TOPIC 26 OF 27

Special Purpose Diodes

🎓 Class 12 Physics CBSE Theory Ch 14 – Semiconductor Electronics ⏱ ~14 min
🌐 Language:

This MCQ module is based on: Special Purpose Diodes

This assessment will be based on: Special Purpose Diodes

Upload images, PDFs, or Word documents to include their content in assessment generation.

Special Purpose Diodes

14.8 Special-Purpose p-n Junction Diodes

Beyond rectification, the p-n junction can be engineered to perform a variety of specialised functions. By tuning the doping levels, the band gap of the semiconductor and the device geometry, we get four important "special diodes":

DeviceOperating biasFunction
Zener diodeReverse (at breakdown)Voltage regulation / reference
PhotodiodeReverseLight → current (sensor)
LED (Light-Emitting Diode)ForwardCurrent → light (emitter)
Solar cellNo bias (illumination only)Light → DC voltage (energy harvester)

14.8.1 Zener Diode — Voltage Regulator

A Zener diode is a heavily doped p-n junction designed to operate in the breakdown region under reverse bias. Two distinct breakdown mechanisms can occur:

  • Zener breakdown (heavy doping, V_br < 6 V): the very thin depletion region produces a huge electric field that rips electrons out of covalent bonds. Tunnelling current rises sharply.
  • Avalanche breakdown (lighter doping, V_br > 6 V): high-energy minority carriers ionise lattice atoms by impact, multiplying the carrier population.

Both produce the same effect: once V exceeds V_z, the diode current can change by orders of magnitude while V across the diode remains nearly constant at V_z. This is the property exploited for voltage regulation.

Zener diode — V-I curve and regulator circuit V I V_z breakdown flat Zener Voltage regulator V_in R_s D_z R_L V_out = V_z (constant)
Fig 14.21–22: (Left) Zener V-I — flat plateau at V_z under reverse bias. (Right) Voltage regulator: Zener clamps V_out to V_z even when V_in fluctuates.

How regulation works

If V_in increases, the extra voltage drops across R_s while V across Zener stays at V_z. If V_in decreases below V_z, the Zener stops conducting and acts like an open circuit — so V_in must always exceed V_z. The Zener current adjusts itself to keep V_out fixed.

Worked Example — Designing a regulator

A 6.2 V Zener regulates a 9 V input. Load draws 20 mA at 6.2 V. Choose R_s so the Zener carries at least 5 mA.

Total current through R_s = I_load + I_Zener = 20 + 5 = 25 mA.

Voltage drop across R_s = V_in − V_z = 9.0 − 6.2 = 2.8 V.

\[ R_s = \frac{V_{in} - V_z}{I_{R_s}} = \frac{2.8}{0.025} = \mathbf{112\ \Omega} \]

Choose the nearest standard value: 100 Ω or 120 Ω.

14.8.2 Optoelectronic Devices — Photodiode and LED

Both rely on the relationship: energy of a photon = E_g of the semiconductor. If hν ≥ E_g, a photon striking the depletion region creates an electron-hole pair (light → current). Conversely, an electron-hole pair recombining releases a photon of energy ≈ E_g (current → light).

Photodiode

A photodiode is a junction diode operated under reverse bias and exposed to light. The transparent window above the junction lets photons reach the depletion region. Each absorbed photon creates an e-h pair which the field separates, producing additional reverse current proportional to the light intensity.

Why operate under reverse bias and not no-bias? Because reverse bias gives a wider depletion region, and the change in fractional current is much larger and more easily measured. Photodiodes are used in TV remote receivers, light meters, optical fibre detectors and barcode scanners.

Light-Emitting Diode (LED)

An LED is a heavily doped p-n junction operated under forward bias. Injected minority carriers recombine with majority carriers near the junction; the released energy emerges as a photon of wavelength λ ≈ hc/E_g.

The colour of an LED is set by the band gap of the semiconductor:

MaterialE_g (eV)Wavelength (nm)Colour
GaAs1.43~870IR (invisible)
GaAs0.6P0.4~1.9~660Red
GaP2.26~550Green
GaN / InGaN~3.4~470Blue
White LEDBlue LED + yellow phosphor

LEDs have several advantages over incandescent bulbs: low operating voltage, low power, long life (~10⁵ h), fast switching, no warm-up time, ruggedness. They have replaced filament bulbs in nearly every general-lighting application.

