Animated Solution for Physics - Electrostatics: Two charged thin infinite plane sheets of uniform surface charge densities σ+ and σ−, where ∣σ+∣>∣σ−∣, intersect at right angle. Which of the following best represents the electric field lines for this system?
Select Answer:
Visualized Solution
SetupofIntersectingSheets
Two intersecting infinite charged sheets:
Horizontal: σ+>0
Vertical: σ−<0
ElectricFieldofaSheet
E=2ε0σ
FieldVectorsinQuadrant1
At point P in Quadrant 1:
E+ is upwards.
E− is leftwards.
ResultantElectricField
∣σ+∣>∣σ−∣⟹∣E+∣>∣E−∣
Enet=E++E−
SlopeofResultantField
Slope of Enet=∣E−∣∣E+∣>1
SymmetryAcrossQuadrants
Symmetry in other quadrants:
Q2: Up-Right
Q3: Down-Right
Q4: Down-Left
FinalFieldLinesPattern
Uniform field ⟹ Straight parallel lines.
Steeper vertical component ⟹ Option (c).
WhatifMagnitudeswereEqual?
If ∣σ+∣=∣σ−∣, field lines would be at exactly 45∘.
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The Sigma Insight: Electric Field Lines, Flux and Gauss's Law
Solution Diagram
The problem of finding the electric field lines for two intersecting infinite plane sheets is a beautiful exercise in vector superposition and symmetry. Let's break down the physics and the geometry behind this elegant setup.
Analyzing the Setup
Imagine two infinite plane sheets intersecting at right angles. We are given two surface charge densities: σ+ on the horizontal sheet and σ− on the vertical sheet. The problem also states a crucial condition: ∣σ+∣>∣σ−∣.
Before we jump into the resultant field, let's recall the behavior of a single infinite charged sheet. The electric field produced by an infinite thin plane sheet is uniform everywhere in space. Its magnitude is given by:
E=2ε0σ
Notice that this formula does not depend on the distance from the sheet! The field is constant. Furthermore, the field points away from a positive charge and towards a negative charge.
The Master Equation
Superposition
Let's pick a point in the first quadrant.
The horizontal sheet (σ+) is positive, so it creates an electric field E+ that points vertically upwards, away from the sheet.
The vertical sheet (σ−) is negative, so it creates an electric field E− that points horizontally to the left, towards the sheet.
The net electric field at our chosen point is simply the vector sum of these two perpendicular components:
Enet=E++E−
Because the individual fields E+ and E− are constant everywhere in the first quadrant, their vector sum Enet must also be a constant vector. A constant vector field means the electric field lines will be straight, parallel lines. This immediately eliminates any options showing curved lines or circles!
The Crucial Condition
Now, let's use the condition ∣σ+∣>∣σ−∣.
Since the magnitude of the electric field is directly proportional to the surface charge density, this inequality tells us that the vertical component is stronger than the horizontal component:
∣E+∣>∣E−∣
Geometrically, if you draw a right-angled triangle with these two vectors, the vertical side is longer than the horizontal side. Therefore, the resultant vector Enet will be steeper—it will make an angle greater than 45∘ with the horizontal axis.
Final Pattern
If we apply this exact same logic to all four quadrants, we find:
- Quadrant 1: Field points Up-Left.
- Quadrant 2: Field points Up-Right.
- Quadrant 3: Field points Down-Right.
- Quadrant 4: Field points Down-Left.
Connecting these straight, steep field lines across the boundaries creates a pattern of nested rhombuses that are stretched vertically. This perfectly matches the visual representation in the correct option.
The beauty of this problem lies in realizing that uniform fields create straight lines, and the ratio of charge densities dictates the exact slope of those lines!