Examoogle
ExamsTest SeriesCBATRank CheckPrevious Year PapersPassBook StoreMy BooksAI Tutor
🛒0
अA
Examoogle

India's most trusted platform for competitive exam PDF books. Expert-authored, watermark-protected, instant access.

Exams & Practice
All Exams & SyllabusMock Test SeriesPrevious Year PapersPractice Questions (MCQs)Recruitment Notifications
Quick Links
Examoogle AI TutorExam NewsBook StoreMy BooksLogin / Sign Up
Support
About UsRefund PolicyPrivacy PolicyTerms of UseContact Us
© 2026 Examoogle. India's #1 competitive exam AI tutor.
🔒 SSL Secured📱 UPI Accepted🧾 GST Invoice
Examoogle

Join 60,000+ competitive exam aspirants

or with email
By continuing, you agree to ourTerms of Service&Privacy Policy
Your Cart
Subtotal₹0
Total₹0
Examoogle • User • info@examoogle.com • EE-2024-8821
Chapter 1 of 12 • Page 1 of 248🔒 Protected PDF • Watermarked
Back to Practice Questions
ElectricalElectronics
PrevNext

The electrons in the conduction band are known as _____.

A

Bound electrons

B

Valence electrons

C

Free electrons

D

None of the above

Correct Answer

Concept & PrincipleElectricalElectronics
Option C

Free electrons

Quick Summary: Electrons in the conduction band have gained sufficient energy to break free from their parent atoms, making them available for charge conduction. Consequently, they are referred to as free electrons as they are not restricted to a specific atomic site and can move through the crystal lattice under an applied electric field.

💡 Explanation

Electrons in the conduction band have gained sufficient energy to break free from their parent atoms, making them available for charge conduction. Consequently, they are referred to as free electrons as they are not restricted to a specific atomic site and can move through the crystal lattice under an applied electric field.

🔢 Key Formulas

Eg=Ec−EvE_g = E_c - E_vEg​=Ec​−Ev​ — Energy bandgap defined by the difference between conduction band edge EcE_cEc​ and valence band edge EvE_vEv​

J=nevdJ = n e v_dJ=nevd​ — Current density where nnn is the density of free electrons, eee is electronic charge, and vdv_dvd​ is drift velocity

⚙️ Working Principle

In a semiconductor, the valence band is filled with electrons bound to atoms. When thermal energy or doping provides energy greater than the bandgap EgE_gEg​, electrons are promoted to the conduction band. Once in the conduction band, the potential energy landscape allows these electrons to act as mobile charge carriers, facilitating electrical current flow.

📌 Key Points
  • ▸

    Free electrons are the primary charge carriers in n-type semiconductors.

  • ▸

    The mobility of free electrons is typically higher than that of holes.

  • ▸

    An electron must absorb energy equal to or greater than EgE_gEg​ to become a free electron.

  • ▸

    At T=0KT = 0 KT=0K, there are no free electrons in an intrinsic semiconductor.

✅ Advantages
  • ▸

    High conductivity when carriers are available

  • ▸

    Allows for control of current via external bias

❌ Disadvantages / Limitations
  • ▸

    Highly dependent on temperature

  • ▸

    Sensitivity to impurities (dopants)

🛠️ Applications / Uses
  • ▸

    Transistor operation (BJT/FET)

  • ▸

    Photodetectors and LEDs

  • ▸

    P-N junction rectifiers

📄 Additional Information
  • ▸

    Bound electrons are associated with covalent bonds in the valence band.

  • ▸

    Option B is incorrect because valence electrons remain associated with the nucleus and do not contribute significantly to conduction.

📊 Diagram / Illustration
Band Theory ModelConduction Band (Free Electrons)Valence Band (Bound Electrons)
✅

C is correct — Electrons that have transitioned to the conduction band are called free electrons because they are no longer bound to any specific atom and are free to move throughout the crystal lattice.

Core Concepts Used
Click any tag to open in AI Tutor
Energy Band Theory Charge Carrier Dynamics Semiconductor Physics
💡 EXAM TIP

Remember that in conductors, the valence and conduction bands overlap, providing a high density of free electrons even at room temperature.

Related Questions

ElectricalElectronics
Calculate the critical current through a long thin superconducting wire of radius 0.5 mm. The critical magnetic
ElectricalElectronics
A superconductor tin has a critical temperature of 3.7 K in zero magnetic field and a critical field of 0.0306 T
ElectricalElectronics
The critical temperature for a metal with isotopic mass 199.5 is 4.185 K. Calculate the isotopic mass if the cri
ElectricalElectronics
For mercury of mass number 202, Tc is 4.2 K. Find the transition temperature for its isotope of mass number 200
ElectricalElectronics
The penetration depth is the __________ where the current drops to 1/e times of its value at the surface.

Discussion (0)

Loading discussion...
PrevNext