Photodiode (reverse) and LED (forward) (a) Photodiode p-n junction μA + − reverse-biased (b) LED p-n junction hν out − + forward-biased Photodiode: photons → e-h pairs → reverse current. LED: forward current → e-h recombination → photons.
Fig 14.X: Photodiode (reverse-biased, light input) vs LED (forward-biased, light output).

14.8.3 Solar Cell

A solar cell is a large-area p-n junction that converts sunlight directly into a DC voltage without any external bias. Sunlight (with photon energies above E_g) creates electron-hole pairs in the depletion region; the built-in field separates them — electrons drift to n-side, holes to p-side. This separation makes the n-side the (−) terminal and the p-side the (+) terminal, generating an EMF.

Design considerations:

  • The semiconductor must have a band gap matched to the solar spectrum (~1.0-1.8 eV is optimal). Si (1.12 eV) and GaAs (1.43 eV) are common.
  • The top junction must be very near the illuminated surface so photons reach the depletion region.
  • Anti-reflection coatings reduce surface losses; metal contact grids let light in while collecting current.
Solar cell — sunlight to DC photons (hν > E_g) n (thin) depletion p-Si (thick) + LOAD
Fig 14.X: Solar cell layered structure. Photons absorbed in/near the depletion region produce e-h pairs which the built-in field separates, driving current through the load.
Why is the n-region kept thin? Because most photons are absorbed within a few μm of the surface. The depletion region must be close to where carriers are generated; otherwise the e-h pairs recombine before being separated.

Comparison Table — All Four Special Diodes

DeviceBiasInputOutputKey role of E_g
ZenerReverse, >V_zVoltageConstant V_zSets V_z (high-doping ⇒ low V_z)
PhotodiodeReverseLight (hν ≥ E_g)Reverse current ∝ intensityCutoff wavelength λ_c = hc/E_g
LEDForwardCurrentLight (λ ≈ hc/E_g)Sets emission colour
Solar cellUnbiased (illuminated)SunlightEMF + currentOptimal E_g ≈ 1-1.8 eV

Worked Example — LED wavelength

A red LED uses a semiconductor with E_g = 1.9 eV. Find the wavelength of emitted photons.
\[ \lambda = \frac{hc}{E_g} = \frac{1240\ \text{eV·nm}}{1.9\ \text{eV}} \approx \mathbf{653\ nm} \]

Indeed the red part of the visible spectrum.

Activity 14.4 — TV-remote photon detector

Point a smartphone camera at the front of any TV remote and press a button. Most phone cameras detect near-IR light and you'll see the LED at the front of the remote glow brightly on screen — even though it looks dark to your eye.

What does this demonstrate? What is the band gap of the LED material if its emission peaks at 950 nm?
It demonstrates that LEDs can emit photons outside the visible range (here, near-IR), and that camera CMOS sensors are sensitive into the IR. Required band gap: E_g = hc/λ = 1240/950 ≈ 1.31 eV. (Close to GaAs.)

Interactive — Zener Voltage Regulator

Watch a regulator clamp the output

Adjust V_in and the load resistance. The simulator shows V_out, current through Zener, and current through load.

9.0 V
120 Ω
500 Ω
V_out: 6.2 V I_load: 12.4 mA I_Zener: 10.9 mA State: regulating

Competency-Based Questions

Q1 (MCQ). A Zener diode is used as a voltage regulator. It is operated in:

  • (a) Forward bias above cut-in
  • (b) Forward bias below cut-in
  • (c) Reverse bias below breakdown
  • (d) Reverse bias at breakdown
(d) The Zener regulator works only when reverse-biased into the breakdown region — that's where V is independent of I.

Q2 (MCQ). For a semiconductor with E_g = 1.55 eV, the longest photon wavelength that creates an e-h pair is approximately:

  • (a) 200 nm
  • (b) 400 nm
  • (c) 500 nm
  • (d) 800 nm
(d) λ_c = 1240/E_g = 1240/1.55 = 800 nm.

Q3 (Short Answer). Why is Si (E_g = 1.12 eV) NOT used to make LEDs that emit visible light?

Visible light requires photon energies of 1.8-3.1 eV (corresponding to 400-700 nm). Si's band gap of 1.12 eV gives photons of ~1100 nm, which lies in the IR — invisible. Also Si is an indirect-band-gap semiconductor, making radiative recombination very inefficient compared to direct-band-gap materials like GaAs and GaN.

Q4 (Numerical). A photodiode with E_g = 1.43 eV (GaAs) — what is the longest wavelength it can detect?

