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CalibratePhysics

Chapter 16

Semiconductor Devices

Maharashtra HSC · 5 subtopics · textbook pages 344–364

Formula SheetEvery formula this chapter can be examined on, in one table.

Introduction — the power supply chain

  • AC mains in India: V=230 VV = 230\ \text{V} (rms), f=50 Hzf = 50\ \text{Hz}. This is the standard input for every rectifier numerical in this chapter.
  • Order of blocks in a DC power supply: transformer →\rightarrow rectifier →\rightarrow filter →\rightarrow voltage regulator →\rightarrow load. Sinusoidal AC becomes pulsating DC, then almost pure DC, then regulated DC.

p-n Junction Diode as a Rectifier

FormulaSymbols, units and conditions
fout=finf_{\text{out}} = f_{\text{in}}
  • Rule, not a derived formula: one pulse of DC per input cycle. With fin=50 Hzf_{\text{in}} = 50\ \text{Hz}, fout=50 Hzf_{\text{out}} = 50\ \text{Hz}.
  • Output (ripple) frequency of a full wave rectifier:
fout=2finf_{\text{out}} = 2 f_{\text{in}}
  • Two pulses of DC per input cycle. With fin=50 Hzf_{\text{in}} = 50\ \text{Hz}, fout=100 Hzf_{\text{out}} = 100\ \text{Hz}.
  • Emitter-to-load current relation in a full wave rectifier is not asked; what is asked are the standard efficiency figures, quoted as rules:
  • RectifierMaximum efficiencyOutput frequency for 50 Hz input
  • Half wave40.6%40.6\%50 Hz50\ \text{Hz}
  • Full wave81.2%81.2\%100 Hz100\ \text{Hz}
  • Full wave efficiency is exactly twice the half wave efficiency.
  • Ripple factor (definition, section 16.2.3):
r=rms value of AC component in the outputvalue of the DC component in the outputr = \dfrac{\text{rms value of AC component in the output}}{\text{value of the DC component in the output}}
  • Dimensionless. Smaller rr means a more effective rectifier; a full wave rectifier has less ripple than a half wave rectifier.
  • Output (ripple) frequency of a half wave rectifier:

Special Purpose Junction Diodes

Zener diode as a voltage regulator

FormulaSymbols, units and conditions
VO=VZV_O = V_Z
  • VOV_O is the voltage across the load RLR_L, VZV_Z the Zener breakdown voltage. Holds as long as Vin>VZV_{in} > V_Z and the Zener stays in its breakdown region.
  • Maximum power rating of the Zener diode:
PZ=IZ(max⁡) VZP_Z = I_{Z(\max)}\, V_Z
  • PZP_Z in watt, IZ(max⁡)I_{Z(\max)} in ampere, VZV_Z in volt. Use it in reverse, IZ(max⁡)=PZ/VZI_{Z(\max)} = P_Z / V_Z, to get the largest safe Zener current.
  • Series (current limiting) resistance:
RS=VS−VZIZR_S = \dfrac{V_S - V_Z}{I_Z}
  • VSV_S (also written VinV_{in}) is the unregulated supply voltage. Putting IZ=IZ(max⁡)I_Z = I_{Z(\max)} gives the minimum safe value of RSR_S.
  • Load current:
IL=VZRLI_L = \dfrac{V_Z}{R_L}
  • Because the load sits in parallel with the Zener, the voltage across it is VZV_Z.
  • Current division at the junction of RSR_S, the Zener and the load:
IS=IZ+ILsoIZ=IS−ILI_S = I_Z + I_L \qquad \text{so} \qquad I_Z = I_S - I_L
  • ISI_S is the current through the series resistor. With no load, IL=0I_L = 0 and IZ=ISI_Z = I_S — this is the worst case for power dissipation in the Zener.
  • Field strength at Zener breakdown in a heavily doped diode: about 3×107 V/m3 \times 10^{7}\ \text{V/m}.
  • Zener diodes with VZ<6 VV_Z < 6\ \text{V} work mainly by Zener breakdown; those with VZ>6 VV_Z > 6\ \text{V} work mainly by avalanche breakdown. Both are called Zener diodes.
  • Regulated output voltage:

