Q.Carbon, silicon and germanium have four valence electrons each. These are characterised by valence and conduction bands separated by energy band gap respectively equal to (Eg)C, (Eg)Si and (Eg)Ge. Which of the following statements is true?
Concept understanding — Band Gap Energy
What is Band Gap Energy? — A First Look
Imagine you have a single atom. Its electrons live in specific, fixed energy levels — like rungs on a ladder. You can't put an electron halfway between two rungs; it's either on one rung or another.
Now bring two atoms close together. Their electron rungs interact and split into two slightly different energies. Bring a billion atoms together — as in a solid crystal — and those original rungs spread into continuous bands of allowed energies, separated by gaps where no electron can exist.
That gap — the forbidden region between two bands — is the band gap.
The Intuition: A Wall Between Two Rooms
Think of the valence band as the ground floor of a building — electrons here are tightly bound to atoms, not free to move. The conduction band is the first floor above — electrons here can roam freely through the crystal, carrying current.
The band gap is the height of the ceiling between these two floors. An electron needs exactly that much energy to jump from the valence band to the conduction band. If you give it less energy, it stays stuck on the ground floor. If you give it exactly the gap energy or more, it can leap up and become a mobile charge carrier.
In a metal, the valence and conduction bands overlap — there is no gap. That's why metals conduct electricity so easily: electrons already have free states available at no energy cost.
The Precise Statement
Band gap energy (Eg) is the minimum energy required to excite an electron from the top of the valence band to the bottom of the conduction band in a solid.
Eg=Econduction band minimum−Evalence band maximum
It is measured in electron volts (eV). One eV is the energy gained by an electron when accelerated through a potential difference of 1 volt — a tiny but convenient unit for atomic-scale energies.
Why Does It Matter?
The band gap determines almost everything about how a material behaves electrically and optically:
| Material type | Typical Eg | Behaviour |
|---|---|---|
| Conductor (metal) | Eg=0 (bands overlap) | Electrons flow freely at room temperature |
| Semiconductor | 0.1 eV<Eg<3 eV | Conducts only when given energy (heat, light) |
| Insulator | Eg>3 eV | Almost no conduction at normal conditions |
A quick rule of thumb: if a material is transparent to visible light, its band gap is larger than about 3.1 eV (the energy of violet light). Diamond (Eg≈5.5 eV) is transparent; silicon (Eg≈1.1 eV) is opaque and shiny.
A Concrete Example: Silicon
Silicon has a band gap of 1.12 eV at room temperature. This means:
- An electron in the valence band needs at least 1.12 eV to jump to the conduction band.
- Visible light photons have energies between 1.8 eV (red) and 3.1 eV (violet). So silicon absorbs most visible light — that's why solar cells are dark.
- At absolute zero, silicon is a perfect insulator. At room temperature, thermal energy (~0.025 eV) is far less than 1.12 eV, but a tiny fraction of electrons still get enough energy from random vibrations to jump the gap — giving silicon its useful semiconducting properties.
Do not confuse band gap energy with the work function. The work function is the energy needed to remove an electron entirely from the solid (into vacuum). Band gap is the energy needed to move an electron from one band to another inside the solid.
The Key Takeaway
Band gap energy is the energy threshold that separates insulating behaviour from conducting behaviour in a solid. It explains why diamond is transparent and silicon is not, why copper conducts electricity effortlessly, and why LEDs emit light of a specific colour (the colour corresponds directly to the band gap energy of the semiconductor).
Band gap energy is a key concept from the NCERT Class 12 Physics Semiconductor Electronics chapter that distinguishes conductors, semiconductors, and insulators, and "band gap energy definition and formula" is a frequently searched topic for CBSE board and JEE Main preparation. This concept also connects directly to LED colour and solar-cell design questions that regularly appear in "semiconductor devices important questions" lists.
Why this formula?
