Photoelectric Effect — NEET Physics PYQ MCQs with Solutions
Free NEET Physics PYQ Photoelectric Effect MCQs with step-by-step solutions (39 questions). Part of Dual Nature of Radiation and Matter. Practise online on Prepizo — no login needed.
▶ Practise Photoelectric Effect online (free)
Questions with solutions
Q1 — Photoelectric Effect · medium · theory
Light of frequency 1.5 times the threshold frequency is incident on a photosensitive material. What will be the photoelectric current if the frequency is halved and intensity is doubled?
A. Four times
B. One-fourth
C. Zero ✓ Correct
D. Doubled
Solution: Initially $\nu = 1.5\nu_0$. When halved, $\nu' = 0.75\nu_0 < \nu_0$ — below the threshold frequency.
No photoelectric emission takes place regardless of intensity, so the photoelectric current is zero.
Q2 — Photoelectric Effect · medium · numerical
The work function of a photosensitive material is 4.0 eV. The longest wavelength of light that can cause photon emission from the substance is (approximately)
A. 3100 nm
B. 966 nm
C. 31 nm
D. 310 nm ✓ Correct
Solution: $\phi = \frac{hc}{\lambda}$
$\lambda = \frac{hc}{\phi} = \frac{6.63 \times 10^{-34} \times 3 \times 10^8}{4 \times 1.6 \times 10^{-19}} = 3.1 \times 10^{-7}$ m $\approx 310$ nm
Q3 — Photoelectric Effect · medium · numerical
When the light of frequency $2\nu_0$ (where $\nu_0$ is threshold frequency), is incident on a metal plate, the maximum velocity of electrons emitted is $v_1$. When the frequency of the incident radiation is increased to $5\nu_0$, the maximum velocity of electrons emitted from the same plate is $v_2$. The ratio of $v_1$ to $v_2$ is
A. 4 : 1
B. 1 : 4
C. 1 : 2 ✓ Correct
D. 2 : 1
Solution: By Einstein's equation, $\frac{1}{2}mv^2 = h\nu - h\nu_0$
For $2\nu_0$: $\frac{1}{2}mv_1^2 = h\nu_0$; for $5\nu_0$: $\frac{1}{2}mv_2^2 = 4h\nu_0$
$\frac{v_1^2}{v_2^2} = \frac{1}{4} \Rightarrow v_1 : v_2 = 1 : 2$
Q4 — Photoelectric Effect · hard · numerical
The photoelectric threshold wavelength of silver is $3250 \times 10^{-10}$ m. The velocity of the electron ejected from a silver surface by ultraviolet light of wavelength $2536 \times 10^{-10}$ m is (Given, $h = 4.14 \times 10^{-15}$ eV-s and $c = 3 \times 10^8$ ms⁻¹)
A. $\approx 6 \times 10^5$ ms⁻¹ ✓ Correct
B. $\approx 0.6 \times 10^6$ ms⁻¹
C. $\approx 61 \times 10^3$ ms⁻¹
D. $\approx 0.3 \times 10^6$ ms⁻¹
Solution: $\frac{1}{2}m_e v^2 = hc\left(\frac{1}{\lambda} - \frac{1}{\lambda_0}\right)$
$v = \sqrt{\frac{2hc}{m_e}\left(\frac{1}{\lambda} - \frac{1}{\lambda_0}\right)} \approx 6 \times 10^5$ ms⁻¹
(Note: options (a) and (b) are numerically the same value — $0.6 \times 10^6 = 6 \times 10^5$; the official key accepted both.)
