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L-25: Dual Nature of Radiation and Matter

Physics — Class 12 · NIOS Code 312 · Module 7 · Source: 312_Physics_Eng_Lesson25.pdf

Dual Nature of Radiation and Matter

Light and matter exhibit both wave-like and particle-like behaviour under different conditions. This lesson covers the photoelectric effect (Einstein's photon theory), photoelectric tubes, de Broglie's matter waves, and their experimental verification. Module 7: Atoms and Nuclei.

NIOS objectives: photoelectric effect and laws; Einstein's equation; de Broglie wavelength; Davisson–Germer experiment.

25.1 Photoelectric Effect

Discovered by Hertz (1887); electrons emitted from metal when light of sufficiently high frequency falls on it — photoelectrons. Distinct from thermionic emission (electrons gain energy from heat, not photons).

Fig 25.1 — Photoelectric Effect Apparatus cathode C photoelectrons anode A light S µA Evacuated tube · A positive → collect electrons · A negative → stopping potential
Fig 25.1 — Photocathode C emits electrons when irradiated; current measured by microammeter

Experimental Observations (Millikan)

  • Kmax (hence stopping potential V₀) increases with frequency ν; independent of intensity.
  • Threshold frequency ν₀ exists below which no emission occurs (material property).
  • Number of photoelectrons per unit area ∝ intensity of light (at fixed ν).
  • Emission is instantaneous (~10⁻⁹ s time lag).
  • Saturation current reached when all emitted electrons are collected (Vs).
eV₀ = ½mv²max = Kmax
V₀ = stopping (cut-off) potential for given ν
Work done against retarding field equals max KE
Graph V₀ vs ν: slope = h/e; x-intercept = ν₀
Fig 25.3–25.4 — Stopping Potential & Photocurrent frequency ν V₀ ν₀ higher ν → higher V₀ I_sat Stopping potential independent of intensity · saturation I ∝ intensity
Fig 25.3–25.4 — Linear V₀–ν relation above threshold; higher ν needs greater retarding potential

25.2 Einstein's Theory of Photoelectric Emission

Light consists of discrete energy bundles — photons. Photoelectric effect = collision between one photon and one bound electron.

E = hν  |  hν = φ₀ + Kmax
φ₀ = work function (minimum energy to eject electron)
φ₀ = hν₀ (threshold frequency)
Kmax = h(ν − ν₀) when ν > ν₀

Work functions (eV): Na 2.5, K 2.3, Zn 3.4, Fe 4.8, Ni 5.9.

Einstein explains: no emission below ν₀; Kmax linear in (ν − ν₀); higher intensity → more photons → more electrons (not higher Kmax); instantaneous transfer; ν₀ depends on material only. Millikan verified Einstein's equation and measured h.

pphoton = h/λ = hν/c
Photon momentum from de Broglie relation
If λ doubles, photon energy E = hc/λ halves
Doubling intensity does not change Kmax

25.3 Photoelectric Tube

Evacuated glass tube: semi-cylindrical cathode (low-work-function coating) + wire anode. Variable accelerating voltage; saturation current ~ nA, proportional to light intensity. Used in cinema sound reproduction, photo-telegraphy, burglar/fire alarms, TV cameras, traffic detectors.

Fig 25.5 — Photoelectric Tube I–V Curve accelerating voltage current I I₁ high I I₂ low I Current saturates · higher intensity → higher I_sat (not V₀)
Fig 25.5 — Photocurrent vs voltage; saturation level set by light intensity

25.4 de Broglie Hypothesis

If light (wave) shows particle nature (photon), matter particles should show wave nature. Symmetry argument + E = mc² reasoning.

λ = h/p = h/(mv)
λ = de Broglie wavelength
Particle momentum p ↔ wave property λ
Converse: wave of λ has momentum p = h/λ
λ = h/√(2qmV) = 12.3/√V Å  (electron)
Electron accelerated through potential V (volts)
½mv² = qV → p = √(2qmV)
100 V electron: λ = 1.23 Å (X-ray range, ~ atomic spacing)

Macroscopic objects (cricket ball): λ imperceptibly small (~10⁻³² m for 50 g ball at 20 cm/s). de Broglie waves observable only for microscopic particles.

25.4.1 Davisson–Germer Experiment (1927)

Electron beam (controlled by accelerating voltage) incident on nickel crystal; detector at angle θ measures scattered intensity. Peak at 54 eV, θ = 50° → λ ≈ 1.67 Å — matches de Broglie prediction. First direct evidence of matter waves (electron diffraction).

Fig 25.6 — Davisson–Germer Experiment electron gun Ni crystal Dₜ diffracted beam (θ) Crystal lattice acts as diffraction grating · Nobel 1937 (Davisson & G.P. Thomson)
Fig 25.6 — Electron diffraction by crystal confirms λ = h/p for matter

25.4.2 Applications — Electron Microscope

Resolution improves with shorter wavelength. Electrons at high KE have λ much smaller than visible light → electron microscopes achieve 10,000×+ magnification vs optical limit ~1000×. TEM (1931, Knoll & Ruska): electron beam through specimen, magnetic lenses, phosphor screen — analogous to light microscope but with electrons.

