Two infinite identical charged sheets and a charged spherical body of charge density ' $\rho$ ' are arranged as shown in figure. Then the correct relation between the electrical fields at $\mathrm{A}, \mathrm{B}, \mathrm{C}$ and D points is:
\( |E_A| = |E_B|; \; E_C > E_D \)
$\left|\vec{E}_{A}\right|=\left|\vec{E}_{B}\right| ; \vec{E}_{C}>\vec{E}_{D}$
We are given two infinite identical charged sheets and a charged spherical body of charge density \( \rho \). We are to find the correct relation between the electric fields at points A, B, C, and D as shown in the figure.
For an infinite plane sheet of charge density \( \sigma \), the electric field near it is given by:
\[ E = \frac{\sigma}{2\varepsilon_0} \]
The direction of the field is away from the sheet if \( \sigma > 0 \) (positive charge) and toward the sheet if \( \sigma < 0 \) (negative charge).
For a uniformly charged non-conducting solid sphere of charge density \( \rho \):
Step 1: Analyze the field due to the two infinite sheets.
Step 2: Now include the effect of the charged spherical body.
The sphere creates an additional electric field directed radially outward since it has positive charge density \( \rho \).
Step 3: Combine all effects.
Hence, inside the region between sheets, both A and B have small but similar fields (mostly due to the sphere), while outside, D has a stronger net field than C.
Therefore, the correct relation between the electric fields is:
\[ |E_A| = |E_B|; \quad E_C > E_D \]
Final Answer: Option (3) \( |E_A| = |E_B|; \; E_C > E_D \)