Photodiode

FormulaSymbols, units and conditions
Rd=Maximum reverse voltageDark currentR_d = \dfrac{\text{Maximum reverse voltage}}{\text{Dark current}}
  • RdR_d in ohm. It is the resistance of the photodiode when it is not illuminated.
  • Total current through a photodiode:
Itotal=Iphotocurrent+IdarkI_{\text{total}} = I_{\text{photocurrent}} + I_{\text{dark}}
  • Rule: the reverse current is proportional to the intensity of the incident light; the dark current is not.
  • Condition for photogeneration: photon energy must exceed the band gap,
hν>Egh\nu > E_g
  • Spectral response of a silicon photodiode: 190 nm190\ \text{nm} (UV) to 1100 nm1100\ \text{nm} (IR).
  • Dark resistance:

Solar cell

FormulaSymbols, units and conditions
PL=V×IP_L = V \times I
  • is maximum. This is the maximum power point.
  • Band gap criterion for the solar cell material: 1.0 eV≤Eg≤1.8 eV1.0\ \text{eV} \le E_g \le 1.8\ \text{eV}; most practical materials have EgE_g about 1.5 eV1.5\ \text{eV}.
  • MaterialBand gap EgE_g
  • Si1.1 eV1.1\ \text{eV}
  • GaAs1.43 eV1.43\ \text{eV}
  • CdTe1.45 eV1.45\ \text{eV}
  • CuInSe1.04 eV1.04\ \text{eV}
  • Power delivered to the load is zero at both ends of the characteristic — at short circuit (current IscI_{sc}, voltage zero) and at open circuit (voltage VocV_{oc}, current zero). Between them there is one point where the delivered power

LED

  • Forward voltage drop of an LED: 1.5 V1.5\ \text{V} to 3.5 V3.5\ \text{V} — much larger than the 0.7 V0.7\ \text{V} of an ordinary silicon diode.
  • Current rating: a few tens of milliampere. A high resistance must therefore be connected in series with an LED.
  • Rule: light output is directly proportional to the forward current.
  • Efficiency figures quoted by the textbook: up to 135135 lumens/watt, lifetime 50 00050\,000 hours or more.

Bipolar Junction Transistor (BJT)

FormulaSymbols, units and conditions
IE=IB+ICI_E = I_B + I_C
  • IEI_E emitter current, IBI_B base current, ICI_C collector current, all in ampere. Typically IBI_B is about 5%5\% of IEI_E and ICI_C about 95%95\% of IEI_E, so IC≈IEI_C \approx I_E.
  • Common base DC current gain:
αDC=ICIE\alpha_{DC} = \dfrac{I_C}{I_E}
  • Dimensionless, always slightly less than 1.
  • Common emitter DC current gain (current amplification factor):
βDC=ICIB\beta_{DC} = \dfrac{I_C}{I_B}
  • Dimensionless; typically 20 to 200 for general purpose transistors.
  • Combined statement:
IC=αIE=βIBI_C = \alpha I_E = \beta I_B
  • Relation between the two gains:
αDC=βDC1+βDCandβDC=αDC1−αDC\alpha_{DC} = \dfrac{\beta_{DC}}{1 + \beta_{DC}} \qquad \text{and} \qquad \beta_{DC} = \dfrac{\alpha_{DC}}{1 - \alpha_{DC}}
  • Obtained from IE=IB+ICI_E = I_B + I_C divided throughout by ICI_C, giving 1αdc=1βdc+1\dfrac{1}{\alpha_{dc}} = \dfrac{1}{\beta_{dc}} + 1.
  • Input dynamic resistance (CE configuration):
ri=(ΔVBEΔIB)VCE constantr_i = \left( \dfrac{\Delta V_{BE}}{\Delta I_B} \right)_{V_{CE}\ \text{constant}}
  • In ohm. Small, because the input junction is forward biased.
  • Output dynamic resistance (CE configuration):
ro=(ΔVCEΔIC)IB constantr_o = \left( \dfrac{\Delta V_{CE}}{\Delta I_C} \right)_{I_B\ \text{constant}}
  • In ohm. Large, because the output junction is reverse biased.
  • Output loop (Kirchhoff) for the CE amplifier:
VCC=VCE+ICRLV_{CC} = V_{CE} + I_C R_L
  • Input loop for the CE amplifier:
VBB=VBE+IBRBV_{BB} = V_{BE} + I_B R_B
  • AC current gain:
βAC=icib=ΔICΔIB\beta_{AC} = \dfrac{i_c}{i_b} = \dfrac{\Delta I_C}{\Delta I_B}
  • Nearly equal to βDC\beta_{DC} at normal operating voltages.
  • Change in output voltage of the amplifier (from VCCV_{CC} constant):
ΔVCE=−RL ΔICsoVo=ΔVCE=−βACRL ΔIB\Delta V_{CE} = - R_L\, \Delta I_C \qquad \text{so} \qquad V_o = \Delta V_{CE} = - \beta_{AC} R_L\, \Delta I_B
  • Voltage gain:
Av=vovi=ΔVCEri ΔIB=−βACRLriA_v = \dfrac{v_o}{v_i} = \dfrac{\Delta V_{CE}}{r_i\, \Delta I_B} = - \dfrac{\beta_{AC} R_L}{r_i}
  • The negative sign means the output is 180∘180^\circ out of phase with the input.
  • Power gain:
Ap=βAC×AvA_p = \beta_{AC} \times A_v
  • Magnitude only — the negative sign of AvA_v is ignored. Power gain is possible because βAC≫1\beta_{AC} \gg 1.
  • Barrier potential of the emitter-base junction for a silicon transistor: 0.6 V0.6\ \text{V} to 0.7 V0.7\ \text{V}. The transistor conducts only when VBEV_{BE} exceeds it.
  • Current relation in any configuration:

Logic Gates — Boolean expressions

FormulaSymbols, units and conditions
Y=X‾Y = \overline{X}
  • OR gate (logical addition), two or more inputs:
Y=A+BY = A + B
  • AND gate (logical multiplication):
Y=A⋅BY = A \cdot B
  • NAND gate (NOT of AND):
Y=A⋅B‾Y = \overline{A \cdot B}
  • NOR gate (NOT of OR):
Y=A+B‾Y = \overline{A + B}
  • Exclusive-OR (X-OR) gate:
C=A⊕B=A‾⋅B+A⋅B‾C = A \oplus B = \overline{A} \cdot B + A \cdot \overline{B}
  • Universal gates: NAND and NOR. Any gate can be built from a combination of NAND gates alone or NOR gates alone.
  • Digital levels: low =0=0 V= 0 = 0\ \text{V}, high =1=+5 V= 1 = +5\ \text{V}.
  • NOT gate (inverter), one input, one output:

The five truth tables in one place

  • ABAND A⋅BA \cdot BOR A+BA + BNAND A⋅B‾\overline{A \cdot B}NOR A+B‾\overline{A + B}X-OR A⊕BA \oplus B
  • 0000110
  • 0101101
  • 1001101
  • 1111000
  • XNOT X‾\overline{X}
  • 01
  • 10

Standard numerical results worked in the textbook

  • A 50 Hz50\ \text{Hz} input gives 50 Hz50\ \text{Hz} out of a half wave rectifier and 100 Hz100\ \text{Hz} out of a full wave rectifier (Example 16.1).
  • Zener regulator, VS=12 VV_S = 12\ \text{V}, VZ=5.0 VV_Z = 5.0\ \text{V}, PZ=2.0 WP_Z = 2.0\ \text{W}, RL=1 kΩR_L = 1\ \text{k}\Omega (Example 16.2): IZ(max⁡)=PZ/VO=2.0/5.0=0.4 A=400 mAI_{Z(\max)} = P_Z / V_O = 2.0/5.0 = 0.4\ \text{A} = 400\ \text{mA}; RS(min⁡)=(12.0−5.0)/0.400=17.5 ΩR_{S(\min)} = (12.0 - 5.0)/0.400 = 17.5\ \Omega; IL=5.0/1000=5.0 mAI_L = 5.0/1000 = 5.0\ \text{mA}; IZ=400−5=395 mAI_Z = 400 - 5 = 395\ \text{mA}.
  • αDC=0.967\alpha_{DC} = 0.967, IE=10 mAI_E = 10\ \text{mA}: IC=αDCIE=9.67 mAI_C = \alpha_{DC} I_E = 9.67\ \text{mA}, so IB=IE−IC=0.33 mAI_B = I_E - I_C = 0.33\ \text{mA}.
  • IE=10 mAI_E = 10\ \text{mA}, IC=9.8 mAI_C = 9.8\ \text{mA}: IB=0.2 mAI_B = 0.2\ \text{mA}.
  • IE=6.28 mAI_E = 6.28\ \text{mA}, IC=6.20 mAI_C = 6.20\ \text{mA}: αDC=6.20/6.28=0.987\alpha_{DC} = 6.20/6.28 = 0.987.
Short NotesThe chapter subtopic by subtopic, in the textbook's own order.5 subtopics
  1. 1Introduction
  2. 2p-n Junction Diode as a Rectifier6 board questions
  3. 3Special Purpose Junction Diodes5 board questions
  4. 4Bipolar Junction Transistor (BJT)4 board questions
  5. 5Logic gates5 board questions
The whole chapter in brief