Band Gap Energy: Why the Formula Holds
The band gap energy Eg is the energy difference between the top of the valence band and the bottom of the conduction band in a solid. The key formula is:
Eg=Ec−Ev
where Ec is the minimum energy of the conduction band and Ev is the maximum energy of the valence band.
But why does this simple difference matter? The answer lies in how electrons behave in a crystal.
The Origin of Energy Bands
In an isolated atom, electrons occupy discrete energy levels. When atoms come together to form a solid, their atomic orbitals overlap. According to the Pauli exclusion principle, no two electrons can occupy the same quantum state. So the discrete levels split into a continuum of closely spaced levels — an energy band.
The valence band is formed from the outermost (valence) atomic orbitals. The conduction band is formed from the next higher set of orbitals (typically the empty orbitals above the valence orbitals). Between these bands lies the band gap — a region of forbidden energies where no electron states exist.
Why the Formula Eg=Ec−Ev Is Not Trivial
You might think: "Of course the gap is the difference between the bottom of one band and the top of another." But the real insight is that Ec and Ev are not arbitrary points — they are the extrema of the band structure.
In a periodic crystal, the electron energy E(k) depends on the wavevector k. The valence band has its maximum at some k-point (often at k=0 for direct-gap semiconductors), and the conduction band has its minimum at some k-point. The band gap is:
Eg=minkcEc(kc)−maxkvEv(kv)
This is not just a difference — it's a minimisation over all possible electron momenta.
Why This Difference Determines Conductivity
The band gap controls whether a material is an insulator, semiconductor, or conductor because of the Fermi-Dirac distribution:
f(E)=1+e(E−EF)/kBT1
At absolute zero, all states below the Fermi level EF are filled, and all above are empty. For an intrinsic semiconductor, EF lies in the middle of the band gap. The probability that an electron is thermally excited from the valence band to the conduction band is proportional to e−Eg/2kBT.
The band gap energy Eg appears in the exponent of the carrier concentration formula:
n=p=NcNve−Eg/2kBT
This is why a small change in Eg causes a huge change in conductivity — it's an exponential dependence.
The Physical Meaning of Eg
The band gap is not just a number — it's the minimum energy required to:
- Break a covalent bond in the crystal (creating an electron-hole pair)
- Promote an electron from a bonding state to an antibonding state
- Create a mobile charge carrier
For example, in silicon (Eg=1.12 eV at 300 K), a photon with energy greater than 1.12 eV can be absorbed, exciting an electron from the valence band to the conduction band. This is why silicon is used in solar cells — the band gap matches the solar spectrum.
A common mistake is to think the band gap is simply the difference between the highest and lowest energy levels in the solid. It is not — it is the gap between the top of the filled valence band and the bottom of the empty conduction band. The bands themselves can be several eV wide.
Why Different Materials Have Different Band Gaps
The band gap depends on:
- Atomic spacing: Closer atoms → more orbital overlap → wider bands → smaller gap (or even no gap)
- Atomic number: Heavier atoms have more diffuse orbitals → more overlap → smaller gap
- Crystal structure: Diamond (indirect gap) vs. zinc blende (direct gap) affect the nature of the gap
The tight-binding model gives a simple derivation: for a 1D chain of atoms with nearest-neighbour hopping integral t, the band width is 4t, and the gap between bands depends on the difference in on-site energies Δ and the hopping integrals:
Eg=Δ2+4t2−2t
This shows that the gap is not simply the atomic energy difference — it's modified by the overlap between orbitals.
The Bottom Line
The formula Eg=Ec−Ev is deceptively simple. It captures the fundamental quantum mechanical result that electrons in a periodic potential have allowed and forbidden energy regions. The band gap is the energy threshold that separates insulating behaviour from conducting behaviour, and it determines virtually all optical and electronic properties of semiconductors.
Concept: Band Gap Energy — the energy gap between the valence and conduction bands determines whether a material behaves as an insulator, semiconductor, or conductor. For group 14 elements, the band gap decreases as we move down the group.
