Solveeit Logo

Question

Question: A spherical shell of radius \[R = 1.5\,{\text{cm}}\] has a charge \[q = 20\,\mu {\text{C}}\] uniform...

A spherical shell of radius R=1.5cmR = 1.5\,{\text{cm}} has a charge q=20μCq = 20\,\mu {\text{C}} uniformly distributed over it. The force exerted by one half over the other half is
A. zero
B. 102N{10^{ - 2}}\,{\text{N}}
C. 500N500\,{\text{N}}
D. 2000N2000\,{\text{N}}

Explanation

Solution

Use the equation for the electrostatic pressure exerted on the surface of the half portion of the shell. Use the value of surface charge density in this equation. Substitute the value of this derived equation in the equation for pressure to determine the force exerted by the half portion on the other half portion of the spherical shell.

Formulae used:
The electrostatic pressure PP exerted by charges on a surface is
P=σ22ε0\Rightarrow P = \dfrac{{{\sigma ^2}}}{{2{\varepsilon _0}}} …… (1)
Here, σ\sigma is the surface charge density and ε0{\varepsilon _0} is the permittivity of free space.
The surface charge density σ\sigma for a spherical surface is
σ=q4πR2\Rightarrow\sigma = \dfrac{q}{{4\pi {R^2}}} …… (2)
Here, qq is the charge distributed over the surface and RR is the radius of the sphere.
The pressure PP on an object is given by
P=FA\Rightarrow P = \dfrac{F}{A} …… (3)
Here, FF is the force on the object and AA is the area on which the force is applied.

Complete step by step solution:
We have given that the radius of the spherical shell is 1.5cm1.5\,{\text{cm}} and the charge which is uniformly distributed over the surface of shell is 20μC20\,\mu {\text{C}}.
R=1.5cm\Rightarrow R = 1.5\,{\text{cm}}
q=20μC\Rightarrow q = 20\,\mu {\text{C}}
Convert the unit of radius in the SI system of units.
R=(1.5cm)(102m1cm)\Rightarrow R = \left( {1.5\,{\text{cm}}} \right)\left( {\dfrac{{{{10}^{ - 2}}\,{\text{m}}}}{{1\,{\text{cm}}}}} \right)
R=1.5×102m\Rightarrow R = 1.5 \times {10^{ - 2}}\,{\text{m}}
Convert the unit of the charge in the SI system of units.
q=(20μC)(106C1μC)\Rightarrow q = \left( {20\,\mu {\text{C}}} \right)\left( {\dfrac{{{{10}^{ - 6}}\,{\text{C}}}}{{1\,\mu {\text{C}}}}} \right)
q=20×106C\Rightarrow q = 20 \times {10^{ - 6}}\,{\text{C}}
Hence, the charge distributed over the spherical shell is 20×106C20 \times {10^{ - 6}}\,{\text{C}}.
The force exerted by one half on the other half of the spherical shell is the force exerted by the inner half circular surface on the opposite half circular surface of the spherical shell.
Hence, the force is exerted on the circular area (πR2\pi {R^2}) of the shell.
Substitute σ22ε0\dfrac{{{\sigma ^2}}}{{2{\varepsilon _0}}} for PP and πR2\pi {R^2} for AA in equation (3).
σ22ε0=FπR2\Rightarrow\dfrac{{{\sigma ^2}}}{{2{\varepsilon _0}}} = \dfrac{F}{{\pi {R^2}}}
Rearrange the above equation for FF.
F=πR2σ22ε0\Rightarrow F = \dfrac{{\pi {R^2}{\sigma ^2}}}{{2{\varepsilon _0}}}
Substitute q4πR2\dfrac{q}{{4\pi {R^2}}} for σ\sigma in the above equation.
F=πR2(q4πR2)22ε0\Rightarrow F = \dfrac{{\pi {R^2}{{\left( {\dfrac{q}{{4\pi {R^2}}}} \right)}^2}}}{{2{\varepsilon _0}}}
F=q232πR2ε0\Rightarrow F = \dfrac{{{q^2}}}{{32\pi {R^2}{\varepsilon _0}}}
Substitute 20×106C20 \times {10^{ - 6}}\,{\text{C}} for qq, 3.143.14 for π\pi , 1.5×102m1.5 \times {10^{ - 2}}\,{\text{m}} for RR and 8.85×1012Fm - 18.85 \times {10^{ - 12}}\,{\text{F}} \cdot {{\text{m}}^{{\text{ - 1}}}} for ε0{\varepsilon _0} in the above equation.
F=(20×106C)232(3.14)(1.5×102m)2(8.85×1012Fm - 1)\Rightarrow F = \dfrac{{{{\left( {20 \times {{10}^{ - 6}}\,{\text{C}}} \right)}^2}}}{{32\left( {3.14} \right){{\left( {1.5 \times {{10}^{ - 2}}\,{\text{m}}} \right)}^2}\left( {8.85 \times {{10}^{ - 12}}\,{\text{F}} \cdot {{\text{m}}^{{\text{ - 1}}}}} \right)}}
F=2000N\therefore F = 2000\,{\text{N}}
Therefore, the force exerted by the one half on the other half is 2000N2000\,{\text{N}}.

Hence, the correct option is D.

Note: The students may think that force exerted on one half portion of the spherical shell on the other half portion is on the whole surface area of the half spherical shell. But the actual pressure is exerted on the area of the inner circular portion of the sphere only. Hence, while substituting in the pressure equation (3), the area should be substituted by the area of the circle on which the force is to be applied.