         DUAL NATURE — KEY POINTS
         ===========================
    Photoelectric     :  hν = φ₀ + Kmax ; emission if ν > ν₀
    Stopping pot.     :  eV₀ = Kmax ; V₀ ∝ ν (slope h/e)
    Intensity effect  :  more electrons, same Kmax
    Photon energy     :  E = hν ; p = hν/c
    de Broglie        :  λ = h/p = h/(mv)
    Electron (V vol)  :  λ = 12.3/√V Å
    Davisson–Germer   :  electron diffraction → matter waves
    Phototube uses    :  cinema sound, alarms, photo-telegraphy

Quick Revision

  • Classical wave theory failed: instant emission, threshold frequency, intensity independence of Kmax.
  • One photon ejects at most one electron (for given frequency).
  • Stopping potential graph: x-intercept ν₀, slope h/e.
  • de Broglie: moving particles, not stationary ones, have matter waves.
  • 100 eV electrons: λ ≈ 1.23 Å — suitable for crystal diffraction studies.
20 cards · click any card to flip
Photoelectric effect
Emission of electrons from metal surface when light of frequency above threshold ν₀ is incident. Electrons called photoelectrons. Discovered by Hertz; explained by Einstein (1905).
Thermionic vs photoelectric emission
Thermionic: electrons gain energy from heat. Photoelectric: electrons gain energy from incident photons (light). Different mechanisms.
Stopping potential V₀
Minimum retarding potential that stops all photoelectrons for a given ν. eV₀ = Kmax = ½mv²max. Increases with frequency ν.
Threshold frequency ν₀
Minimum frequency below which no photoelectrons are emitted. Material-specific. Related to work function: φ₀ = hν₀.
Work function φ₀
Minimum energy needed for electron to escape metal surface. Typical values: Na 2.5 eV, K 2.3 eV, Zn 3.4 eV, Ni 5.9 eV.
Einstein's photoelectric equation
hν = φ₀ + Kmax. Photon energy = work function + max kinetic energy of ejected electron. Kmax = h(ν − ν₀).
Effect of light intensity
At fixed ν: more photons → more photoelectrons → higher photocurrent. Kmax unchanged. Saturation current ∝ intensity.
Effect of frequency
Higher ν → higher Kmax and higher stopping potential V₀. Independent of intensity. Must exceed ν₀ for any emission.
Photon energy and momentum
E = hν = hc/λ. Momentum p = h/λ = hν/c. If λ doubles, E halves. Massless energy packet of light.
V₀ vs ν graph
Linear above ν₀. Slope = h/e. x-intercept = ν₀ (threshold). y-intercept related to −hν₀/e. Millikan verified this.
Why photoelectric effect is instantaneous?
Single photon–electron collision transfers energy in one step. Time lag ~10⁻⁹ s. No need to accumulate energy over time (unlike classical theory).
Photoelectric tube
Evacuated tube with photosensitive cathode (low φ₀ coating) and anode. Converts light to electric current. Saturation current ~ nA, ∝ intensity.
Applications of photoelectric cell
Cinema sound reproduction, photo-telegraphy, burglar/fire alarms, TV camera scanning, traffic law detection, counting systems.
Wave-particle duality
Same entity shows wave properties (interference, diffraction) and particle properties (photoelectric effect, momentum) under different conditions.
de Broglie wavelength
λ = h/p = h/(mv). Every moving particle has associated matter wave. Submitted as Ph.D thesis (1924); Nobel 1929.
Electron wavelength formula
λ = h/√(2qmV) = 12.3/√V Å. Example: V=100 → λ=1.23 Å. V=182 → λ=0.91 Å. Comparable to atomic spacings.
Why no de Broglie waves for cricket ball?
λ = h/(mv). Large mass m → λ extremely small (~10⁻³⁴ m order), far below detectable scale. Quantum effects only for microscopic particles.
Davisson–Germer experiment
Electrons scattered from Ni crystal show diffraction peaks. 54 eV electrons at θ=50° gave λ≈1.67 Å matching h/p. Confirmed matter waves (1927).
Electron microscope advantage
Shorter de Broglie λ than visible light → much higher resolution and magnification (10,000×+). TEM uses magnetic lenses and electron beam through specimen.
Classical theory failures
Could not explain: (1) existence of threshold frequency, (2) Kmax independent of intensity, (3) instantaneous emission, (4) linear V₀–ν relation.

Q1. In photoelectric emission, electrons gain energy from:

Q2. Einstein's photoelectric equation is:

Q3. If the intensity of incident light is doubled (frequency fixed), Kmax of photoelectrons:

Q4. The slope of the graph between stopping potential V₀ and frequency ν is:

Q5. The work function of a metal depends on:

Q6. de Broglie wavelength of a particle is given by:

Q7. An electron accelerated through 100 V has de Broglie wavelength approximately:

Q8. Davisson–Germer experiment demonstrated:

Q9. Saturation current in a phototube depends on:

Q10. If the wavelength of electromagnetic radiation is doubled, photon energy:

eV₀ = K_max = ½mv²_max
E = hν = hc/λ
hν = φ₀ + K_max
φ₀ = hν₀
K_max = h(ν − ν₀)
V₀ = (h/e)(ν − ν₀)
p = h/λ = hν/c
λ = h/p = h/(mv)
λ = h/√(2qmV) = 12.3/√V Å
½mv² = qV
I_sat ∝ intensity (fixed ν)

1. Formulas & Definitions

Full Ch 25 study guide — photoelectric effect, Einstein's equation, photons, and de Broglie matter waves.

eV₀ = K_max = ½mv²_max

Definition: Stopping potential — retarding field work equals maximum photoelectron kinetic energy.