Q5 — Photoelectric Effect · hard · numerical
When a metallic surface is illuminated with radiation of wavelength $\lambda$, the stopping potential is V. If the same surface is illuminated with radiation of wavelength $2\lambda$, the stopping potential is $\frac{V}{4}$. The threshold wavelength for the metallic surface is
A. $5\lambda$
B. $\frac{5}{2}\lambda$
C. $3\lambda$ ✓ Correct
D. $4\lambda$
Solution: Case 1: $eV = \frac{hc}{\lambda} - \frac{hc}{\lambda_0}$
Case 2: $\frac{eV}{4} = \frac{hc}{2\lambda} - \frac{hc}{\lambda_0}$, i.e. $eV = \frac{4hc}{2\lambda} - \frac{4hc}{\lambda_0}$
Equating: $\frac{1}{\lambda} - \frac{1}{\lambda_0} = \frac{2}{\lambda} - \frac{4}{\lambda_0} \Rightarrow \lambda_0 = 3\lambda$
Q6 — Photoelectric Effect · hard · numerical
Photons with energy 5 eV are incident on a cathode C in a photoelectric cell. The maximum energy of emitted photoelectrons is 2 eV. When photons of energy 6 eV are incident on C, no photoelectrons will reach the anode A, if the stopping potential of A relative to C is
A. +3 V
B. +4 V
C. −1 V
D. −3 V ✓ Correct
Solution: Work function: $\phi = 5 - 2 = 3$ eV
With 6 eV photons, $K_{max} = 6 - 3 = 3$ eV.
To stop these electrons the anode must be 3 V negative relative to the cathode: $V_A - V_C = -3$ V
Q7 — Photoelectric Effect · hard · numerical
A certain metallic surface is illuminated with monochromatic light of wavelength $\lambda$. The stopping potential for photoelectric current for this light is $3V_0$. If the same surface is illuminated with light of wavelength $2\lambda$, the stopping potential is $V_0$. The threshold wavelength for this surface for photoelectric effect is
A. $6\lambda$
B. $4\lambda$ ✓ Correct
C. $\frac{\lambda}{4}$
D. $\frac{\lambda}{6}$
Solution: $\frac{hc}{\lambda} = W + 3eV_0$ and $\frac{hc}{2\lambda} = W + eV_0$ (so $\frac{hc}{\lambda} = 2W + 2eV_0$)
Subtracting: $W = eV_0$, hence $\frac{hc}{\lambda} = 4eV_0$
$\lambda_{th} = \frac{hc}{W} = \frac{4eV_0\lambda}{eV_0} = 4\lambda$
Q8 — Photoelectric Effect · medium · numerical
A photoelectric surface is illuminated successively by monochromatic light of wavelength $\lambda$ and $\frac{\lambda}{2}$. If the maximum kinetic energy of the emitted photoelectrons in the second case is 3 times that in the first case, the work function of the surface of the material is (h = Planck's constant, c = speed of light)
A. $\frac{hc}{2\lambda}$ ✓ Correct
B. $\frac{hc}{\lambda}$
C. $\frac{2hc}{\lambda}$
D. $\frac{hc}{3\lambda}$
Solution: $K_{max} = \frac{hc}{\lambda} - \phi$ and $3K_{max} = \frac{2hc}{\lambda} - \phi$
Multiplying the first by 3 and equating: $\frac{3hc}{\lambda} - 3\phi = \frac{2hc}{\lambda} - \phi$
$\phi = \frac{hc}{2\lambda}$
Q9 — Photoelectric Effect · hard · numerical
Light of wavelength 500 nm is incident on a metal with work function 2.28 eV. The de-Broglie wavelength of the emitted electron is
A. $< 2.8 \times 10^{-10}$ m
B. $< 2.8 \times 10^{-9}$ m
C. $\geq 2.8 \times 10^{-9}$ m ✓ Correct
D. $\leq 2.8 \times 10^{-12}$ m
Solution: Photon energy $E = \frac{hc}{\lambda} = 2.48$ eV, so $K_{max} = 2.48 - 2.28 = 0.2$ eV
Minimum de-Broglie wavelength: $\lambda_e = \frac{12.27}{\sqrt{0.2}}$ Å $\approx 2.8 \times 10^{-9}$ m
Slower electrons have longer wavelengths, so $\lambda \geq 2.8 \times 10^{-9}$ m.