16.1 Introduction

  • A p-n junction diode acts as a switch: forward biased it is a closed switch and current flows; reverse biased it is an open switch and only a negligibly small current flows. This switching action is what makes it a rectifier.
  • AC is generated and transmitted more cheaply than DC, so mains supply is AC — in India 230 V230\ \text{V}, 50 Hz50\ \text{Hz}, varying sinusoidally. Gadgets such as a TV or a mobile charger need DC, so the mains must be rectified.
  • Block chain of a DC power supply, in order: AC mains →\rightarrow transformer →\rightarrow rectifier →\rightarrow filter →\rightarrow voltage regulator →\rightarrow load.
StageWaveform there
Secondary of transformerSinusoidal AC, stepped up or down
After rectifierPulsating DC, unidirectional, contains ripple
After filterAlmost pure DC, small ripple may remain
After regulatorSteady, regulated pure DC of the required value
  • Ripple: the AC component present in the DC output of a rectifier.

16.2 Rectifiers

  • Rectification: the conversion of AC voltage into DC voltage. Rectifier: an electronic circuit which rectifies AC voltage.
  • Two types: half wave rectifier (one diode) and full wave rectifier (two diodes, centre tapped transformer).

Half wave rectifier

  • Secondary coil AB of the transformer is in series with a diode D and the load RLR_L.
  • Positive half cycle: A is at higher potential than B, D is forward biased, it conducts, current flows through RLR_L.
  • Negative half cycle: A is at lower potential than B, D is reverse biased, it does not conduct, no current flows.
  • Output across RLR_L is a set of alternate pulses in one direction only; the negative half cycles are lost. Output frequency =50 Hz= 50\ \text{Hz} for a 50 Hz50\ \text{Hz} input.
  • Two advantages of using a transformer: it steps the AC input up or down as the circuit requires, and it isolates the rectifier from the mains, reducing the risk of electric shock.

Full wave rectifier

  • Centre tapped transformer with diodes D1D_1 and D2D_2; they conduct alternately.
  • Positive half cycle: A is at higher potential than B, D1D_1 conducts, current through RLR_L follows the path APQRC.
  • Negative half cycle: B is at higher potential than A, D2D_2 conducts, current through RLR_L follows the path BPQRC.
  • Current through RLR_L is in the same direction in both half cycles, so the output is continuous pulses. Output frequency =100 Hz= 100\ \text{Hz} for a 50 Hz50\ \text{Hz} input.
  • Advantages: rectification takes place in both half cycles of the AC input, and the ripple is less than in a half wave rectifier.

Distinguish: half wave and full wave rectifier

PointHalf wave rectifierFull wave rectifier
Number of diodesOneTwo
TransformerOrdinary secondaryCentre tapped secondary
Half cycles usedOnly the positive half cyclesBoth half cycles
OutputAlternate pulsesContinuous pulses
Output frequency (50 Hz input)50 Hz50\ \text{Hz}100 Hz100\ \text{Hz}
Maximum efficiency40.6%40.6\%81.2%81.2\%
RippleMoreLess

Ripple factor and filters

  • Ripple factor r=rms value of AC componentvalue of DC componentr = \dfrac{\text{rms value of AC component}}{\text{value of DC component}} in the rectifier output. A smaller ripple factor means a more effective rectifier.
  • A filter circuit removes the AC component (the ripple) from the rectifier output and allows only the DC component through.
  • Capacitor filter: the pulsating DC is applied across a capacitor in parallel with the load. As the rectifier voltage rises the capacitor charges up to the peak voltage VpV_p at the end of the quarter cycle and supplies current to the load. When the rectifier voltage falls, the capacitor discharges through RLR_L and the load voltage drops only slightly, because the next voltage peak recharges the capacitor immediately. Repeating this smooths the output.
  • Capacitor filter is widely used because of its low cost, small size and light weight; it is preferred for small load currents and is common in battery eliminators.
  • Unregulated power supply: one whose output voltage changes when a load is connected across it. Regulated power supply: one whose output remains steady even after a load is connected.