Derivation

Minimum negative potential V₀ that stops fastest photoelectrons for given frequency ν.

Variables

V₀ = stopping (cut-off) potential · K_max in joules or eV

Why it works

Experimental measure of K_max; linear V₀–ν graph verifies Einstein's theory.

Historical context

Millikan verified slope h/e and measured Planck's constant.

Deep understanding

V₀ independent of light intensity; depends only on ν for given metal.

2. Diagrams & Visuals

eV₀ = K_max

Color-coded visual · step-by-step breakdown below

  1. Apply retarding potential V₀
  2. Find minimum V₀ stopping all electrons
  3. K_max = eV₀
  4. Plot V₀ vs ν

3. Solved Examples

Basic

Q: V₀=2 V.

Solution: K_max=2 eV

Answer: 2 eV

Intermediate

Q: Double ν?

Solution: V₀ increases

Answer: Not intensity

Advanced

Q: ν < ν₀?

Solution: No emission

Answer: V₀ undefined

Exam

Q: Stopping potential?

Solution: eV₀=K_max

Answer: Sec 25.1

E = hν = hc/λ

Definition: Energy of a single photon of frequency ν or wavelength λ.

Derivation

Light consists of discrete energy quanta (photons), not continuous waves alone.

Variables

h = 6.63×10⁻³⁴ J·s · c = 3×10⁸ m/s

Why it works

Foundation of Einstein's photoelectric explanation.

Historical context

Einstein (1905); Nobel Prize for photoelectric effect.

Deep understanding

If λ doubles, photon energy halves.

2. Diagrams & Visuals

E = hν

Color-coded visual · step-by-step breakdown below

  1. Know frequency ν or wavelength λ
  2. E = hν or hc/λ
  3. Energy per photon
  4. Not total beam energy

3. Solved Examples

Basic

Q: ν=5×10¹⁴ Hz.

Solution: E≈3.3×10⁻¹⁹ J

Answer: ~2 eV

Intermediate

Q: λ=600 nm.

Solution: E≈3.3×10⁻¹⁹ J

Answer: ~2 eV

Advanced

Q: Double ν?

Solution: E doubles

Answer: Linear in ν

Exam

Q: Photon energy?

Solution:

Answer: Sec 25.2

hν = φ₀ + K_max

Definition: Einstein's photoelectric equation — energy conservation in photon–electron collision.

Derivation

Photon energy = work to escape surface + maximum kinetic energy of electron.

Variables

φ₀ = work function (eV or J) · valid when ν > ν₀

Why it works

Explains threshold frequency, linear K_max vs ν, intensity independence of K_max.

Historical context

One photon ejects at most one electron.

Deep understanding

Classical wave theory failed all four key observations.

2. Diagrams & Visuals

hν = φ₀ + K_max

Color-coded visual · step-by-step breakdown below

  1. Photon energy hν
  2. Subtract work function φ₀
  3. Remainder = K_max
  4. Require ν > ν₀

3. Solved Examples

Basic

Q: hν=5 eV, φ₀=2 eV.

Solution: K_max=3 eV

Answer: 3 eV

Intermediate

Q: hν=φ₀?

Solution: K_max=0

Answer: Threshold

Advanced

Q: hν<φ₀?

Solution: No emission

Answer: Below ν₀

Exam

Q: Einstein equation?

Solution: hν=φ₀+K_max

Answer: Sec 25.2

φ₀ = hν₀

Definition: Work function — minimum energy to eject electron from metal surface.

Derivation

Threshold frequency ν₀ is minimum ν for photoelectric emission; φ₀ = hν₀.

Variables

φ₀ in eV · material property (Na 2.5, Ni 5.9 eV)

Why it works

Different metals have different ν₀ and φ₀.

Historical context

Independent of light intensity; depends on surface material.

Deep understanding

Coating cathode with low-φ material improves phototube sensitivity.

2. Diagrams & Visuals

φ₀ = hν₀

Color-coded visual · step-by-step breakdown below

  1. Identify metal
  2. Find threshold ν₀
  3. φ₀ = hν₀
  4. Or use tabulated φ₀ in eV

3. Solved Examples

Basic

Q: ν₀=6×10¹⁴ Hz.

Solution: φ₀≈2.5 eV

Answer: ~2.5 eV

Intermediate

Q: Na φ₀=2.5 eV.

Solution: Lower ν₀ needed

Answer: Easier emission

Advanced

Q: Intensity effect on φ₀?

Solution: None

Answer: Material only

Exam

Q: Work function?

Solution: hν₀

Answer: Sec 25.2

K_max = h(ν − ν₀)

Definition: Maximum photoelectron kinetic energy above threshold frequency.

Derivation

Rearrangement of hν = φ₀ + K_max with φ₀ = hν₀.