Reasoning:
- Carbon (diamond) is an insulator with a very large band gap (~5.5 eV).
- Silicon and germanium are semiconductors; their band gaps are smaller and decrease down the group: Si (~1.1 eV), Ge (~0.7 eV).
- Therefore, the order is: (Eg)C>(Eg)Si>(Eg)Ge.
The correct statement is (c): (Eg)C>(Eg)Si>(Eg)Ge.
The band gap energy decreases as we move down Group 14 in the periodic table. Carbon (diamond) has the largest gap, silicon a smaller one, and germanium the smallest. The correct order is (Eg)C>(Eg)Si>(Eg)Ge, which corresponds to option (c).
The key idea here is that the band gap energy in semiconductors and insulators is not arbitrary — it is directly linked to the strength of the covalent bond and the size of the atom. Carbon, silicon, and germanium all belong to Group 14 and have four valence electrons each. In their solid state, they form a diamond-like crystal structure where each atom is covalently bonded to four neighbours.
Why does the band gap change as we go down the group? The valence electrons in a solid occupy bands — the valence band (filled with bonding electrons) and the conduction band (empty, higher energy). The energy gap between them, Eg, is the minimum energy needed to promote an electron from a bonding state to a conducting state. A larger gap means the material is more insulating; a smaller gap means it is more semiconducting.
The trend is governed by two factors that work together:
-
Atomic size and bond length: As we go from C to Si to Ge, the atomic radius increases. This means the distance between neighbouring atoms in the crystal also increases. A longer bond is weaker — the shared electrons are less tightly held. This reduces the splitting between bonding and antibonding energy levels, which directly shrinks the band gap.
-
Electronegativity: Carbon is the most electronegative in the group. It holds its valence electrons very tightly, requiring more energy to free them. Silicon and germanium are less electronegative, so their electrons are more easily excited into the conduction band.
The result is a clear, monotonic decrease: diamond (carbon) has a band gap of about 5.5 eV (making it an insulator), silicon has about 1.1 eV, and germanium has about 0.67 eV. So the order is (Eg)C>(Eg)Si>(Eg)Ge.
A common mistake is to think that because germanium is "heavier" it must have a larger gap. In fact, heavier atoms have more diffuse orbitals and weaker bonds, which reduce the gap. The trend is opposite to atomic mass.
Now let’s check the options:
-
Option (a) says (Eg)Si<(Eg)Ge<(Eg)C. This is wrong because it places germanium’s gap above silicon’s — the actual order is the reverse.
-
Option (b) says (Eg)C<(Eg)Ge>(Eg)Si. This is nonsense — it claims carbon has the smallest gap, which is completely false, and also gives germanium the largest, which is also false.
-
Option (c) says (Eg)C>(Eg)Si>(Eg)Ge. This matches the known trend exactly.
-
Option (d) says all three are equal. This is clearly wrong — the materials have very different electrical properties (diamond is an insulator, silicon and germanium are semiconductors).
You can remember the trend as: higher up in Group 14 → larger band gap. Carbon (top) is an insulator, silicon and germanium (below) are semiconductors, and tin/lead (further down) are metals (zero gap). This is a classic periodic property.
The correct option is (c).
Method: Trend Analysis Using Periodic Table Position
The band gap energy of an element depends on how tightly the valence electrons are bound to the nucleus. For elements in the same group (Group 14: C, Si, Ge), as you go down the group, the atomic size increases and the valence electrons become less tightly held. This means less energy is needed to jump from the valence band to the conduction band — so the band gap decreases.
Steps:
- Identify the group: Carbon, silicon, and germanium all belong to Group 14 of the periodic table.
- Recall the order of increasing atomic size: C (smallest) → Si → Ge (largest).
- Larger atoms have weaker hold on valence electrons → smaller band gap.
- Therefore, band gap decreases as we move down the group: C has the largest gap, Ge the smallest.