λ_max = hc/E_g = 1240 nm·eV / 1.43 eV ≈ 867 nm (near-IR).

Q5 (HOTS). Why must the n-region of a solar cell be kept very thin compared to the p-region?

Sunlight is incident on the n-side. Most photons are absorbed within a few μm of the surface. If the n-region were thick, e-h pairs would be generated far from the depletion region, and would recombine before the built-in field could separate them. Keeping n thin ensures the depletion region (with its strong field) is close to where most carriers are generated, maximising collection efficiency.

Assertion–Reason Questions

Options: (A) Both true, R correct explanation. (B) Both true, R not the correct explanation. (C) A true, R false. (D) A false, R true.

Assertion: A photodiode is operated in reverse bias.

Reason: Reverse bias widens the depletion region and makes the fractional change in current due to incoming photons more pronounced.

(A) Both correct, and the reason explains the assertion.

Assertion: White LEDs are usually made by combining a blue LED with a yellow phosphor.

Reason: No single semiconductor band gap can produce all visible wavelengths simultaneously.

(A) Both correct, and the reason explains the assertion. The blue LED excites the phosphor, which down-converts to a broad yellow emission; mixing blue + yellow gives white perception.

Assertion: A solar cell does NOT need an external battery to produce a current through a load.

Reason: The built-in junction field separates photo-generated electron-hole pairs and develops an EMF on its own.

(A) Both correct, and the reason explains the assertion. The solar cell is the EMF source.

Frequently Asked Questions - Special Purpose Diodes

What is the main concept covered in Special Purpose Diodes?
In NCERT Class 12 Physics Chapter 14 (Semiconductor Electronics), "Special Purpose Diodes" covers the core principles and equations students need for board exam success. The MyAiSchool lesson explains the topic with definitions, derivations, worked examples, and interactive simulations. Key formulas and dimensional analysis are included to build conceptual depth and problem-solving skills aligned with the CBSE 2025-26 syllabus.
How is Special Purpose Diodes useful in real-life applications?
Real-life applications of "Special Purpose Diodes" from NCERT Class 12 Physics Chapter 14 include electronics, communication systems, medical imaging, solar energy, semiconductor devices, and modern technology. The MyAiSchool lesson links every concept to a tangible example so students see physics as a problem-solving framework for the physical world, not as abstract formulas.
What are the key formulas in Special Purpose Diodes?
Key formulas in "Special Purpose Diodes" (NCERT Class 12 Physics Chapter 14 Semiconductor Electronics) are derived step-by-step in the MyAiSchool lesson. Students should memorize the final formula AND understand its derivation for full board marks. Each formula is listed with its dimensional formula, SI unit, applicability range, and common pitfalls. The Summary section at the end of each part includes a quick-reference formula card.
How does this part connect to other parts of Chapter 14?
NCERT Class 12 Physics Chapter 14 (Semiconductor Electronics) is structured so each part builds on the previous one. "Special Purpose Diodes" connects directly to neighbouring parts via shared definitions, units, and methodology. The MyAiSchool lesson cross-references related concepts with internal links so students can navigate the whole chapter as one connected story rather than disconnected fragments.
What types of CBSE board questions come from Special Purpose Diodes?
CBSE board questions from "Special Purpose Diodes" typically include: (1) 1-mark MCQs on definitions and formulas, (2) 2-mark short-answer derivations or applications, (3) 3-mark numerical problems with units, (4) 5-mark long-answer derivations followed by application. The MyAiSchool lesson tags each Competency-Based Question (CBQ) with Bloom level (L1-L6) so students know how to study for each weight.
How can students use the interactive simulation effectively?
The interactive simulation in the "Special Purpose Diodes" lesson allows students to adjust input parameters (sliders or selectors) and see physical quantities update in real time. To use it effectively: (1) try extreme values to understand limiting cases, (2) compare with the analytical formula, (3) check unit consistency, (4) test special configurations from worked examples. The simulation reinforces conceptual intuition that pure formula manipulation cannot.
AI Tutor
Physics Class 12 Part II – NCERT (2025-26)
Ready
Hi! 👋 I'm Gaura, your AI Tutor for Special Purpose Diodes. Take your time studying the lesson — whenever you have a doubt, just ask me! I'm here to help.

🎯 Practise Physics

Sit a full paper on what you have been studying, marked question by question.

Board exam sample papers

All papers for this subject →

Mock exams

All mock exams for this subject →

🎁 Join our community and get free AI credits!