Variables

Linear in (ν − ν₀) · slope h when K in J

Why it works

Direct prediction tested by Millikan's V₀–ν experiments.

Historical context

K_max unchanged when intensity doubles.

Deep understanding

Higher ν → higher K_max, not higher intensity.

2. Diagrams & Visuals

ν₀ K_max ∝ (ν−ν₀)

Color-coded visual · step-by-step breakdown below

  1. Find ν and ν₀
  2. K_max = h(ν−ν₀)
  3. Or K_max = hν−φ₀
  4. Convert to eV if needed

3. Solved Examples

Basic

Q: ν=8×10¹⁴, ν₀=5×10¹⁴ Hz.

Solution: K_max=h×3×10¹⁴

Answer: ~1.2 eV

Intermediate

Q: ν=ν₀?

Solution: K_max=0

Answer: Zero

Advanced

Q: Double intensity?

Solution: K_max same

Answer: Key test

Exam

Q: K_max formula?

Solution: h(ν−ν₀)

Answer: Sec 25.2

V₀ = (h/e)(ν − ν₀)

Definition: Linear relation between stopping potential and frequency.

Derivation

From eV₀ = K_max = h(ν−ν₀); slope of V₀–ν graph = h/e.

Variables

x-intercept = ν₀ · y-intercept = −hν₀/e

Why it works

Millikan used this graph to measure h accurately.

Historical context

Linear above ν₀; no emission below ν₀.

Deep understanding

Slope h/e ≈ 4.14×10⁻¹⁵ V·s; universal constant check.

2. Diagrams & Visuals

slope = h/e

Color-coded visual · step-by-step breakdown below

  1. Measure V₀ for various ν
  2. Plot V₀ vs ν
  3. Slope = h/e
  4. x-intercept = ν₀

3. Solved Examples

Basic

Q: Graph slope?

Solution: h/e

Answer: h/e

Intermediate

Q: ν₀ from graph?

Solution: x-intercept

Answer: Threshold

Advanced

Q: Intensity changes slope?

Solution: No

Answer: Same line

Exam

Q: V₀–ν slope?

Solution: h/e

Answer: Sec 25.1

p = h/λ = hν/c

Definition: Momentum of a photon (massless particle of light).

Derivation

de Broglie relation applied to photon; p = E/c for massless particle.

Variables

p (kg·m/s) · photon has momentum despite zero rest mass

Why it works

Radiation pressure; complements particle nature of light.

Historical context

Links photoelectric (energy) and radiation pressure (momentum).

Deep understanding

Shorter λ → higher photon momentum.

2. Diagrams & Visuals

p = hν/c

Color-coded visual · step-by-step breakdown below

  1. Know ν or λ
  2. p = hν/c or h/λ
  3. Momentum of photon
  4. Use in collision problems

3. Solved Examples

Basic

Q: λ=600 nm.

Solution: p≈1.1×10⁻²⁷ kg·m/s

Answer: ~10⁻²⁷

Intermediate

Q: ν doubles?

Solution: p doubles

Answer: p∝ν

Advanced

Q: Rest mass of photon?

Solution: Zero

Answer: Always moves at c

Exam

Q: Photon momentum?

Solution: hν/c

Answer: Sec 25.2

λ = h/p = h/(mv)

Definition: de Broglie wavelength — wave associated with moving particle.

Derivation

Symmetry with photon: if light has particle nature, matter has wave nature.

Variables

λ (m) · p = mv for non-relativistic particles

Why it works

Explains electron diffraction; foundation of quantum mechanics.

Historical context

de Broglie (1924); Nobel 1929; Davisson–Germer confirmed (1927).

Deep understanding

Only moving particles have λ; macroscopic objects have negligible λ.

2. Diagrams & Visuals

λ = h/p

Color-coded visual · step-by-step breakdown below

  1. Find momentum p = mv
  2. λ = h/p
  3. Compare λ to obstacle size
  4. Diffraction if λ ~ spacing

3. Solved Examples

Basic

Q: Electron p=10⁻²⁴.

Solution: λ≈6.6×10⁻¹⁰ m

Answer: ~0.66 nm

Intermediate

Q: Double v?

Solution: λ halves

Answer: λ∝1/v

Advanced

Q: Cricket ball?

Solution: λ~10⁻³⁴ m

Answer: Undetectable

Exam

Q: de Broglie?

Solution: h/p

Answer: Sec 25.4

λ = h/√(2qmV) = 12.3/√V Å

Definition: de Broglie wavelength of electron accelerated through potential V volts.

Derivation

½mv² = qV → p = √(2qmV) → λ = h/p.

Variables

V in volts · q = e for electron · 12.3 Å·V^½ constant

Why it works

Quick calculation for electron diffraction experiments.

Historical context

V=100 V → λ=1.23 Å (atomic/X-ray scale). Davisson–Germer: 54 eV → λ≈1.67 Å.

Deep understanding

Higher V → shorter λ → better electron microscope resolution.

2. Diagrams & Visuals

λ = 12.3/√V Å

Color-coded visual · step-by-step breakdown below

  1. Accelerating voltage V (volts)
  2. λ = 12.3/√V angstrom
  3. Or λ = h/√(2eV×m_e)
  4. Compare to crystal spacing

3. Solved Examples

Basic

Q: V=100 V.