The correct order is:
(Eg)C>(Eg)Si>(Eg)Ge
Answer: Option (c)
Common Mistakes Students Make on This Band Gap Question
Mistake 1: Confusing the trend of band gap with atomic size
Many students think that since carbon is smaller than silicon, and silicon smaller than germanium, the band gap should follow the same order — decreasing with size. That part is actually correct. The mistake comes from reversing the inequality or mixing up which element has the largest gap.
Carbon (diamond) has the largest band gap (~5.5 eV), germanium the smallest (~0.67 eV), and silicon sits in between (~1.12 eV). So the correct order is:
(Eg)C>(Eg)Si>(Eg)Ge
That matches option (c).
Mistake 2: Thinking band gap increases down the group
Some students memorise that conductivity increases down Group 14 (C → Si → Ge → Sn → Pb) and then incorrectly conclude that band gap must also increase. This is backwards. Conductivity increases because band gap decreases — more electrons can jump to the conduction band at room temperature.
Higher conductivity does NOT mean higher band gap. They are inversely related for intrinsic semiconductors.
Mistake 3: Forgetting that carbon (diamond) is an insulator
Carbon in its diamond form has a band gap so large (~5.5 eV) that at room temperature, almost no electrons cross it. That makes it an insulator, not a semiconductor. Students sometimes treat all four elements as semiconductors and then guess wrong.
Diamond (carbon) is an insulator. Silicon and germanium are semiconductors. This alone tells you carbon's band gap is much larger than the other two.
Mistake 4: Picking option (a) because it "looks like" a decreasing trend
Option (a) says (Eg)Si<(Eg)Ge<(Eg)C. This has silicon's gap smaller than germanium's — which is false. The actual decreasing order is C > Si > Ge. Students who vaguely remember "band gap decreases down the group" sometimes write the elements in the wrong sequence.
How to avoid: Always write the elements in order of increasing atomic number: C (6), Si (14), Ge (32). Then recall that band gap decreases as atomic size increases. So C has the largest, Ge the smallest.
Mistake 5: Not recognising that option (b) is nonsense
Option (b) says (Eg)C<(Eg)Ge>(Eg)Si. This claims carbon's gap is smaller than germanium's — which is wildly wrong. Yet some students pick it because they see a "greater than" sign and think it matches some trend they half-remember.
How to avoid: Test the extreme values. If you know diamond is an insulator and germanium is a semiconductor, then carbon's gap must be larger. Any option that says otherwise is automatically wrong.
Final answer: Option (c) (Eg)C>(Eg)Si>(Eg)Ge is correct.
- AP EAPCET 2026Set eng-2026-05-13-FN1 markMCQQ.The minimum energy gap of a semi-conductor used in manufacturing LED is (A) 3 eV (B) 3.6 eV (C) 2.8 eV (D) 1.8 eV
›Reveal solutionSolution
This tests the standard semiconductor-electronics fact (NCERT) that LED materials need Eg≥1.8 eV to emit visible light, since Eg=hc/λ and the visible spectrum's red edge (∼700 nm) sets this lower bound.
Concept and Intuition
In an LED, forward biasing causes electron-hole recombination at the junction, and each recombination releases a photon whose energy roughly equals the semiconductor's band gap Eg. For the emitted light to be visible (400–700 nm), the photon energy must be at least as large as the energy corresponding to the longest visible wavelength (red, ∼700 nm), since longer wavelength = lower photon energy. This is why ordinary Si or Ge junctions (small gaps) emit only infrared, while LED materials (GaAs, GaP, GaAsP etc.) are chosen with larger gaps.
Step-by-Step Solution
- Photon energy and wavelength are related by E=λhc.
- The longest (least energetic) visible wavelength is about λ≈700 nm =700×10−9 m.
- Compute the corresponding energy: E=700×10−9(6.63×10−34)(3×108)≈2.84×10−19 J ≈1.77 eV.