Q10 — Photoelectric Effect · medium · numerical
When the energy of the incident radiation is increased by 20%, the kinetic energy of the photoelectrons emitted from a metal surface increased from 0.5 eV to 0.8 eV. The work function of the metal is
A. 0.65 eV
B. 1.0 eV ✓ Correct
C. 1.3 eV
D. 1.5 eV
Solution: $0.5 = E - \phi_0$ and $0.8 = 1.2E - \phi_0$
Subtracting: $0.3 = 0.2E \Rightarrow E = 1.5$ eV
$\phi_0 = 1.5 - 0.5 = 1.0$ eV
Q11 — Photoelectric Effect · medium · numerical
For photoelectric emission from certain metal, the cut-off frequency is $\nu$. If radiation of frequency $2\nu$ impinges on the metal plate, the maximum possible velocity of the emitted electron will be (m is the electron mass)
A. $\sqrt{\frac{h\nu}{2m}}$
B. $\sqrt{\frac{h\nu}{m}}$
C. $\sqrt{\frac{2h\nu}{m}}$ ✓ Correct
D. $2\sqrt{\frac{h\nu}{m}}$
Solution: $\frac{1}{2}mv_{max}^2 = h(2\nu) - h\nu = h\nu$
$v_{max} = \sqrt{\frac{2h\nu}{m}}$
Q12 — Photoelectric Effect · medium · numerical
Light of two different frequencies whose photons have energies 1 eV and 2.5 eV respectively illuminate a metallic surface whose work function is 0.5 eV successively. Ratio of maximum speeds of emitted electrons will be
A. 1 : 2 ✓ Correct
B. 1 : 1
C. 1 : 5
D. 1 : 4
Solution: $KE_1 = 1 - 0.5 = 0.5$ eV; $KE_2 = 2.5 - 0.5 = 2$ eV
$\frac{v_1^2}{v_2^2} = \frac{KE_1}{KE_2} = \frac{1}{4} \Rightarrow \frac{v_1}{v_2} = \frac{1}{2}$
Q13 — Photoelectric Effect · easy · theory
Photoelectric emission occurs only when the incident light has more than a certain minimum
A. wavelength
B. intensity
C. frequency ✓ Correct
D. power
Solution: Photoelectric emission requires $\nu \geq \nu_0$ (threshold frequency). The incident light must have more than a certain minimum frequency, regardless of intensity.
Q14 — Photoelectric Effect · easy · numerical
In photoelectric emission process from a metal of work function 1.8 eV, the kinetic energy of most energetic electrons is 0.5 eV. The corresponding stopping potential is
A. 1.3 V
B. 0.5 V ✓ Correct
C. 2.3 V
D. 1.8 V
Solution: The stopping potential corresponds to the maximum kinetic energy:
$eV_0 = K_{max} = 0.5$ eV $\Rightarrow V_0 = 0.5$ V
Q15 — Photoelectric Effect · easy · theory
The number of photoelectrons emitted for light of a frequency $\nu$ (higher than the threshold frequency $\nu_0$) is proportional to
A. $\nu - \nu_0$
B. threshold frequency ($\nu_0$)
C. intensity of light ✓ Correct
D. frequency of light ($\nu$)
Solution: The number of photoelectrons emitted depends only on the intensity of the incident light (one photon ejects one electron). Frequency decides their maximum kinetic energy, not their number.
Q16 — Photoelectric Effect · medium · theory
In the phenomenon of electric discharge through gases at low pressure, the coloured glow in the tube appears as a result of
A. excitation of electrons in the atoms
B. collision between the atoms of the gas
C. collisions between the charged particles emitted from the cathode and the atoms of the gas ✓ Correct
D. collision between different electrons of the atoms of the gas
Solution: In electric discharge through gases at low pressure, charged particles emitted from the cathode collide with the atoms of the gas, producing the coloured glow in the tube.