16.3 Special purpose junction diodes

Four studied: Zener diode, photodiode, solar cell, LED. The Zener works on junction breakdown; the other three make use of photosensitivity.

Zener diode

  • A Zener diode is a heavily doped p-n junction diode designed to work in the breakdown region. Heavy doping makes the depletion layer very thin.
  • Zener breakdown: increasing the reverse voltage raises the electric field across the junction; the field exerts a force on the bound electrons, covalent bonds break, electrons are freed and a large current flows. More voltage frees more electrons, so the current rises rapidly.
  • Zener breakdown does not damage the diode; ordinary reverse breakdown of a normal diode does.
  • Symbol in words: an ordinary diode symbol (triangle pointing at a bar) with the bar bent at both ends into the shape of the letter Z.
  • Characteristic in words: in forward bias it behaves exactly like a normal diode (current rises sharply past the knee). In reverse bias almost no current flows until the reverse voltage reaches VZV_Z; there the current increases suddenly and steeply, while the voltage across the diode stays constant at VZV_Z however large the current becomes.
  • VZV_Z depends on doping: heavier doping gives a thinner depletion layer and a lower breakdown voltage; lighter doping gives a higher breakdown voltage. Diodes below 6 V6\ \text{V} operate mainly by Zener breakdown, those above 6 V6\ \text{V} mainly by avalanche breakdown; both are called Zener diodes.
  • As a regulator: RSR_S in series limits the current; the Zener is in reverse bias across the load RLR_L, so VO=VZV_O = V_Z. If VinV_{in} rises, the extra voltage is dropped across RSR_S and VZV_Z is unchanged. If RLR_L falls, ILI_L rises and IZI_Z falls by the same amount, again keeping VZV_Z constant.
  • Specifications on a datasheet: Zener V-I characteristic, Zener voltage VZV_Z, maximum Zener current IZMI_{ZM}, power rating, Zener resistance (impedance) RZR_Z.
  • Applications: voltage regulator, fixed reference voltage in transistor biasing, peak clipper or limiter in wave shaping, protection of meters against accidental fluctuations.

Photodiode

  • A photodiode is a special p-n junction diode which converts light energy into electrical energy; also called a photodetector or photosensor. It is always operated in reverse bias, and only minority carrier current flows through it.
  • Construction: the junction is placed inside a glass window so that only the junction is exposed to light; the rest of the diode is painted with an opaque colour or covered.
  • Dark current: the reverse saturation current that flows even when the photodiode is not illuminated. It is due to minority carriers and depends only on their concentration, not on the applied voltage.
  • On illumination with photons of energy greater than the band gap, electron-hole pairs are generated in the depletion region; the intrinsic field of the depletion region separates them, electrons going to the anode and holes to the cathode, so the reverse current increases.
  • Reverse current depends on the intensity of the incident light; total current == photocurrent ++ dark current.
  • Characteristic in words: a family of reverse-bias curves, one per light intensity, each nearly flat (current almost independent of reverse voltage) and each higher than the one below it. The reverse current first increases with intensity and then settles at a constant saturation current.
  • Dark resistance Rd=maximum reverse voltagedark currentR_d = \dfrac{\text{maximum reverse voltage}}{\text{dark current}}. Sensitivity improves when the dark current is minimised.
  • Advantages: quick response to light; linear response (reverse current proportional to intensity); high speed of operation; light weight and compact; wide spectral response (silicon: 190 nm190\ \text{nm} to 1100 nm1100\ \text{nm}); relatively low cost.
  • Disadvantages: properties are temperature dependent; low reverse current at low illumination.
  • Applications: counters and switches, burglar alarms, detection of visible and invisible radiation, fast switching circuits, fibre optic communication, optocouplers, photo sensors for light intensity, fire and smoke detectors.