Solution: λ=1.23 Å

Answer: 1.23 Å

Intermediate

Q: V=400 V.

Solution: λ=0.615 Å

Answer: 0.615 Å

Advanced

Q: 4× voltage?

Solution: λ halves

Answer: λ∝1/√V

Exam

Q: Electron λ at V?

Solution: 12.3/√V Å

Answer: Sec 25.4

½mv² = qV

Definition: Kinetic energy gained by charge q accelerated through potential difference V.

Derivation

Work done by electric field W = qV converts to KE (non-relativistic).

Variables

Used to find electron momentum for de Broglie λ

Why it works

Links accelerating voltage in Davisson–Germer to matter wavelength.

Historical context

Electron gun in vacuum tubes and microscopes.

Deep understanding

Combines with λ=h/p to give 12.3/√V formula.

2. Diagrams & Visuals

½mv² = qV

Color-coded visual · step-by-step breakdown below

  1. Charge q, voltage V
  2. KE = qV
  3. p = √(2mqV)
  4. Then λ = h/p

3. Solved Examples

Basic

Q: e, V=50 V.

Solution: KE=50 eV

Answer: 50 eV

Intermediate

Q: Double V?

Solution: KE doubles

Answer: 2qV

Advanced

Q: Proton same V?

Solution: Same KE in eV

Answer: Different λ

Exam

Q: Accelerated particle KE?

Solution: qV

Answer: Sec 25.4

I_sat ∝ intensity (fixed ν)

Definition: Saturation photocurrent proportional to light intensity at fixed frequency.

Derivation

More photons per second → more photoelectrons emitted (one photon, one electron).

Variables

I_sat = saturation current · K_max unchanged

Why it works

Distinguishes intensity effect from frequency effect.

Historical context

Key evidence against classical wave theory predicting K_max ∝ intensity.

Deep understanding

Doubling intensity doubles I_sat but not V₀ or K_max.

2. Diagrams & Visuals

higher I → higher I_sat

Color-coded visual · step-by-step breakdown below

  1. Fix frequency ν > ν₀
  2. Vary intensity
  3. Measure saturation current
  4. I_sat ∝ intensity

3. Solved Examples

Basic

Q: Double intensity.

Solution: I_sat doubles

Answer: 2× current

Intermediate

Q: K_max changes?

Solution: No

Answer: Same ν

Advanced

Q: Below ν₀?

Solution: I_sat=0

Answer: No photons emitted

Exam

Q: Intensity effect?

Solution: I_sat only

Answer: Sec 25.1

5. Special Features & Extras

Complete study guide for Dual Nature of Radiation and Matter.

Exam Tips & Tricks

  • Einstein: hν = φ₀ + K_max — emission only if ν > ν₀.
  • Intensity changes I_sat, NOT K_max or V₀.
  • Frequency changes K_max and V₀, NOT φ₀.
  • V₀–ν graph: slope = h/e, x-intercept = ν₀.
  • Photon: E = hν, p = hν/c — massless.
  • de Broglie: λ = h/p; electron: λ = 12.3/√V Å.
  • 100 V electron: λ ≈ 1.23 Å — crystal diffraction scale.

Common Student Mistakes

  • Thinking higher intensity increases K_max
  • Confusing thermionic emission (heat) with photoelectric (photons)
  • Using de Broglie λ for stationary particles
  • Forgetting φ₀ = hν₀ when finding threshold
  • Wrong slope for V₀–ν graph (h instead of h/e)
  • Applying 12.3/√V to protons without adjusting mass/charge

Memory Aids & Mnemonics

Einstein: "Photon pays φ₀ rent, keeps rest as K_max"
Intensity vs frequency: "Bright light = more electrons, not faster ones"
de Broglie electron: "12.3 over root V gives Å — remember 100 V → 1.23 Å"
Duality: "Light: wave in interference, particle in photoelectric"

Which Formula When?

  • Max electron energy? → K_max = hν − φ₀ or eV₀
  • Threshold frequency? → φ₀ = hν₀
  • Verify Planck's constant? → V₀ = (h/e)(ν − ν₀)
  • Photon energy/momentum? → E = hν, p = hν/c
  • Matter wave of particle? → λ = h/p
  • Electron from voltage V? → λ = 12.3/√V Å
  • Photocurrent vs brightness? → I_sat ∝ intensity

QUICK REFERENCE — Ch 25 Dual Nature

eV₀ = K_max = ½mv²_maxE = hν = hc/λhν = φ₀ + K_maxφ₀ = hν₀K_max = h(ν − ν₀)V₀ = (h/e)(ν − ν₀)p = h/λ = hν/cλ = h/p = h/(mv)λ = h/√(2qmV) = 12.3/√V Žmv² = qVI_sat ∝ intensity (fixed ν)

Key: hν=φ₀+K_max · eV₀=K_max · λ=h/p · λ_e=12.3/√V Å

Work functions (eV): Na 2.5 · K 2.3 · Zn 3.4 · Fe 4.8 · Ni 5.9

Tip: Always check ν > ν₀ before applying photoelectric equations.

PYQ — Previous Year Questions

Extracted from NIOS Physics (312) board exam papers in your PDF. Chapter L25 — Dual Nature of Radiation and Matter only. Use Model Answer for marking points; Explanation for concept clarity.

