A nonuniform, but spherically symmetric, distribution of charge has a charge density ρ(r) given as follows:
ρ(r)=ρ0(1−r/R) | for r≤R |
ρ(r)=0 | for r≥R |
where ρ0=3Q/πR3 is a positive constant.
Part A
Find the total charge contained in the charge distribution.
Express your answer in terms of some or all of the variables r, R, Q, and appropriate constants.
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Part B
Obtain an expression for the electric field in the region r≥R.
Express your answer in terms of some or all of the variables r, R, Q, and appropriate constants.
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Part C
Obtain an expression for the electric field in the region r≤R.
Express your answer in terms of some or all of the variables r, R, Q, and appropriate constants.
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Part D
Find the value of r at which the electric field is maximum.
Express your answer in terms of some or all of the variables r, R, Q, and appropriate constants.
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Part E
Find the value of that maximum field.
Express your answer in terms of some or all of the variables r, R, Q, and appropriate constants.
A) We can consider an infinitely thin shell having thickness dr and surface area 4πr². The charge on that shell is
dQ = ρ(r)*A*dr = ρ0(1 - r/R)(4πr²)dr = 4π*ρ0(r² - r³/R)dr
which when integrated from 0 to r is
total charge = 4π*ρ0(r³/3 + r^4/(4R))
and when r = R our total charge is
total charge = 4π*ρ0(R³/3 + R³/4) = 4π*ρ0*R³/12 = π*ρ0*R³ / 3
and after substituting ρ0 = 3Q / πR³ we have
total charge = Q ◄
B) E = kQ/d²
since the distribution is symmetric spherically
C) dE = k*dq/r² = k*4π*ρ0(r² - r³/R)dr / r² = k*4π*ρ0(1 - r/R)dr
so
E(r) = k*4π*ρ0*(r - r²/(2R)) from zero to r is
and after substituting for ρ0 is
E(r) = k*4π*3Q(r - r²/(2R)) / πR³ = 12kQ(r/R³ - r²/(2R^4))
which could be expressed other ways.
D) dE/dr = 0 = 12kQ(1/R³ - r/R^4) means that
r = R for a min/max (and we know it's a max since r = 0 is a min).
E) E = 12kQ(R/R³ - R²/(2R^4)) = 12kQ / 2R² = 6kQ / R²
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