Derive Continuity Equation (Appeared: May 2022, May 2023, Dec 2023)
Continuity Equation (Appeared: May 2022, May 2023, Dec 2023)
The Continuity Equation is a mathematical expression that describes the conservation of electric charge in a semiconductor or conducting medium. It ensures that charge doesn't magically appear or disappear—what goes in must come out unless it is stored or lost.
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Concept Overview
In telecommunication circuits and semiconductor devices like diodes and transistors:
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Electrons and holes are moving.
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Their movement creates current.
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The density of charge in a region may change with time.
This change is captured by the continuity equation.
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General Statement
The Continuity Equation is:
∂ρ/∂t + ∇ · J = 0
Where:
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ρ = charge density (C/m³)
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∂ρ/∂t = rate of change of charge density with time
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∇ · J = divergence of current density J (A/m²)
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J = current density vector
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Physical Meaning
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If more current leaves a region than enters, charge inside decreases → ∂ρ/∂t becomes negative.
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If charge builds up in a region, that means not all current is leaving.
In simple words:
Rate of charge increase = Current coming in − Current going out
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Application in Semiconductors
In semiconductors (e.g. PN junctions):
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Two types of charge carriers: electrons (n) and holes (p).
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Each has its own current:
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Jn → electron current density
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Jp → hole current density
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We write two continuity equations:
For Electrons:
∂n/∂t = (1/q) ∇ · Jn + G - R
For Holes:
∂p/∂t = -(1/q) ∇ · Jp + G - R
Where:
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n and p = electron and hole concentration
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q = magnitude of electron charge
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G = generation rate (creating new carriers)
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R = recombination rate (carriers disappearing)
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Derivation Step-by-Step { Write only steps mentioned in bold for 5marks questions}:
Step 1: Charge in a Volume
Let Q be the total charge inside volume V.
Q = ∫_V ρ dV
Step 2: Change in Charge with Time
Rate of change:
dQ/dt = ∫_V ∂ρ/∂t dV
Step 3: Net Current Flow (Outward)
Using Gauss's Divergence Theorem:
I_out = ∮_S J · dA = ∫_V ∇ · J dV
So, total current leaving volume = divergence of current inside volume.
Step 4: Apply Conservation of Charge
Charge can't vanish, so:
dQ/dt = – I_out
This gives:
∫_V ∂ρ/∂t dV = – ∫_V ∇ · J dV
Since this must be true for any volume, we equate the integrands:
∂ρ/∂t + ∇ · J = 0
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Significance in Electronics and Telecommunication
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Used in MOSFETs, diodes, BJT, and IC design.
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Forms the base for device simulations (e.g. in SPICE).
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Ensures signal integrity in high-speed digital/analogue circuits.
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Useful in electromagnetic wave propagation, transmission lines, and antenna theory.
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Key Takeaways
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It is a conservation law for electric charge.
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Helps model how charge carriers behave inside a material.
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Without this, telecommunication devices wouldn't function predictably.
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