Solar cell (photovoltaic cell)

  • A solar cell converts solar energy directly into electrical energy; it is a source of DC power.
  • Structure: a p-n junction with the thin n-side facing the radiation and a relatively thick p-side at the back. Both sides are coated with conducting material — the front contact on the n-side, the back (rear) contact on the p-side. An antireflection coating on the n-side lets visible light through but reflects IR (heat) radiation, protecting the cell from temperature changes.
  • Working, in four steps: (1) electron-hole pairs are generated in the depletion region; (2) electrons and holes are separated and collected at the cathode and the anode; (3) the accumulated carriers generate a voltage across the cell; (4) the power produced is dissipated in the load connected across the cell.
  • The separation of carriers is possible because of the intrinsic electric field of the depletion region — otherwise the pairs would simply recombine and no current would be produced.
  • Characteristic in words: the illuminated V-I curve is drawn in the fourth quadrant, because the cell supplies current to the load instead of drawing it. Its intercept on the current axis is the short circuit current IscI_{sc} and its intercept on the voltage axis is the open circuit voltage VocV_{oc}. Power delivered is zero at both ends and is maximum at one point in between, the maximum power point.
  • Criteria for the material: band gap between 1.0 eV1.0\ \text{eV} and 1.8 eV1.8\ \text{eV}, high optical absorption, good electrical conductivity, easy availability.
  • Uses: charging batteries during the day so they supply power at night; power at remote places, for calculators, satellites and space stations; traffic signals; communication stations; lux meters to measure light intensity.

Distinguish: photodiode and solar cell

PointPhotodiodeSolar cell
BiasOperated in reverse biasOperated with no external bias; it is itself the source
FunctionDetects light, converts it into a measurable currentConverts light into electric power
Quantity of interestReverse current proportional to intensityOutput voltage and current delivered to a load
Working quadrantThird quadrant (reverse bias)Fourth quadrant
Junction areaSmallLarge

Light Emitting Diode (LED)

  • An LED is a diode which emits light when a large forward current passes through it.
  • Symbol in words: the ordinary diode symbol with two small arrows pointing away from it, showing emitted light.
  • Construction: the n-region is more heavily doped than the p-region; the junction is encased in a dome-shaped transparent case so that light is emitted uniformly in all directions and internal reflections are minimised; metal electrodes on either side act as contacts, the longer leg being the anode; the device is made so that the emitted light is not reabsorbed, with recombination occurring at the surface for maximum light output.
  • Working: in forward bias, electrons from the conduction band recombine with holes in the valence band, releasing enough energy to produce photons of monochromatic light. Because the layer is thin, a good number of these photons escape the junction. Light output is directly proportional to the forward current.
  • Characteristic in words: similar to the forward characteristic of an ordinary diode — negligible current until the cut-in voltage, then a steep rise — except that the forward drop is much larger, 1.5 V1.5\ \text{V} to 3.5 V3.5\ \text{V}.
  • Colour depends on the compound semiconductor used: AlGaAs gives infrared, GaAsP red or yellow, AlGaP red or green, ZnSe blue.
  • Advantages: energy efficient (up to 135135 lumens/watt), long lifetime (50 00050\,000 hours or more), rugged solid state light with no filament, almost no warm-up (emits in nanoseconds), excellent colour rendering, environment friendly (no mercury), controllable brightness and colour.
  • Disadvantages: hazardous blue light quality, temperature dependence, voltage sensitivity, high initial cost.
  • Applications: burglar alarms, counters, optical communication, indicator lamps, cell phone displays, LED television, vehicle head lamps, decorative illumination, street lighting, seven segment displays.
  • White LED: made by wavelength conversion — a blue LED excites a yellow phosphor, and the mixture of blue and yellow light appears white. The blue LED was invented by Shuji Nakamura (Nobel Prize in Physics, 2014).

16.4 Bipolar Junction Transistor (BJT)

  • A junction transistor is a semiconductor device with two junctions and three terminals. The current is carried by both electrons and holes, so it is called bipolar.
  • Two types: n-p-n (a thin p-type base between two n-type layers) and p-n-p (a thin n-type base between two p-type layers).
  • Symbols in words: three leads meeting at a vertical bar (the base); the emitter lead carries an arrow. For n-p-n, the arrow points away from the base, out of the emitter. For p-n-p, the arrow points from the emitter towards the base. The arrow always shows the direction of conventional current.
RegionThicknessDopingRole
EmitterThickHeavySupplies a large number of majority carriers
BaseThinLightPasses most carriers on; controls the transistor action
CollectorLargest areaIntermediateCollects most of the carriers, dissipates heat
  • Two-diode analogy: a transistor behaves like two junction diodes connected back to back. It cannot, however, be made by joining two diodes.
  • Biasing for normal (active) operation: emitter-base junction forward biased, collector-base junction reverse biased. The E-B junction then has low resistance and the C-B junction high resistance.
  • Working of an n-p-n transistor: electrons are the majority carriers in the emitter. When VBEV_{BE} exceeds the barrier potential (0.60.6 to 0.7 V0.7\ \text{V} for silicon), electrons are injected into the base. A few recombine in the base and form IBI_B (about 5%5\% of IEI_E); the rest diffuse across the thin base into the collector-base depletion region and are swept into the collector by its field, forming ICI_C (about 95%95\% of IEI_E). A p-n-p transistor works exactly the same way with holes as the carriers.
  • IE=IB+ICI_E = I_B + I_C, and since IBI_B is small, IC≈IEI_C \approx I_E.
  • Three configurations: common emitter (CE), common base (CB), common collector (CC). The CE amplifier gives the highest current gain and power gain of the three, because the input impedance is low (forward biased junction) and the output impedance is high (reverse biased junction).