Chapter 25 — Dual Nature of Radiation and Matter (L25)

6 questions · Section B · Sources: 312/MAY/204A–C, 68/ESS/1-312-A

Section B — Short Answer (2 marks)

PYQ1. Calculate the momentum of a photon of frequency ν.

2 marks · Section B Q36 · 312/MAY/204A

Model Answer

Photon energy E = hν

Momentum p = E/c = hν/c

Also p = h/λ where λ = c/ν

Explanation

Photons have zero rest mass but carry momentum p = hν/c — radiation pressure and Compton effect (L25 §25.1).

PYQ2. Work function for iron is 4.8 eV. Will photoemission take place if radiations of frequency 12×10¹⁴ Hz are incident on an iron cathode?

2 marks · Section B Q36 · 312/MAY/204B

Model Answer

Photon energy: E = hν = 6.626×10⁻³⁴ × 12×10¹⁴ = 7.95×10⁻¹⁹ J

In eV: E = 7.95×10⁻¹⁹ / 1.6×10⁻¹⁹ ≈ 4.97 eV

Since E > φ₀ (4.8 eV), photoemission will occur. Kmax ≈ 0.17 eV

Explanation

Einstein condition: emission only if hν ≥ φ₀. Intensity affects photocurrent, not threshold (L25 §25.1).

PYQ3. Threshold frequency for a metal is 1.160×10¹⁵ Hz. Calculate the work function of the metal in electron volt.

2 marks · Section B Q36 · 312/MAY/204C

Model Answer

φ₀ = hν₀ = 6.626×10⁻³⁴ × 1.160×10¹⁵ = 7.686×10⁻¹⁹ J

φ₀ = 7.686×10⁻¹⁹ / 1.6×10⁻¹⁹ ≈ 4.8 eV

Explanation

Threshold frequency ν₀ is minimum ν for photoelectric emission; work function φ₀ = hν₀ (L25 §25.1).

PYQ4. Draw a diagram to show experimental arrangement for observing the photoelectric effect.

2 marks · Section B Q30 · 68/ESS/1-312-A

Model Answer

Labelled diagram: evacuated glass tube; photosensitive cathode (emitter); anode/collector; monochromatic light through quartz window; variable potential difference; microammeter for photocurrent.

Light ejects photoelectrons from cathode; current measured for different frequency/intensity and retarding voltage.

Explanation

Standard Hertz–Lenard / Millikan-type setup to study Einstein's photoelectric equation (L25 §25.1).

PYQ5. Draw a plot showing the variation of photoelectric current with anode potential for two different frequencies ν₁ > ν₂ of incident radiation having the same intensity. In which case will the stopping potential be higher?

2 marks · Section B Q30 (OR) · 68/ESS/1-312-A (Marking Scheme)

Model Answer

Two I–V curves saturating at same current (same intensity) but different stopping potentials.

Stopping potential higher for ν₁ (ν₁ > ν₂) because Kmax = hν − φ₀ increases with frequency.

Marking scheme: greater frequency → more negative stopping potential magnitude.

Explanation

Same intensity ⇒ same number of photons per second ⇒ same saturation current (for ν above threshold). Stopping potential V₀ = Kmax/e depends only on ν, not intensity (L25 §25.1).

PYQ6. Write any two applications of photocells.

2 marks · Section B Q31 · 68/ESS/1-312-A (Marking Scheme)

Model Answer

Any two, e.g.:

  • Automatic switching of street lights / exposure meters in cameras
  • Burglar alarms and door-openers (light beam interrupted)
  • Sound reproduction in motion pictures; solar cells (photovoltaic variant)

Explanation

Photocells convert light to electrical signal via photoelectric effect — used wherever light intensity must be detected (L25 §25.1).

Problem Solving — L25 Dual Nature of Radiation and Matter

Six problems spanning this chapter’s NIOS syllabus. Every question is built from the notes and formula sheet: solve with equations first, then read the formal textbook-style write-up, the easy explanation, and the topic in depth (formulas, meaning, exam tips). Explanations open by default.

Question 1 of 6Photoelectric

Light of frequency f hits a metal with work function φ. Write Einstein’s equation and meaning of threshold frequency.

hf = φ + K_max
K_max = eV₀

Solution — step by step with formulas

  1. hf = φ + K_max.
  2. f₀ = φ/h; no emission if f < f₀.

Final answer: hf = φ + K_max; f₀ = φ/h

Formulas used in this problem

hf = φ + K_max
K_max = eV₀

Textbook formal language

Photon energy quanta explain instantaneous emission and f-dependent K_max.

Working formula set for this problem: hf = φ + K_max; K_max = eV₀. In the NIOS presentation, physical quantities must be expressed in SI units and the relevant law or definition stated before substitution. Vector quantities require an explicit choice of positive direction; scalar work and energy require attention to sign conventions of the textbook.

Easy language (same idea, plain words)

Each photon spends some energy freeing the electron; leftover is KE. Too red ⇒ no electrons.

Read the question once for the story, once for the numbers. Write the formula, plug in values with units, then simplify. If a result looks huge or tiny, re-check powers of ten and whether you used sin/cos of the correct angle.

