi$
 
yes
 
And nothing in that equation is a function of $\theta$ so integration gives $$F_v = \frac{GM m}{4a^2 2\pi} \cos\phi \int_0^{2\pi} d\theta $$
 
yes, and $\cos \phi = \dfrac{\sqrt 3}{2}$
Done @JohnRennie. Thank you :).
 

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