Question 26
A solid metal sphere
of radius R is isolated in space.
The sphere is positively charged so that the electric potential at its surface
is VS.
The electric field strength at the surface is ES.
(a)
On the axes of Fig. 6.1, show the variation of the electric
potential with distance x from the centre of the
sphere for values of x from x
= 0 to x = 3R.
Fig. 6.1
[3]
(b)
On the axes of Fig. 6.2, show the variation of the electric field
strength with distance x from the centre of the
sphere for values of x from x
= 0 to x = 3R.
Fig. 6.2
[3]
[Total: 6]
Reference: Past Exam Paper – June 2012 Paper 41 & 43 Q6
Solution:
(a)
sketch: from
x = 0 to x = R, potential is constant at VS
smooth curve
through (R, VS) and (2R, 0.5VS)
smooth curve
continues to (3R, 0.33VS)
{Electric
potential: V = Q / 4πϵ0x where x is the
distance from the centre
For a
conductor, the potential is constant inside the sphere. So, from x = 0 to x = R
(that is, inside the sphere), potential = VS and is constant. This
is a horizontal line in the graph.
Hence, we
also have the point (R, VS).
VS
= Q / 4πϵ0R
From the
equation for potential above, the potential V is inversely proportional to x.
The greater the value of x, the smaller the potential.
V = Q / 4πϵ0x
When x = R, V
= Q / 4πϵ0R = VS
When x = 2R,
V = Q / 4πϵ0(2R) = ½ VS (2R, 0.5 VS)
When x = 3R,
V = Q / 4πϵ0(3R) = 1/3 VS (2R, 0.33 VS)
}
(b)
sketch: from
x = 0 to x = R, field strength is zero
smooth curve
through (R, E) and (2R, 0.25E)
smooth curve
continues to (3R, 0.11E)
{Electric field
strength: E = Q / 4πϵ0x2 where x
is the distance from the centre
For a
conductor, the field strength is zero inside the sphere. So, from x = 0 to x =
R (that is, inside the sphere), field strength = zero. This is a horizontal
line in the graph.
At the
surface of the sphere, the field strength is maximum. This is the point (R, 1.0
ES).
From the
equation for field strength above, the field strength E is inversely
proportional to x2. The greater the value of x, the smaller the
potential.
E = Q / 4πϵ0x2
When x = R, E
= Q / 4πϵ0R2
= ES (R, ES)
When x = 2R,
E = Q / 4πϵ0(2R)2
= ¼ ES (R, 0.25ES)
When x = 3R,
E = Q / 4πϵ0(3R)2
= 1/9 ES (R, 0.11ES)
}
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