- So the semiconductor's band gap must be at least ≈1.8 eV for the emitted radiation to fall within (or above, moving toward blue/violet) the visible range — this is the standard quoted minimum energy gap for LED semiconductors.
Common Mistakes
- Confusing this with the Si/Ge band gaps (1.1 eV / 0.7 eV), which are too small and would only give infrared emission, not visible LED light.
- Picking a much larger number (like 3 or 3.6 eV) — those overshoot into the UV end and are not the minimum required gap.
✓Final answerThe correct option is (D) — 1.8 eV.
ANSWER: D
- AP EAPCET 2025Set eng-2025-05-22-FN1 markMCQQ.A cc camera is fabricated using a semiconducting material having a band gap of 3 eV. The wavelength of light it can detect is nearly (A) 210 nm (B) 546 nm (C) 413 nm (D) 345 nm
›Reveal solutionSolution
Tests the photon-energy/band-gap relation for a photodetector; the threshold wavelength is λ=hc/Eg.
Concept and Intuition
A semiconductor detector (like a CCD) can only detect photons whose energy is at least equal to the band gap Eg, since an electron must be excited from the valence band to the conduction band. The longest wavelength (lowest energy) it can detect is the threshold wavelength corresponding exactly to Eg.
Step-by-Step Solution
- Use the convenient relation E(eV)=λ(nm)1240 eV⋅nm, derived from E=hc/λ with hc≈1240 eV·nm.
- Given Eg=3 eV, solve for λ: λ=31240=413.3 nm.
- This matches option (C), 413 nm.
Common Mistakes
- Forgetting to use hc=1240 eV·nm and instead mixing up units (Joules vs eV) without converting, leading to a wrong power of ten.
- Confusing this with the minimum detectable wavelength instead of maximum — the band gap sets the longest wavelength (lowest energy) detectable, not the shortest.
✓Final answerThe correct option is (C) — 413 nm.
ANSWER: C
- AP EAPCET 2024Set ap-2024-05-16-FN1 markMCQQ.Semiconductors suitable for solar cell fabrication have a band gap nearby (A) 0.015 eV (B) 1.5 eV (C) 15 eV (D) 150 eV
›Reveal solutionSolution
Solar cells are made from semiconductors whose band gap is close to 1.5 eV, matched to the peak of the solar spectrum's usable photon energies.
Concept and Intuition
A semiconductor absorbs a photon and creates an electron-hole pair only if the photon's energy exceeds the band gap Eg. Too small a gap wastes photon energy as heat; too large a gap means many solar photons don't have enough energy to be absorbed at all. The band gaps of practical solar-cell materials (silicon ~1.1 eV, GaAs ~1.4 eV) cluster near the value that gives the best trade-off, commonly quoted in textbooks as approximately 1.5 eV.
Step-by-Step Solution
- Recall that a good photovoltaic material needs Eg neither too small (excess thermalisation losses) nor too large (many photons below threshold, unabsorbed).
- Real solar-cell semiconductors (Si, GaAs) have band gaps in the 1–1.5 eV range.
- Among the choices, 0.015 eV is far too small (that's an infrared/microwave photon energy scale), and 15 eV, 150 eV are far too large (X-ray/UV scale, essentially no solar photons have that much energy).
- The physically reasonable value is 1.5 eV.
Common Mistakes
- Confusing band gap energy scale with photon energies of visible light (~1.8–3.1 eV) — solar cells are optimised slightly below this range to capture more of the broad solar spectrum including infrared.
- Picking an order-of-magnitude-wrong option without sanity-checking against known semiconductor band gaps.
✓Final answerThe correct option is (B) — 1.5 eV.
