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Question: In space, a region centered at origin contains charge such that electric potential (V) varies with r...

In space, a region centered at origin contains charge such that electric potential (V) varies with radial distance (r) as V = ar³ + ar². The magnitude of charge density (ρ) at radial distance r = 1 unit is Nα∈₀ then N is ______. (∈₀ is electric permittivity)

Answer

18

Explanation

Solution

The electric potential is given by V=ar3+ar2V = ar^3 + ar^2. The electric field E\vec{E} is related to the potential by E=V\vec{E} = -\nabla V. In spherical coordinates, for a potential that depends only on the radial distance r, the electric field is radial and its magnitude is given by Er=dVdrE_r = -\frac{dV}{dr}. Er=ddr(ar3+ar2)=(3ar2+2ar)E_r = -\frac{d}{dr}(ar^3 + ar^2) = -(3ar^2 + 2ar).

The charge density ρ\rho is related to the electric field by Gauss's law in differential form, E=ρ0\nabla \cdot \vec{E} = \frac{\rho}{\in_0}. In spherical coordinates, for a spherically symmetric electric field E=Er(r)r^\vec{E} = E_r(r) \hat{r}, the divergence is E=1r2r(r2Er)\nabla \cdot \vec{E} = \frac{1}{r^2} \frac{\partial}{\partial r}(r^2 E_r). First, calculate r2Err^2 E_r: r2Er=r2(3ar22ar)=3ar42ar3r^2 E_r = r^2 (-3ar^2 - 2ar) = -3ar^4 - 2ar^3. Next, calculate r(r2Er)\frac{\partial}{\partial r}(r^2 E_r): r(3ar42ar3)=12ar36ar2\frac{\partial}{\partial r}(-3ar^4 - 2ar^3) = -12ar^3 - 6ar^2. Now, calculate the divergence: E=1r2(12ar36ar2)=12ar6a\nabla \cdot \vec{E} = \frac{1}{r^2}(-12ar^3 - 6ar^2) = -12ar - 6a.

Using Gauss's law, the charge density is: ρ(r)=0(E)=0(12ar6a)\rho(r) = \in_0 (\nabla \cdot \vec{E}) = \in_0 (-12ar - 6a).

We need to find the magnitude of the charge density at radial distance r = 1 unit. ρ(r=1)=0(12a(1)6a)=0(12a6a)=18a0\rho(r=1) = \in_0 (-12a(1) - 6a) = \in_0 (-12a - 6a) = -18a\in_0. The magnitude of the charge density at r=1 is ρ(r=1)=18a0=18a0|\rho(r=1)| = |-18a\in_0| = 18|a|\in_0.

The problem states that the magnitude of charge density at radial distance r = 1 unit is Nα∈₀. So, we have the equation: 18a0=Nα018|a|\in_0 = Nα∈₀.

For N to be a specific numerical value independent of the constants 'a' and 'α', it is implied that the constant 'a' used in the potential function is the same as the constant 'α' mentioned in the expression for the magnitude of charge density. Let's assume a=αa = \alpha. Then the equation becomes: 18α0=Nα018|\alpha|\in_0 = Nα∈₀.

The expression Nα∈₀ represents the magnitude of the charge density, so it must be non-negative. Since 0\in_0 is positive, Nα must be non-negative. If α>0\alpha > 0, then α=α|\alpha| = \alpha. The equation is 18α0=Nα018\alpha\in_0 = N\alpha\in_0. Assuming α0\alpha \neq 0 and 00\in_0 \neq 0, we can divide by α0\alpha\in_0 to get 18=N18 = N. If α<0\alpha < 0, then α=α|\alpha| = -\alpha. The equation is 18(α)0=Nα018(-\alpha)\in_0 = N\alpha\in_0. Dividing by α0\alpha\in_0 (assuming α0\alpha \neq 0 and 00\in_0 \neq 0), we get 18=N-18 = N. However, if α<0\alpha < 0, then Nα must be non-negative, which requires N to be non-positive. N=18N = -18 fits this condition. If α=0\alpha = 0, then V=0V=0, ρ=0\rho=0, and the magnitude is 0. Nα0=0N\alpha\in_0 = 0, which is true for any N. But the problem describes a region containing charge, implying ρ0\rho \neq 0, so a0a \neq 0, and thus α0\alpha \neq 0.

Given that the question asks for a single integer value of N without specifying the sign of α, the most likely interpretation is that N is the positive factor multiplying α0|\alpha|\in_0, or that α is assumed to be positive, or that the problem implicitly defines α as a|a|. If the magnitude is Nα0N|\alpha|\in_0, then 18a0=Nα018|a|\in_0 = N|\alpha|\in_0. If a=αa=\alpha, then 18α0=Nα018|\alpha|\in_0 = N|\alpha|\in_0, which gives N=18N=18 (provided α0\alpha \neq 0). This yields a unique positive integer value for N.

