Electron Devices: Chapter 1: Semiconductor

Continuity Equation

Semiconductor

Questions: 1. State and explain the continuity equation. 2. Important Example Solved Problems

Continuity Equation

• The carrier concentration in the body of a semiconductor is a function of time and distance.

• Mathematically, a partial differential equation governs this functional relationship between carrier concentration, time and distance. Such an equation is called continuity equation.

• The equation is based on the fact that charge can neither be created nor destroyed.

• Consider the infinitesimal n type element of volume of area A and length dx as shown in Fig. 1.17.1.


• The average hole concentration is p/m3.

• The current entering the volume at x is I and leaving at x + dx is I + dI. This change in current is because of diffusion.

• Now due to diffusion the concentration of charge carriers decreases exponentially with the distance.

Hence,

 dI = Number of coulombs per second decreased within the volume

  ……... (1.17.1)

• Now if τp is the mean life time of the holes then, Р/τp = Holes per second lost by recombination per unit volume.

• Due to recombination, number of coulombs per second decreased within the given volume is,

 = (Charge on hole) × (Holes/sec per unit volume) × (Volume)

 = q × P/τP × (Adx) = qA dx × P/τP

         ……... (1.17.2)

• While let g is the rate at which electron hole pairs are generated by thermal generation per unit volume. Due to this, number of coulombs per second increases with the volume

 = (Charges on hole) × (Rate of a generation) × (Volume) = q g A dx

     ……… (1.17.3)

• Thus the total change in number of coulombs per second is because of three factors as indicated by the equations (1.17.1), (1.17.2) and (1.17.3).

• Total change in holes per unit volume per second is dp/dt. Hence the total change in coulombs per second within the given volume

 = q dp/dt (Volume) = q A dx dp/dt

        ….. (1.17.4)

• According to law of conservation of charges,

 q A dx dp/dt = ‒ q A dx P/τP + qgAdx ‒ dI

           ……... (1.17.5)

Key Point: The negative sign indicates decrease while positive indicates increase in number of coulombs per second.


 J = I/A = Current density

 I = JA

i.e. dI = AdJ as A is constant.


       ………..(1.17.7)

• The total current density J is due to drift and diffusion current.


 J = −qDp dp/dx + pqμPE = Diffusion + Drift

           ……… (1.17.8)

where

E = Electric field intensity within the volume

• If the semiconductor is in thermal equilibrium and subjected to no external electric field then hole density will attain a constant value P0. Under this condition I = 0 i.e. J = 0 and dp/dt = 0 due to equilibrium. Using in (1.17.7),

 0 = ‒P0P + g ‒ 0

i.e.  g = Р0 / τр

         ………. (1.17.9)

• The equation (1.17.9) indicates the thermal equilibrium i.e. the rate at which holes are thermally generated just equal to the rate at which holes are lost due to the recombination.

• Using (1.17.8) and (1.17.9) in (1.17.7),


        ………. (1.17.10)

• This is called equation of conservation of charge or the continuity equation.

• As holes in n type material are considered, let us use the suffix n. And as concentration is a function of both time t and distance x, let us use partial differentiation, Hence the final continuity equation takes the form as,


• Similarly the continuity equation for the electrons in p type material can be written as,


Let us see the special cases for continuity equation under the condition of zero electric field.

 

1. Concentration Independent of Distance and E = 0

• As concentration is not dependent on x and E = 0, the last two terms on right hand side of the continuity equation become zero. Hence equation reduces as,


• This is a differential equation interms of pn and the solution of this equation is,

 Pn‒Pn0 = Kq‒t/τp

where K = Constant

• τp is mean life time but also time constant of the above equation.

Key Point: Thus τp can be defined as the time taken by the injected concentration to fall to 36.78 % of its initial value.

 

2. Concentration Independent of Time and E = 0

• As concentration is not dependent on t and E = 0, the left hand side of continuity equation is zero and last term on right hand side is zero.


       ………. (1.17.14)

 But

 √[DPτP] = LP = Diffusion length of holes

• Hence the solution of the equation (1.17.14) takes the form,

  Pn ‒ Pn0 = K1q‒x/LP + K2q‒x/LP

where K1, K2 = Constantsis

 

3. Concentration Varies Sinusoidally with Time and E = 0

• The injected concentration varies sinusoidally with an angular frequency of ω. The sinusoidal variation is indicated in phasor form as,

  Pn(x, t) = Pn(x) qjwt

• Substituting in continuity equation with E = 0,


• For zero frequency (ω = 0), the equation takes the form as obtained for special case discussed in 1.17.2.

• Hence a.c. solution for w ≠ 0 can be obtained from d.c. solution by replacing Lp by Lp/√[1+jωτp]

• Thus continuity equation is the fundamental law governing the flow of charge.


Review Question

1. State and explain the continuity equation.

 

Electron Devices: Chapter 1: Semiconductor : Tag: electronics : Semiconductor - Continuity Equation


Electron Devices: Chapter 1: Semiconductor



Under Subject


Electron Devices

EC25C01 2nd Semester ECE Dept | 2025 Regulation | 2nd Semester 2025 Regulation



Related Subjects


English Essentials II

EN25C02 2nd Semester | 2025 Regulation | 2nd Semester 2025 Regulation



Linear Algebra

MA25C02 2nd Semester | 2025 Regulation


Electron Devices

EC25C01 2nd Semester ECE Dept | 2025 Regulation | 2nd Semester 2025 Regulation


Data Structures using CPlusPlus

CS25C05 2nd Semester ECE Dept | 2025 Regulation | 2nd Semester 2025 Regulation


Circuits and Network Analysis

EC25C02 2nd Semester ECE Dept | 2025 Regulation | 2nd Semester 2025 Regulation


Re-Engineering for Innovation

ME25C05 2nd Semester | 2025 Regulation | 2nd Semester 2025 Regulation


Engineering Drawing - Laboratory

ME25C01 2nd Semester | 2025 Regulation | 2nd Semester 2025 Regulation


Data Structures using CPlusPlus - Laboratory

CS25C05 2nd Semester ECE Dept | 2025 Regulation | 2nd Semester 2025 Regulation


Devices and Circuits Laboratory

EC25C03 2nd Semester ECE Dept | 2025 Regulation | 2nd Semester 2025 Regulation