Analyzing the Setup
Imagine a parallel plate capacitor where the negative plate is positioned at x=0 and the positive plate is at x=3d
Right in the middle of this setup, spanning from x=d to x=2d, we place a dielectric slab of thickness d. This creates three distinct regions: an air gap, a dielectric medium, and another air gap.
The Electric Field
Let's first think about the electric field
We know from fundamental electrostatics that electric field lines always originate from positive charges and terminate at negative charges. Since our positive plate is at x=3d and the negative plate is at x=0, the electric field must point from right to left. In vector terms, it points in the −x direction everywhere between the plates.
What about its magnitude? In the air gaps (0<x<d and 2d<x<3d), the electric field has a constant magnitude, let's call it E0. However, inside the dielectric slab (d<x<2d), the material gets polarized. This polarization creates an internal electric field that opposes the external one, effectively weakening the net electric field to E0/K, where K is the dielectric constant.
So, while the magnitude of the electric field drops inside the dielectric, its direction remains strictly unchanged. This confirms that option (b) is correct and option (a) is incorrect.
The Electric Potential
Now, let's analyze the electric potential V
The relationship between the electric field and the potential is given by the gradient equation:
Rearranging this, we get:
Since we established that the electric field E is negative everywhere (pointing in the −x direction), the term −E is always positive. Therefore, for any forward step dx>0, the change in potential dV is strictly positive.
Physically, this makes perfect sense: as you move from x=0 to x=3d, you are walking from the negative plate (lower potential) towards the positive plate (higher potential). You are moving against the electric field lines, which means you are climbing up the potential hill. The potential increases continuously across all three regions. The only difference is that the rate of increase (the slope of the V−x graph) is slightly less steep inside the dielectric because the electric field is weaker there.
Conclusion
To summarize, the introduction of the dielectric slab alters the magnitude of the electric field but preserves its direction
Furthermore, traversing from the negative to the positive plate guarantees a continuous increase in electric potential. Thus, the correct statements are (b) and (c).