CE characteristics

  • Input characteristic: variation of IBI_B with VBEV_{BE}, keeping VCEV_{CE} fixed. In words: current is very small until the barrier potential is overcome, after which the curve looks like that of a forward biased diode. Slope gives ri=ΔVBE/ΔIBr_i = \Delta V_{BE} / \Delta I_B.
  • Output characteristic: variation of ICI_C with VCEV_{CE}, keeping IBI_B constant. In words: ICI_C rises steeply for very small VCEV_{CE} and then becomes almost flat — ICI_C is independent of VCEV_{CE} as long as the collector-emitter junction stays reverse biased. Each higher fixed IBI_B gives a higher flat curve. Slope of the flat part gives ro=ΔVCE/ΔICr_o = \Delta V_{CE} / \Delta I_C.

Transistor as an amplifier (CE)

  • An amplifier increases the amplitude of an alternating signal (voltage, current or power).
  • Circuit in words: an n-p-n transistor in CE configuration; a DC bias VBBV_{BB} with RBR_B in the base circuit, a supply VCCV_{CC} with the load resistance RLR_L in the collector circuit, a small sinusoidal signal viv_i superimposed on the DC bias at the input, and a capacitor in the output to block the DC component so that only the amplified AC appears across the output.
  • Working: the AC signal changes VBEV_{BE}, hence IBI_B, hence ICI_C. Since VCC=VCE+ICRLV_{CC} = V_{CE} + I_C R_L with VCCV_{CC} fixed, a change in ICI_C forces an opposite change in VCEV_{CE}, and this change is the amplified output.
  • Av=−βACRLriA_v = -\dfrac{\beta_{AC} R_L}{r_i}, negative sign meaning input and output are out of phase; Ap=βAC×AvA_p = \beta_{AC} \times A_v in magnitude.
  • A transistor amplifies power but does not generate power — the extra power comes from the DC supply VCCV_{CC}, not from nothing.

16.5 Logic gates

  • Analog signal: a continuously varying voltage or current, e.g. a sine wave. Digital signal: one that can take only two discrete values, e.g. a square wave. In a digital circuit these are low (0 V0\ \text{V}) and high (+5 V+5\ \text{V}).
  • Logic gate: a digital circuit with one or more inputs but only one output, which follows a certain logical relationship between input and output voltages. They are called gates because they control the flow of signal or information.
  • Truth table: a table showing all possible combinations of the inputs with the corresponding outputs. It defines the function of the gate.
  • Boolean expression: the mathematical statement giving the relationship between the input and output of a logic gate.
GateBoolean expressionOutput is high when
NOTY=X‾Y = \overline{X}The single input is low
ORY=A+BY = A + BAny one input, or both, is high
ANDY=A⋅BY = A \cdot BBoth inputs are high simultaneously
NANDY=A⋅B‾Y = \overline{A \cdot B}Not both inputs are high
NORY=A+B‾Y = \overline{A + B}Both inputs are low
X-ORC=A⊕BC = A \oplus BThe two inputs are at different levels
ABANDORNANDNORX-OR
0000110
0101101
1001101
1111000
  • Symbols in words: NOT is a triangle with a small circle (bubble) at its tip. AND is a D-shape, flat at the input side and round at the output. OR is a curved shield shape, concave at the input side and pointed at the output. NAND is the AND shape with a bubble at the output. NOR is the OR shape with a bubble at the output. X-OR is the OR shape with one extra curved line across the inputs.
  • NAND and NOR are called universal gates because any gate can be implemented using only NAND gates or only NOR gates.
  • The NOT gate is also known as an inverter, because it produces a negated version of the input at its output.