Q17 — Photoelectric Effect · medium · numerical
The work function of a surface of a photosensitive material is 6.2 eV. The wavelength of the incident radiation for which the stopping potential is 5 V lies in the
A. ultraviolet region
B. visible region
C. infrared region
D. X-ray region ✓ Correct
Solution: $h\nu = \phi + eV_0 = 6.2 + 5 = 11.2$ eV
A photon of 11.2 eV corresponds to $\lambda \approx 1100$ Å, which lies in the X-ray region.
Q18 — Photoelectric Effect · medium · numerical
A 5 W source emits monochromatic light of wavelength 5000 Å. When placed 0.5 m away, it liberates photoelectrons from a photosensitive metallic surface. When the source is moved to a distance of 1.0 m, the number of photoelectrons liberated will be reduced by a factor of
A. 4 ✓ Correct
B. 8
C. 16
D. 2
Solution: Intensity $\propto \frac{1}{d^2}$. Doubling the distance reduces intensity to $\frac{1}{4}$.
The number of photoelectrons is proportional to intensity, so it is reduced by a factor of 4.
Q19 — Photoelectric Effect · easy · theory
A photocell employs photoelectric effect to convert
A. change in the frequency of light into a change in electric voltage
B. change in the intensity of illumination into a change in photoelectric current ✓ Correct
C. change in the intensity of illumination into a change in the work function of the photocathode
D. change in the frequency of light into a change in the electric current
Solution: For a fixed frequency, the photoelectric current increases linearly with the intensity of the incident light. A photocell therefore converts a change in the intensity of illumination into a change in photoelectric current.
Q20 — Photoelectric Effect · medium · numerical
A photosensitive metallic surface has work function $h\nu_0$. If photons of energy $2h\nu_0$ fall on this surface, the electrons come out with a maximum velocity of $4 \times 10^6$ m/s. When the photon energy is increased to $5h\nu_0$, then maximum velocity of photoelectrons will be
A. $2 \times 10^6$ m/s
B. $2 \times 10^7$ m/s
C. $8 \times 10^5$ m/s
D. $8 \times 10^6$ m/s ✓ Correct
Solution: $\frac{1}{2}m(4 \times 10^6)^2 = 2h\nu_0 - h\nu_0 = h\nu_0$
$\frac{1}{2}mv^2 = 5h\nu_0 - h\nu_0 = 4h\nu_0$
Dividing: $v^2 = 4 \times (4 \times 10^6)^2 \Rightarrow v = 8 \times 10^6$ m/s
Q21 — Photoelectric Effect · medium · numerical
The work functions for metals A, B and C are respectively 1.92 eV, 2.0 eV and 5 eV. According to Einstein's equation, the metals which will emit photoelectrons for a radiation of wavelength 4100 Å is/are
A. None of these
B. A only
C. A and B only ✓ Correct
D. All the three metals
Solution: Photon energy for 4100 Å: $E = \frac{hc}{\lambda} = \frac{12375}{4100} \approx 3$ eV
Emission occurs when $E > \phi$. Since $W_A = 1.92$ eV and $W_B = 2.0$ eV are less than 3 eV (but $W_C = 5$ eV is greater), only A and B emit photoelectrons.
Q22 — Photoelectric Effect · medium · theory
A photoelectric cell is illuminated by a point source of light 1 m away. When the source is shifted to 2 m, then
A. each emitted electron carries half the initial energy
B. number of electrons emitted is a quarter of the initial number ✓ Correct
C. each emitted electron carries one quarter of the initial energy
D. number of electrons emitted is half the initial number
Solution: Intensity $\propto \frac{1}{d^2}$: doubling the distance makes the intensity one-fourth.
The number of photoelectrons is proportional to intensity, so it becomes a quarter of the initial number. The energy of each electron is unchanged (it depends on frequency).
