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Electrostatics question

2022 · Shift 2 · Q45
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Electrostatics question

2022 · Shift 2 · Q45

JEE AdvancedPhysicsElectrostaticsMultiple correct+4 / −2
In the figure, the inner (shaded) region AAA represents a sphere of radius rA=1r_{A}=1rA​=1, within which the electrostatic charge density varies with the radial distance rrr from the center as ρA=kr\rho_{A}=k rρA​=kr, where kkk is positive. In the spherical shell BBB of outer radius rBr_{B}rB​, the electrostatic charge density varies as ρB=2kr\rho_{B}=\frac{2 k}{r}ρB​=r2k​. Assume that dimensions are taken care of. All physical quantities are in their SI units. JEE Advanced 2022 Paper 2 Online Physics - Electrostatics Question 25 English Which of the following statement(s) is(are) correct?
  1. A
    If rB=32r_{B}=\sqrt{\frac{3}{2}}rB​=23​​, then the electric field is zero everywhere outside BBB.
  2. B
    If rB=32r_{B}=\frac{3}{2}rB​=23​, then the electric potential just outside BBB is kϵ0\frac{k}{\epsilon_{0}}ϵ0​k​.
  3. C
    If rB=2r_{B}=2rB​=2, then the total charge of the configuration is 15πk15 \pi k15πk.
  4. D
    If rB=52r_{B}=\frac{5}{2}rB​=25​, then the magnitude of the electric field just outside BBB is 13πkϵ0\frac{13 \pi k}{\epsilon_{0}}ϵ0​13πk​.
View written solutionFree

Correct answer: B

The user wants me to solve a physics problem about electrostatics. I need to evaluate four statements regarding a spherically symmetric charge distribution.

The charge distribution is defined in two regions:

  1. Region A (inner sphere): For 0≤r≤rA=10 \le r \le r_A=10≤r≤rA​=1, the charge density is ρA(r)=kr\rho_A(r) = krρA​(r)=kr.
  2. Region B (spherical shell): For rA=1≤r≤rBr_A=1 \le r \le r_BrA​=1≤r≤rB​, the charge density is ρB(r)=2kr\rho_B(r) = \frac{2k}{r}ρB​(r)=r2k​.

I will first calculate the total charge of the configuration and then use it to find the electric field and potential outside the sphere, which will allow me to check each statement.

Step 1: Calculate the charge in Region A (QAQ_AQA​)

The charge QAQ_AQA​ in the inner sphere (from r=0r=0r=0 to rA=1r_A=1rA​=1) is found by integrating the charge density over the volume. The volume element is dV=4πr2drdV = 4\pi r^2 drdV=4πr2dr. QA=∫0rAρA(r)dV=∫01(kr)(4πr2)drQ_A = \int_{0}^{r_A} \rho_A(r) dV = \int_{0}^{1} (kr) (4\pi r^2) drQA​=∫0rA​​ρA​(r)dV=∫01​(kr)(4πr2)dr QA=4πk∫01r3dr=4πk[r44]01Q_A = 4\pi k \int_{0}^{1} r^3 dr = 4\pi k \left[ \frac{r^4}{4} \right]_{0}^{1}QA​=4πk∫01​r3dr=4πk[4r4​]01​ QA=4πk(144−0)=πkQ_A = 4\pi k \left( \frac{1^4}{4} - 0 \right) = \pi kQA​=4πk(414​−0)=πk

Step 2: Calculate the charge in Region B (QBQ_BQB​)

The charge QBQ_BQB​ in the spherical shell (from r=rA=1r=r_A=1r=rA​=1 to rBr_BrB​) is: QB=∫rArBρB(r)dV=∫1rB(2kr)(4πr2)drQ_B = \int_{r_A}^{r_B} \rho_B(r) dV = \int_{1}^{r_B} \left(\frac{2k}{r}\right) (4\pi r^2) drQB​=∫rA​rB​​ρB​(r)dV=∫1rB​​(r2k​)(4πr2)dr QB=8πk∫1rBrdr=8πk[r22]1rBQ_B = 8\pi k \int_{1}^{r_B} r dr = 8\pi k \left[ \frac{r^2}{2} \right]_{1}^{r_B}QB​=8πk∫1rB​​rdr=8πk[2r2​]1rB​​ QB=4πk(rB2−12)=4πk(rB2−1)Q_B = 4\pi k (r_B^2 - 1^2) = 4\pi k (r_B^2 - 1)QB​=4πk(rB2​−12)=4πk(rB2​−1)

Step 3: Calculate the total charge of the configuration (QtotalQ_{total}Qtotal​)

The total charge is the sum of the charges in both regions: Qtotal=QA+QB=πk+4πk(rB2−1)Q_{total} = Q_A + Q_B = \pi k + 4\pi k (r_B^2 - 1)Qtotal​=QA​+QB​=πk+4πk(rB2​−1) Qtotal=πk(1+4rB2−4)=πk(4rB2−3)Q_{total} = \pi k (1 + 4r_B^2 - 4) = \pi k (4r_B^2 - 3)Qtotal​=πk(1+4rB2​−4)=πk(4rB2​−3)

Step 4: Evaluate each statement

For a spherically symmetric charge distribution, the electric field and potential outside the distribution (for r>rBr > r_Br>rB​) are given by: E(r)=14πϵ0Qtotalr2E(r) = \frac{1}{4\pi \epsilon_0} \frac{Q_{total}}{r^2}E(r)=4πϵ0​1​r2Qtotal​​ V(r)=14πϵ0Qtotalr(assuming V(∞)=0)V(r) = \frac{1}{4\pi \epsilon_0} \frac{Q_{total}}{r} \quad (\text{assuming } V(\infty)=0)V(r)=4πϵ0​1​rQtotal​​(assuming V(∞)=0)