Traps that cost marks

  • Half wave output frequency is 50 Hz50\ \text{Hz}, not 100 Hz100\ \text{Hz}. Only the full wave rectifier doubles the frequency. Many students swap the two.
  • A full wave rectifier needs a centre tapped transformer. Leaving the centre tap out of the diagram loses marks even if the working is written correctly.
  • Half wave efficiency 40.6%40.6\%, full wave 81.2%81.2\% — full wave is twice half wave, not four times.
  • A Zener diode is always used in reverse bias when regulating. Drawing it forward biased is a straight loss of marks.
  • Never omit the series resistance RSR_S in a Zener regulator circuit. Its job is to limit the Zener current and protect the diode; the load RLR_L is in parallel with the Zener, not in series.
  • Zener breakdown does not damage the diode. Ordinary reverse breakdown of a normal diode does. State the difference explicitly when asked how a Zener differs from an ordinary diode.
  • A photodiode is reverse biased, a solar cell is unbiased. Do not describe a photodiode as forward biased.
  • Dark current is not zero and is not caused by light — it flows because of minority carriers even in complete darkness.
  • LED forward drop is 1.51.5 to 3.5 V3.5\ \text{V}, not 0.7 V0.7\ \text{V}, and an LED must have a series resistance because its current rating is only a few tens of milliampere.
  • In an LED it is the n-region that is more heavily doped, and the light comes from electron-hole recombination, not from heating of the junction.
  • Base is thin and lightly doped — write both, not just one. That is what makes most carriers reach the collector instead of recombining in the base.
  • In a transistor, IEI_E is the largest current, not ICI_C. And IE=IB+ICI_E = I_B + I_C, so IB=IE−ICI_B = I_E - I_C — the commonest slip in the numericals is subtracting the wrong pair.
  • αDC=IC/IE\alpha_{DC} = I_C/I_E is always less than 1; βDC=IC/IB\beta_{DC} = I_C/I_B is large. Getting these two the wrong way round makes every gain calculation wrong.
  • The negative sign in AvA_v is physics, not an error: it records the 180∘180^\circ phase difference between input and output. Drop it only when quoting a magnitude for the power gain.
  • In the output characteristic, IBI_B is held constant; in the input characteristic, VCEV_{CE} is held constant. Stating the wrong constant loses the mark.
  • Write the truth table with all four input combinations in order, even if the question asks only for the Boolean expression — and remember the NAND output is high in three rows out of four, not one.
  • NAND and NOR are universal, not AND and OR.
Solved Numerical ExamplesWorked numericals to attempt first, each with a hint before the full solution.Coming soon

These are being added chapter by chapter. They are solved numericals from the prescribed book and the reference guides — not previous board questions, which live under Practice — so that you can work through the method before meeting it in a real paper.

Important DerivationsEvery derive / obtain / prove question in this chapter. 1 have come up in two or more papers.1
  1. 1
    Relation between αdc\alpha_{dc} and βdc\beta_{dc} (transistor current gains) Repeats
    Define αdc\alpha_{dc} and βdc\beta_{dc}. Obtain the relation between them.

    Asked in: July 2022 (Q.21, 3 marks); February 2024 (Q.17, 3 marks)

    Show the derivation
    Step 1
    In case of common emitter configuration, α\alpha is the ratio of the collector current to the emitter current.
    αDC=ICIE....(1)\alpha_{DC}=\dfrac{I_C}{I_E}\qquad....(1)
    Step 2
    Similarly, the current gain or the current amplification factor (β\beta) is defined as the ratio of the collector current to the base current.
    βDC=ICIB....(2)\beta_{DC}=\dfrac{I_C}{I_B}\qquad....(2)
    Step 3
    Since, IE=IB+ICI_E=I_B+I_C
    Dividing throughout by ICI_C, we have,
    IEIC=IBIC+1\dfrac{I_E}{I_C}=\dfrac{I_B}{I_C}+1
    ∴1αdc=1βdc+1....[From (1) and (2)]\therefore\dfrac{1}{\alpha_{dc}}=\dfrac{1}{\beta_{dc}}+1\qquad....\text{[From (1) and (2)]}
    ∴αDC=βdc1+βdc\therefore\alpha_{DC}=\dfrac{\beta_{dc}}{1+\beta_{dc}}
    ∴βDC=αdc1−αdc\therefore\beta_{DC}=\dfrac{\alpha_{dc}}{1-\alpha_{dc}}

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