Let's assume the convention that the constant 'a' in the potential is the same as 'α' in the expression for magnitude, and the magnitude is given as Nα0N|\alpha|\in_0. Then 18α0=Nα018|\alpha|\in_0 = N|\alpha|\in_0. N=18N = 18.

Alternatively, if the problem statement "magnitude of charge density (ρ) at radial distance r = 1 unit is Nα∈₀" is interpreted strictly, it means ρ(1)=Nα0|\rho(1)| = N\alpha\in_0. We found ρ(1)=18a0|\rho(1)| = 18|a|\in_0. So, 18a0=Nα018|a|\in_0 = N\alpha\in_0. If we assume a=αa=\alpha and α>0\alpha > 0, then 18α0=Nα018\alpha\in_0 = N\alpha\in_0, so N=18N=18. If we assume a=αa=\alpha and α<0\alpha < 0, then 18(α)0=Nα018(-\alpha)\in_0 = N\alpha\in_0, so 18=N-18 = N. In this case, Nα=(18)(β)=18β=18αN\alpha = (-18)(-\beta) = 18\beta = 18|\alpha|, which is positive, consistent with the magnitude. However, integer type questions usually expect a non-negative integer unless otherwise specified. The most standard interpretation in such physics problems is that the constant α is positive or that N represents the positive numerical factor. Let's assume N is the positive numerical factor such that the magnitude is Na0N|a|\in_0 where aa is the constant in the potential, and the problem uses α to denote this constant aa. So, 18a0=Na018|a|\in_0 = N|a|\in_0. This gives N=18N=18.

The final answer is 18\boxed{18}.

Explanation of the solution:

  1. Calculate the electric field Er(r)E_r(r) from the given potential V(r)=ar3+ar2V(r) = ar^3 + ar^2 using Er=dVdrE_r = -\frac{dV}{dr}.
  2. Calculate the charge density ρ(r)\rho(r) from the electric field using Gauss's law in differential form ρ=0E\rho = \in_0 \nabla \cdot \vec{E}. For a spherically symmetric field, E=1r2r(r2Er)\nabla \cdot \vec{E} = \frac{1}{r^2} \frac{\partial}{\partial r}(r^2 E_r).
  3. Evaluate the charge density at r=1 unit: ρ(1)\rho(1).
  4. Calculate the magnitude of the charge density at r=1 unit: ρ(1)|\rho(1)|.
  5. Equate this magnitude to the given expression Nα0Nα∈₀ and solve for N, assuming the constant 'a' in the potential is the same as 'α' in the expression for the magnitude, and N is the positive numerical factor.

Calculation: V=ar3+ar2V = ar^3 + ar^2 Er=ddr(ar3+ar2)=(3ar2+2ar)E_r = -\frac{d}{dr}(ar^3 + ar^2) = -(3ar^2 + 2ar) ρ(r)=01r2r(r2Er)=01r2r(r2(3ar22ar))\rho(r) = \in_0 \frac{1}{r^2} \frac{\partial}{\partial r}(r^2 E_r) = \in_0 \frac{1}{r^2} \frac{\partial}{\partial r}(r^2 (-3ar^2 - 2ar)) ρ(r)=01r2r(3ar42ar3)=01r2(12ar36ar2)=0(12ar6a)\rho(r) = \in_0 \frac{1}{r^2} \frac{\partial}{\partial r}(-3ar^4 - 2ar^3) = \in_0 \frac{1}{r^2}(-12ar^3 - 6ar^2) = \in_0 (-12ar - 6a) At r=1, ρ(1)=0(12a6a)=18a0\rho(1) = \in_0 (-12a - 6a) = -18a\in_0. Magnitude ρ(1)=18a0=18a0|\rho(1)| = |-18a\in_0| = 18|a|\in_0. Given magnitude is Nα0Nα∈₀. Assuming a=αa=\alpha, magnitude is 18α018|\alpha|\in_0. Equating 18α0=Nα018|\alpha|\in_0 = Nα∈₀. If we interpret Nα0Nα∈₀ as Nα0N|\alpha|\in_0, then 18α0=Nα018|\alpha|\in_0 = N|\alpha|\in_0, which gives N=18N=18. If we interpret Nα0Nα∈₀ literally, then 18α0=Nα018|\alpha|\in_0 = Nα∈₀. If α>0\alpha>0, 18α0=Nα0    N=1818\alpha\in_0 = N\alpha\in_0 \implies N=18. If α<0\alpha<0, 18(α)0=Nα0    18α0=Nα0    N=1818(-\alpha)\in_0 = N\alpha\in_0 \implies -18\alpha\in_0 = N\alpha\in_0 \implies N=-18. Since the question asks for N as a positive integer often the case in "N is ____" questions, and magnitude is positive, the standard interpretation leads to N=18.