Given a uniform electric field E in the positive X-direction:
ΔV = -E·Δr
O(0,0), A(+2 cm,0)
Δr = 2 cm î
VA - VO = -E·2 cm < 0
⇒ VO > VA
• B(0,+1 cm)
Δr = 1 cm ĵ
VB - VO = -E·0 = 0
⇒ VO = VB
Only option (1) VO > VA is correct.
Thus, we have VO=VB and VO\(>\)VA, which means the correct answer is (1).
The electric potential decreases in the direction of the electric field. Since the electric field points along the positive X direction, it means that as you move in this direction, the potential decreases.
Point O is at the origin, so it’s the reference point. Point A is along the X-axis at r=+2 cm, which is in the direction of the field.
Therefore, the potential at A will be lower than at O. Point B is along the Y-axis at y=+1 cm.
Since there is no component of the electric field along the Y-axis, no work is done in moving a charge from O to B.
Hence, the potential at B is the same as at O.
Thus, we have VO=VB and VO\(>\)VA, which means the correct answer is (1).
Match List - I with List - II:
List - I:
(A) Electric field inside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(B) Electric field at distance \( r > 0 \) from a uniformly charged infinite plane sheet with surface charge density \( \sigma \).
(C) Electric field outside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(D) Electric field between two oppositely charged infinite plane parallel sheets with uniform surface charge density \( \sigma \).
List - II:
(I) \( \frac{\sigma}{\epsilon_0} \)
(II) \( \frac{\sigma}{2\epsilon_0} \)
(III) 0
(IV) \( \frac{\sigma}{\epsilon_0 r^2} \) Choose the correct answer from the options given below: