Which of the following is the correct graph between gravitational field F on a particle with distance r due to a thin spherical shell of radius R ? (.r is measured from the centre of the spherical shell.)

Question

Which of the following is the correct graph between gravitational field F on a particle with distance r due to a thin spherical shell of radius R ? (.r is measured from the centre of the spherical shell.) (A) Option 1

(B)

(C)

(D)

Tardigrade Admin · Accepted Answer

Gravitational field due to the thin spherical shell. Inside the shell, F=0 ..(For r < R) On the surface of the shell, Solution

F=(G M/R2) For r=R Outside the shell, F=(G M/r2) â¦ (.For r>R.) The variation of F with distance r from the centre is as shown in the figure.

Q. Which of the following is the correct graph between gravitational field $F$ on a particle with distance $r$ due to a thin spherical shell of radius $R$ ? $(r i s m e a s u re d f ro m t h e ce n t re o f t h e s p h er i c a l s h e ll)$

Gravitational field due to the thin spherical shell.
Inside the shell,
$F = 0$ ..(For r < R)
On the surface of the shell,

$F = \frac{GM}{R ^{2}}$ For $r = R$
Outside the shell,
$F = \frac{GM}{r ^{2}}$ … $(F or r > R)$
The variation of F with distance r from the centre is as shown in the figure.

Q. Which of the following is the correct graph between gravitational field F on a particle with distance r due to a thin spherical shell of radius R ? (rismeasuredfromthecentreofthesphericalshell)

Gravitational field due to the thin spherical shell. Inside the shell, F=0 ..(For r < R) On the surface of the shell, F=R2GM​ For r=R Outside the shell, F=r2GM​ … (Forr>R) The variation of F with distance r from the centre is as shown in the figure.

Q. Which of the following is the correct graph between gravitational field $F$ on a particle with distance $r$ due to a thin spherical shell of radius $R$ ? $(r i s m e a s u re d f ro m t h e ce n t re o f t h e s p h er i c a l s h e ll)$

Gravitational field due to the thin spherical shell.
Inside the shell,
$F = 0$ ..(For r < R)
On the surface of the shell,

$F = \frac{GM}{R ^{2}}$ For $r = R$
Outside the shell,
$F = \frac{GM}{r ^{2}}$ … $(F or r > R)$
The variation of F with distance r from the centre is as shown in the figure.