Topic in depth — Photoelectric effect

Intensity raises number of photons, hence photocurrent, not K_max (above threshold).

Link to chapter notes (L25 — Photoelectric effect): this idea sits with the definitions and worked examples in the detailed notes and formula sheet. Memorise: hf = φ + K_max; K_max = eV₀. In multi-step questions, keep a free-body diagram or energy flow sketch before algebra; most errors are missing forces or wrong signs, not hard maths.

Exam tip

Quote the law in one line, then write hf = φ + K_max; K_max = eV₀ before numbers. Box the final answer with unit. For numericals, keep at least three significant figures until the last step unless the data are coarse.

Common mistakes

  • Mixing up scalar and vector quantities (e.g. treating momentum as unsigned).
  • Using the wrong sign convention for work/heat/force direction.
  • Forgetting to convert units (g↔kg, cm↔m, minutes↔seconds).
  • Applying a formula outside its assumptions (e.g. F = ma when mass is not constant).
Question 2 of 6Stopping potential

If stopping potential is 2.0 V, find K_max of photoelectrons in eV.

eV₀ = K_max

Solution — step by step with formulas

  1. K_max = 2.0 eV.

Final answer: K_max = 2.0 eV

Formulas used in this problem

eV₀ = K_max

Textbook formal language

Stopping potential measures maximum KE via eV₀ = K_max.

Working formula set for this problem: eV₀ = K_max. In the NIOS presentation, physical quantities must be expressed in SI units and the relevant law or definition stated before substitution. Vector quantities require an explicit choice of positive direction; scalar work and energy require attention to sign conventions of the textbook.

Easy language (same idea, plain words)

Need 2 V reverse to stop the fastest electrons—so they had 2 eV KE.

Read the question once for the story, once for the numbers. Write the formula, plug in values with units, then simplify. If a result looks huge or tiny, re-check powers of ten and whether you used sin/cos of the correct angle.

Topic in depth — Stopping potential

V₀ depends on frequency, not intensity (above threshold).

Link to chapter notes (L25 — Stopping potential): this idea sits with the definitions and worked examples in the detailed notes and formula sheet. Memorise: eV₀ = K_max. In multi-step questions, keep a free-body diagram or energy flow sketch before algebra; most errors are missing forces or wrong signs, not hard maths.

Exam tip

Quote the law in one line, then write eV₀ = K_max before numbers. Box the final answer with unit. For numericals, keep at least three significant figures until the last step unless the data are coarse.

Common mistakes

  • Mixing up scalar and vector quantities (e.g. treating momentum as unsigned).
  • Using the wrong sign convention for work/heat/force direction.
  • Forgetting to convert units (g↔kg, cm↔m, minutes↔seconds).
  • Applying a formula outside its assumptions (e.g. F = ma when mass is not constant).
Question 3 of 6Photon

Find energy and momentum of a photon of wavelength 500 nm (h=6.63×10⁻³⁴, c=3×10⁸).

E = hf
p = h/λ

Solution — step by step with formulas

  1. E = hc/λ ≈ 3.98×10⁻¹⁹ J.
  2. p = h/λ ≈ 1.33×10⁻²⁷ kg·m·s⁻¹.

Final answer: E ≈ 4.0×10⁻¹⁹ J; p = h/λ

Formulas used in this problem

E = hf
p = h/λ

Textbook formal language

Photons are quantum of EM field with E = hf and p = E/c = h/λ.

Working formula set for this problem: E = hf; p = h/λ. In the NIOS presentation, physical quantities must be expressed in SI units and the relevant law or definition stated before substitution. Vector quantities require an explicit choice of positive direction; scalar work and energy require attention to sign conventions of the textbook.

Easy language (same idea, plain words)

Bluer light means punchier photons with more momentum each.

Read the question once for the story, once for the numbers. Write the formula, plug in values with units, then simplify. If a result looks huge or tiny, re-check powers of ten and whether you used sin/cos of the correct angle.

Topic in depth — Photon properties

Photon rest mass is zero; always speed c in vacuum.

Link to chapter notes (L25 — Photon properties): this idea sits with the definitions and worked examples in the detailed notes and formula sheet. Memorise: E = hf; p = h/λ. In multi-step questions, keep a free-body diagram or energy flow sketch before algebra; most errors are missing forces or wrong signs, not hard maths.

Exam tip

Quote the law in one line, then write E = hf; p = h/λ before numbers. Box the final answer with unit. For numericals, keep at least three significant figures until the last step unless the data are coarse.

Common mistakes

  • Mixing up scalar and vector quantities (e.g. treating momentum as unsigned).
  • Using the wrong sign convention for work/heat/force direction.
  • Forgetting to convert units (g↔kg, cm↔m, minutes↔seconds).
  • Applying a formula outside its assumptions (e.g. F = ma when mass is not constant).
Question 4 of 6de Broglie

Calculate de Broglie wavelength of an electron with speed 10⁶ m·s⁻¹ (m=9.1×10⁻³¹).

λ = h/p = h/(mv)

Solution — step by step with formulas

  1. p = mv ≈ 9.1×10⁻²⁵.
  2. λ = h/p ≈ 7.3×10⁻¹⁰ m.

