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New answer posted

3 months ago

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R
Raj Pandey

Contributor-Level 9

at point P,

= K E P + P E P

= 1 2 m v P 2 + { G M 1 m ( r / 2 ) G M 2 m r / 2 }

at infinity (ie for escaping from both masses)

v P = 4 G ( M 1 + M 2 ) r

New answer posted

3 months ago

0 Follower 3 Views

V
Vishal Baghel

Contributor-Level 10

U = G m ( M m ) d * 4 + 2 x ( G m 2 2 d )

For Umax

d U d m = 0 m = M 2 M m = 2

New answer posted

3 months ago

0 Follower 1 View

V
Vishal Baghel

Contributor-Level 10

Inside a uniform spherical shell, electric field is zero every where & electric potential is constant but not zero, every where

New answer posted

3 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

g 1 = G M ( R + h ) 2

g 1 = g ( 1 + h R ) 2

Given h = D = 2R

g 1 = g ( 1 + 2 R R ) 2

g 1 = g 9

New answer posted

3 months ago

0 Follower 3 Views

P
Payal Gupta

Contributor-Level 10

m = 1kg ; ΔU=Gmem (R+h) (GmemR)

ΔU=GMmRGMmR+h

=mg0Rmg0R (1+hR)=mg0 {11 (1+3RR)}

=mg0R (34)

=34*1*10*6400km

=48000*103J.

=48MJ.

New answer posted

3 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

The law of gravitation holds good for any pair of bodies in the universe.

This is correct statement.

The weight of any person becomes zero when the person is at the centre of the Earth.

Weight = mg

= m * 0 [g = 0 at the centre of the Earth]

= 0

New answer posted

3 months ago

0 Follower 5 Views

V
Vishal Baghel

Contributor-Level 10

F on P =  G M M r 2 + 2 G M M ( 2 r ) 2

F o n P = G * 1 0 4 1 3 2 ( 1 + 1 2 ) 1 0 0 G

New answer posted

3 months ago

0 Follower 3 Views

A
alok kumar singh

Contributor-Level 10

 

E A E B = G M m A 2 * 3 r G M m B 2 * 4 r = m A m B * 4 3 = 4 3 * 4 3 = 1 6 9

New answer posted

3 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

g = G M r 2

d g = 2 G M r 3 d r

d g * 1 0 0 = 2 ( G M r 2 ) d r r * 1 0 0

d g g * 1 0 0 = 2 * 2 ? = 4 %

New answer posted

3 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

g ( a t h ) = g ( a t d e p t h α h ) h << R

g ( 1 2 h R ) = g ( 1 α h R )

1 2 h R = 1 α h R 2 h R = α h R α = 2

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