A: If rB=32r_{B}=\sqrt{\frac{3}{2}}rB​=23​​, then the electric field is zero everywhere outside BBB. The electric field is zero outside B only if Qtotal=0Q_{total} = 0Qtotal​=0. Let's calculate QtotalQ_{total}Qtotal​ for rB=3/2r_B = \sqrt{3/2}rB​=3/2​: Qtotal=πk(4(32)2−3)=πk(4(32)−3)=πk(6−3)=3πkQ_{total} = \pi k \left( 4\left(\sqrt{\frac{3}{2}}\right)^2 - 3 \right) = \pi k \left( 4\left(\frac{3}{2}\right) - 3 \right) = \pi k (6 - 3) = 3\pi kQtotal​=πk(4(23​​)2−3)=πk(4(23​)−3)=πk(6−3)=3πk Since kkk is positive, Qtotal=3πk≠0Q_{total} = 3\pi k \neq 0Qtotal​=3πk=0. Thus, the statement is incorrect. In fact, since rB>rA=1r_B > r_A=1rB​>rA​=1, both QA=πkQ_A = \pi kQA​=πk and QB=4πk(rB2−1)Q_B = 4\pi k (r_B^2 - 1)QB​=4πk(rB2​−1) are positive. So QtotalQ_{total}Qtotal​ can never be zero.

B: If rB=32r_{B}=\frac{3}{2}rB​=23​, then the electric potential just outside BBB is kϵ0\frac{k}{\epsilon_{0}}ϵ0​k​. First, calculate QtotalQ_{total}Qtotal​ for rB=3/2r_B = 3/2rB​=3/2: Qtotal=πk(4(32)2−3)=πk(4(94)−3)=πk(9−3)=6πkQ_{total} = \pi k \left( 4\left(\frac{3}{2}\right)^2 - 3 \right) = \pi k \left( 4\left(\frac{9}{4}\right) - 3 \right) = \pi k (9 - 3) = 6\pi kQtotal​=πk(4(23​)2−3)=πk(4(49​)−3)=πk(9−3)=6πk Now, calculate the potential just outside B, i.e., at r=rB=3/2r=r_B=3/2r=rB​=3/2: V(rB)=14πϵ0QtotalrB=14πϵ06πk3/2V(r_B) = \frac{1}{4\pi \epsilon_0} \frac{Q_{total}}{r_B} = \frac{1}{4\pi \epsilon_0} \frac{6\pi k}{3/2}V(rB​)=4πϵ0​1​rB​Qtotal​​=4πϵ0​1​3/26πk​ V(rB)=6πk4πϵ0(3/2)=6k6ϵ0=kϵ0V(r_B) = \frac{6\pi k}{4\pi \epsilon_0 (3/2)} = \frac{6k}{6\epsilon_0} = \frac{k}{\epsilon_0}V(rB​)=4πϵ0​(3/2)6πk​=6ϵ0​6k​=ϵ0​k​ This matches the statement. Thus, the statement is correct.

C: If rB=2r_{B}=2rB​=2, then the total charge of the configuration is 15πk15 \pi k15πk. Calculate QtotalQ_{total}Qtotal​ for rB=2r_B=2rB​=2: Qtotal=πk(4(2)2−3)=πk(4(4)−3)=πk(16−3)=13πkQ_{total} = \pi k (4(2)^2 - 3) = \pi k (4(4) - 3) = \pi k (16 - 3) = 13\pi kQtotal​=πk(4(2)2−3)=πk(4(4)−3)=πk(16−3)=13πk The statement claims the total charge is 15πk15\pi k15πk. This is different from our calculated value. Thus, the statement is incorrect.

D: If rB=52r_{B}=\frac{5}{2}rB​=25​, then the magnitude of the electric field just outside BBB is 13πkϵ0\frac{13 \pi k}{\epsilon_{0}}ϵ0​13πk​. First, calculate QtotalQ_{total}Qtotal​ for rB=5/2r_B=5/2rB​=5/2: Qtotal=πk(4(52)2−3)=πk(4(254)−3)=πk(25−3)=22πkQ_{total} = \pi k \left( 4\left(\frac{5}{2}\right)^2 - 3 \right) = \pi k \left( 4\left(\frac{25}{4}\right) - 3 \right) = \pi k (25 - 3) = 22\pi kQtotal​=πk(4(25​)2−3)=πk(4(425​)−3)=πk(25−3)=22πk Now, calculate the electric field magnitude just outside B, i.e., at r=rB=5/2r=r_B=5/2r=rB​=5/2: E(rB)=14πϵ0QtotalrB2=14πϵ022πk(5/2)2E(r_B) = \frac{1}{4\pi \epsilon_0} \frac{Q_{total}}{r_B^2} = \frac{1}{4\pi \epsilon_0} \frac{22\pi k}{(5/2)^2}E(rB​)=4πϵ0​1​rB2​Qtotal​​=4πϵ0​1​(5/2)222πk​ E(rB)=22πk4πϵ0(25/4)=22k25ϵ0E(r_B) = \frac{22\pi k}{4\pi \epsilon_0 (25/4)} = \frac{22k}{25\epsilon_0}E(rB​)=4πϵ0​(25/4)22πk​=25ϵ0​22k​ The statement claims the magnitude is 13πkϵ0\frac{13 \pi k}{\epsilon_{0}}ϵ0​13πk​. This does not match our calculated value. Thus, the statement is incorrect.

Conclusion

Based on the step-by-step evaluation, only statement B is correct.

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