ANSWER: B
- AP EAPCET 2024Set eng-2024-05-20-AN1 markMCQQ.If the energy gap of a substance is 5.4 eV, then the substance is (A) Insulator (B) Conductor (C) p-type semiconductor (D) n-type semiconductor
›Reveal solutionSolution
A band gap as large as 5.4 eV is far too wide for thermal excitation across it at room temperature — this is the signature of an insulator, not a semiconductor or conductor.
Concept and Intuition
In band theory, electrical conduction depends on how easily electrons can be promoted from the filled valence band to the empty conduction band. In conductors, the bands overlap (or the conduction band is partially filled), so no gap needs to be crossed. In semiconductors, a small gap (roughly under 3 eV) allows some thermal or doping-assisted excitation, giving moderate conductivity. In insulators, the gap is large (several eV), so essentially no electrons can be thermally promoted across it at ordinary temperatures, and the material does not conduct.
Step-by-Step Solution
- Note the given band gap: Eg=5.4 eV.
- Compare against typical benchmarks: semiconductors like Si (1.1 eV) and Ge (0.7 eV) have gaps well under 3 eV; classic insulators like diamond have gaps around 5.4–5.5 eV.
- Since 5.4 eV matches the insulator range (and is far above semiconductor values), the substance must be an insulator.
Common Mistakes
- Assuming any nonzero gap automatically means "semiconductor" — the size of the gap is what distinguishes semiconductors from insulators.
- Confusing p-type/n-type (doped semiconductor classifications) with the intrinsic band-gap size question being asked here.
✓Final answerThe correct option is (A) — Insulator.
ANSWER: A
- AP EAPCET 2024Set eng-2024-05-21-FN1 markMCQQ.The semiconductor used for fabrication of visible LEDs must at least have a band gap of (A) 0.6 eV (B) 1.2 eV (C) 1.8 eV (D) 0.9 eV
›Reveal solutionSolution
The band gap sets the photon energy (and hence colour) an LED emits; to reach even the lowest-energy visible colour (red, ~700 nm), the gap must be at least about 1.8 eV.
Concept and Intuition
An LED emits photons with energy approximately equal to its semiconductor's band gap (Eg≈hc/λ). Visible light ranges from about 700 nm (red, lowest photon energy) to 400 nm (violet, highest photon energy). A material with too small a band gap would only emit infrared, not visible light — so for any visible-light LED to be possible at all, the minimum acceptable band gap corresponds to the least energetic visible colour, red.
Step-by-Step Solution
- Longest visible wavelength (least energetic, sets the floor): λ≈700 nm.
- Photon energy: E=λhc=700 nm1240 eV⋅nm≈1.77 eV ≈1.8 eV.
- So the band gap must be at least about 1.8 eV for the semiconductor to be usable for a visible LED.
Common Mistakes
- Using the violet/blue end (400 nm, ~3.1 eV) instead of red — that would give the maximum photon energy, not the minimum band-gap threshold for visibility.
- Forgetting the handy shortcut E(eV)=1240/λ(nm).
✓Final answerThe correct option is (C) — 1.8 eV.
ANSWER: C
- AP EAPCET 2023Set eng-2023-05-15-AN1 markMCQQ.The material used in the fabrication of infrared LED's is (A) silicon (B) germanium (C) gallium arsenide phospide (D) carbon dioxide
›Reveal solutionSolution
This tests which semiconductor material family is used to fabricate LEDs; compound semiconductors like gallium arsenide phosphide are used, not elemental Si/Ge.
Concept and Intuition
An LED needs a direct band-gap semiconductor so that when an electron recombines with a hole across the junction, the energy is released efficiently as a photon rather than being lost as heat (phonons). Silicon and germanium are elemental semiconductors with an indirect band gap, so they recombine radiation very inefficiently and are not used for light-emission (they are used for diodes/transistors, not LEDs). Compound semiconductors formed from group III and group V elements — such as gallium arsenide (GaAs) and its phosphide-doped variants (GaAsP) — have direct band gaps and can be tuned by varying composition to emit anywhere from infrared through visible colours.