Final answer: λ ≈ 0.73 nm

Formulas used in this problem

λ = h/p = h/(mv)

Textbook formal language

Material particles exhibit wave nature with λ = h/p.

Working formula set for this problem: λ = h/p = h/(mv). In the NIOS presentation, physical quantities must be expressed in SI units and the relevant law or definition stated before substitution. Vector quantities require an explicit choice of positive direction; scalar work and energy require attention to sign conventions of the textbook.

Easy language (same idea, plain words)

Faster or heavier ⇒ shorter wavelength; electrons show measurable λ in crystals.

Read the question once for the story, once for the numbers. Write the formula, plug in values with units, then simplify. If a result looks huge or tiny, re-check powers of ten and whether you used sin/cos of the correct angle.

Topic in depth — Matter waves

Davisson–Germer experiment confirmed electron diffraction.

Link to chapter notes (L25 — Matter waves): this idea sits with the definitions and worked examples in the detailed notes and formula sheet. Memorise: λ = h/p = h/(mv). In multi-step questions, keep a free-body diagram or energy flow sketch before algebra; most errors are missing forces or wrong signs, not hard maths.

Exam tip

Quote the law in one line, then write λ = h/p = h/(mv) before numbers. Box the final answer with unit. For numericals, keep at least three significant figures until the last step unless the data are coarse.

Common mistakes

  • Mixing up scalar and vector quantities (e.g. treating momentum as unsigned).
  • Using the wrong sign convention for work/heat/force direction.
  • Forgetting to convert units (g↔kg, cm↔m, minutes↔seconds).
  • Applying a formula outside its assumptions (e.g. F = ma when mass is not constant).
Question 5 of 6Wave-particle

State wave–particle duality for light and for electrons in one sentence each.

Solution — step by step with formulas

  1. Light: interference (wave) and photoelectric (particle).
  2. Electrons: tracks/KE (particle) and diffraction (wave).

Final answer: Both show wave and particle aspects in different experiments

Textbook formal language

Quantum objects need both descriptions; classical either/or fails.

Working formula set for this problem: (see solution steps). In the NIOS presentation, physical quantities must be expressed in SI units and the relevant law or definition stated before substitution. Vector quantities require an explicit choice of positive direction; scalar work and energy require attention to sign conventions of the textbook.

Easy language (same idea, plain words)

Light and matter can act like waves or bullets depending on the experiment.

Read the question once for the story, once for the numbers. Write the formula, plug in values with units, then simplify. If a result looks huge or tiny, re-check powers of ten and whether you used sin/cos of the correct angle.

Topic in depth — Duality

Complementarity: full wave and particle pictures are mutually exclusive in one setup.

Link to chapter notes (L25 — Duality): this idea sits with the definitions and worked examples in the detailed notes and formula sheet. Memorise: (see solution steps). In multi-step questions, keep a free-body diagram or energy flow sketch before algebra; most errors are missing forces or wrong signs, not hard maths.

Exam tip

Quote the law in one line, then write (see solution steps) before numbers. Box the final answer with unit. For numericals, keep at least three significant figures until the last step unless the data are coarse.

Common mistakes

  • Mixing up scalar and vector quantities (e.g. treating momentum as unsigned).
  • Using the wrong sign convention for work/heat/force direction.
  • Forgetting to convert units (g↔kg, cm↔m, minutes↔seconds).
  • Applying a formula outside its assumptions (e.g. F = ma when mass is not constant).
Question 6 of 6Photon pressure

Why can intense light exert pressure on a surface?

p = E/c (photon)

Solution — step by step with formulas

  1. Photons carry momentum h/λ; reflection/absorption transfers momentum ⇒ force.

Final answer: Momentum transfer from photons

Formulas used in this problem

p = E/c (photon)

Textbook formal language

Radiation pressure is force per area from EM momentum flux.

Working formula set for this problem: p = E/c (photon). In the NIOS presentation, physical quantities must be expressed in SI units and the relevant law or definition stated before substitution. Vector quantities require an explicit choice of positive direction; scalar work and energy require attention to sign conventions of the textbook.

Easy language (same idea, plain words)

Light punches gently with many photon kicks—strong beams can move dust in space.

Read the question once for the story, once for the numbers. Write the formula, plug in values with units, then simplify. If a result looks huge or tiny, re-check powers of ten and whether you used sin/cos of the correct angle.

Topic in depth — Radiation pressure idea

Perfect reflection transfers 2p per photon vs absorption p.

Link to chapter notes (L25 — Radiation pressure idea): this idea sits with the definitions and worked examples in the detailed notes and formula sheet. Memorise: p = E/c (photon). In multi-step questions, keep a free-body diagram or energy flow sketch before algebra; most errors are missing forces or wrong signs, not hard maths.

Exam tip

Quote the law in one line, then write p = E/c (photon) before numbers. Box the final answer with unit. For numericals, keep at least three significant figures until the last step unless the data are coarse.

Common mistakes

  • Mixing up scalar and vector quantities (e.g. treating momentum as unsigned).
  • Using the wrong sign convention for work/heat/force direction.
  • Forgetting to convert units (g↔kg, cm↔m, minutes↔seconds).
  • Applying a formula outside its assumptions (e.g. F = ma when mass is not constant).