Q23 — Photoelectric Effect · easy · theory
When ultraviolet rays are incident on a metal plate, the photoelectric effect does not occur. It occurs by incidence of
A. infrared rays
B. X-rays ✓ Correct
C. radiowaves
D. light waves
Solution: If ultraviolet light cannot cause emission, the incident wavelength must be even shorter (higher energy). Among the options, only X-rays have a wavelength shorter than ultraviolet, so only X-rays can cause photoelectric emission.
Q24 — Photoelectric Effect · easy · theory
Which of the following is not the property of cathode rays?
A. It produces heating effect
B. It does not deflect in electric field ✓ Correct
C. It casts shadow
D. It produces fluorescence
Solution: Cathode rays are streams of electrons (negatively charged), so they DO deflect in an electric field — towards the positive plate. They produce heating, travel in straight lines (cast shadows), and cause fluorescence.
Q25 — Photoelectric Effect · easy · numerical
A light source is at a distance d from a photoelectric cell, then the number of photoelectrons emitted from the cell is n. If the distance of light source and cell is reduced to half, then the number of photoelectrons emitted will become
A. $\frac{n}{2}$
B. $2n$
C. $4n$ ✓ Correct
D. $n$
Solution: Intensity $\propto \frac{1}{d^2}$. Halving the distance makes the intensity 4 times, so the number of photoelectrons becomes $4n$.
Q26 — Photoelectric Effect · easy · theory
Einstein's work on photoelectric effect gives support to
A. $E = mc^2$
B. $E = h\nu$ ✓ Correct
C. $h\nu = \frac{1}{2}mv^2$
D. $E = \frac{h}{\lambda}$
Solution: Einstein explained the photoelectric effect by treating light as concentrated packets (photons), each of energy $h\nu$ — supporting the relation $E = h\nu$.
Q27 — Photoelectric Effect · easy · theory
When intensity of incident light increases
A. photocurrent increases ✓ Correct
B. photocurrent decreases
C. kinetic energy of emitted photoelectrons increases
D. kinetic energy of emitted photoelectrons decreases
Solution: More intensity means more incident photons, hence more ejected electrons and a larger photocurrent. The kinetic energy of the electrons depends on frequency, not intensity.
Q28 — Photoelectric Effect · medium · numerical
The photoelectric work function for a metal surface is 4.125 eV. The cut-off wavelength for this surface is
A. 4125 Å
B. 3000 Å ✓ Correct
C. 6000 Å
D. 2062.5 Å
Solution: $\lambda_0 = \frac{hc}{W_0} = \frac{6.6 \times 10^{-34} \times 3 \times 10^8}{4.125 \times 1.6 \times 10^{-19}} = 3 \times 10^{-7}$ m $= 3000$ Å
Q29 — Photoelectric Effect · hard · numerical
In a photoemissive cell, with exciting wavelength $\lambda$, the fastest electron has speed v. If the exciting wavelength is changed to $\frac{3\lambda}{4}$, the speed of the fastest emitted electron will be
A. $v\left(\frac{3}{4}\right)^{1/2}$
B. $v\left(\frac{4}{3}\right)^{1/2}$
C. less than $v\left(\frac{4}{3}\right)^{1/2}$
D. greater than $v\left(\frac{4}{3}\right)^{1/2}$ ✓ Correct
Solution: $\frac{1}{2}mv^2 = \frac{hc}{\lambda} - W_0$ and $\frac{1}{2}mv'^2 = \frac{4hc}{3\lambda} - W_0$
Since the photon energy increases by a factor $\frac{4}{3}$ but the work function stays the same, the kinetic energy increases by more than $\frac{4}{3}$:
$v' > v\sqrt{\frac{4}{3}}$
Q30 — Photoelectric Effect · easy · numerical
Light of wavelength 5000 Å falls on a sensitive plate with photoelectric work function of 1.9 eV. The kinetic energy of the photoelectron emitted will be
A. 0.58 eV ✓ Correct
B. 2.48 eV
C. 1.24 eV
D. 1.16 eV
Solution: $E = \frac{12375}{5000} = 2.48$ eV
$KE = E - W_0 = 2.48 - 1.9 = 0.58$ eV