Step-by-Step Solution
- Rule out silicon and germanium: both are elemental, indirect-band-gap semiconductors, used for diodes/transistors but not efficient light emitters.
- Rule out carbon dioxide: this is a gas, not a semiconductor, and plays no role in LED fabrication.
- The remaining option, gallium arsenide phosphide, is a III–V compound semiconductor family used industrially to fabricate LEDs (with composition tuned for different emission wavelengths, including the infrared end of the family).
Common Mistakes
- Assuming any semiconductor works for LEDs — direct band gap is essential, which rules out Si and Ge.
- Overlooking that CO2 is not a solid-state material at all.
✓Final answerThe correct option is (C) — gallium arsenide phospide.
ANSWER: C
- AP EAPCET 2022Set eng-2022-07-06-FN1 markMCQQ.The energy of a photon in a monochromatic light of wavelength 621 nm matches with the band gap of a semiconducting material. Then the minimum energy required to create an electron-hole pair from the semiconductor is [Take hc = 1242 eV – nm, where h is Planck's constant and c is speed of light in vacuum] (A) 3.4 eV (B) 1.7 eV (C) 2 eV (D) 2.2 eV
›Reveal solutionSolution
A straightforward E=hc/λ calculation, using the given hc=1242 eV·nm shortcut, gives exactly 2 eV — and since the problem tells us this photon energy matches the band gap, that band-gap energy is the minimum energy needed to create an electron-hole pair.
Concept and Intuition
In a semiconductor, an electron can be excited from the valence band to the conduction band (creating an electron-hole pair) only if it absorbs at least the band-gap energy Eg. A photon with exactly this energy is the threshold case — the minimum energy photon capable of creating a pair. Since the problem states the photon's energy equals the band gap, computing the photon energy directly gives us Eg, the minimum pair-creation energy.
Step-by-Step Solution
- Photon energy: E=λhc, using the convenient constant hc=1242 eV·nm.
- E=6211242=2 eV.
- Since this equals the band gap by the problem's premise, the minimum electron-hole pair creation energy is also 2 eV.
Common Mistakes
- Forgetting to use the eV·nm form of hc and instead mixing SI units (J, m) inconsistently, leading to unit-conversion errors.
- Overthinking the question — no additional physics (like exciton binding energy) is implied here; it's a direct application of E=hc/λ.
✓Final answerThe correct option is (C) — 2 eV.
ANSWER: C
- AP EAPCET 2022Set eng-2022-07-08-AN1 markMCQQ.The class of materials having the largest band gap in the following is (A) Metals (B) Semi-metals (C) Semi-Conductors (D) Insulators
›Reveal solutionSolution
Band gap size increases from metals (essentially zero) through semiconductors to insulators, which have the largest band gap — that is exactly what makes them insulators.
Concept and Intuition
In band theory of solids, electrical conductivity is governed by the energy gap between the filled valence band and the empty conduction band. Metals have overlapping or touching bands (zero or negligible gap), so electrons move freely — high conductivity. Semiconductors have a small but nonzero gap (~1 eV for Si/Ge), so only a few electrons are thermally promoted across it at room temperature. Insulators have a very large band gap (several eV, e.g., diamond ~5.5 eV), so essentially no electrons can be thermally excited into the conduction band — this large gap is the defining reason they don't conduct.
Step-by-Step Solution
- Compare typical band gaps: metals ≈ 0 eV, semiconductors ≈ 0.7–1.5 eV, insulators ≈ several eV (often > 3 eV).
- "Semi-metals" have a very small or zero gap too, similar to metals.
- The largest band gap among the listed classes belongs to insulators.
Common Mistakes
- Confusing semiconductors with insulators — semiconductors have a small gap, not the largest.
- Assuming metals have the largest gap because they're "more common" or "denser" — conductivity is about gap size, and metals have essentially none.
✓Final answerThe correct option is (D) — Insulators.
ANSWER: D
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