Wave Nature of Light — NEET Physics PYQ MCQs with Solutions
Free NEET Physics PYQ Wave Nature of Light MCQs with step-by-step solutions (16 questions). Part of Dual Nature of Radiation and Matter. Practise online on Prepizo — no login needed.
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Questions with solutions
Q1 — Wave Nature of Light · medium · numerical
The de-Broglie wavelength of an electron moving with kinetic energy of 144 eV is nearly
A. $102 \times 10^{-3}$ nm ✓ Correct
B. $102 \times 10^{-4}$ nm
C. $102 \times 10^{-5}$ nm
D. $102 \times 10^{-2}$ nm
Solution: $\lambda = \frac{12.27}{\sqrt{V}}$ Å $= \frac{12.27}{\sqrt{144}} = \frac{12.27}{12} \approx 1.02$ Å
$1.02$ Å $= 0.102$ nm $= 102 \times 10^{-3}$ nm
Q2 — Wave Nature of Light · easy · theory
The wave nature of electrons was experimentally verified by
A. de-Broglie
B. Hertz
C. Einstein
D. Davisson and Germer ✓ Correct
Solution: de-Broglie proposed the hypothesis of matter waves, but it was the Davisson–Germer experiment (electron diffraction from a nickel crystal) that experimentally verified the wave nature of electrons.
Q3 — Wave Nature of Light · medium · numerical
An electron is accelerated from rest through a potential difference of V volt. If the de-Broglie wavelength of the electron is $1.227 \times 10^{-2}$ nm, the potential difference is
A. $10^2$ V
B. $10^3$ V
C. $10^4$ V ✓ Correct
D. 10 V
Solution: $\lambda = \frac{12.27}{\sqrt{V}}$ Å
$1.227 \times 10^{-2}$ nm $= 0.1227$ Å $\Rightarrow \sqrt{V} = \frac{12.27}{0.1227} = 100$
$V = 10^4$ V
Q4 — Wave Nature of Light · medium · numerical
A proton and an $\alpha$-particle are accelerated from rest to the same energy. The de-Broglie wavelengths $\lambda_p$ and $\lambda_\alpha$ are in the ratio
A. 2 : 1 ✓ Correct
B. 1 : 1
C. $\sqrt{2}$ : 1
D. 4 : 1
Solution: $\lambda = \frac{h}{\sqrt{2m\,KE}}$
With equal kinetic energies and $m_\alpha = 4m_p$:
$\frac{\lambda_p}{\lambda_\alpha} = \sqrt{\frac{m_\alpha}{m_p}} = \sqrt{4} = \frac{2}{1}$
Q5 — Wave Nature of Light · medium · numerical
An electron is accelerated through a potential difference of 10,000 V. Its de-Broglie wavelength is (nearly) ($m_e = 9 \times 10^{-31}$ kg)
A. $12.2 \times 10^{-12}$ m ✓ Correct
B. $12.2 \times 10^{-14}$ m
C. 12.2 nm
D. $12.2 \times 10^{-13}$ m
Solution: $\lambda = \frac{12.27}{\sqrt{V}}$ Å $= \frac{12.27}{\sqrt{10000}} = \frac{12.27}{100}$ Å
$= 12.27 \times 10^{-12}$ m
Q6 — Wave Nature of Light · hard · numerical
An electron of mass m with a velocity $v = v_0\hat{i}$ ($v_0 > 0$) enters an electric field $E = -E_0\hat{i}$ ($E_0$ = constant > 0) at $t = 0$. If $\lambda_0$ is its de-Broglie wavelength initially, then its de-Broglie wavelength at time t is
A. $\lambda_0 t$
B. $\lambda_0\left(1 + \frac{eE_0}{mv_0}t\right)$
C. $\frac{\lambda_0}{\left(1 + \frac{eE_0}{mv_0}t\right)}$ ✓ Correct
D. $\lambda_0$
Solution: Force on the electron (negative charge in field $-E_0\hat{i}$) is $eE_0$ along $\hat{i}$, so it accelerates: $v = v_0 + \frac{eE_0}{m}t$
$\lambda = \frac{h}{mv} = \frac{h}{mv_0\left(1 + \frac{eE_0}{mv_0}t\right)} = \frac{\lambda_0}{1 + \frac{eE_0}{mv_0}t}$
Q7 — Wave Nature of Light · medium · numerical
The de-Broglie wavelength of a neutron in thermal equilibrium with heavy water at a temperature T (Kelvin) and mass m, is
A. $\frac{h}{\sqrt{mkT}}$
B. $\frac{h}{\sqrt{3mkT}}$ ✓ Correct
C. $\frac{2h}{\sqrt{3mkT}}$
D. $\frac{2h}{\sqrt{mkT}}$
Solution: Thermal kinetic energy: $KE = \frac{3}{2}kT$
$\lambda = \frac{h}{\sqrt{2m\,KE}} = \frac{h}{\sqrt{2m \times \frac{3}{2}kT}} = \frac{h}{\sqrt{3mkT}}$
Q8 — Wave Nature of Light · hard · numerical
An electron of mass m and a photon have same energy E. The ratio of de-Broglie wavelengths associated with them is (c being velocity of light)
A. $\left(\frac{E}{2m}\right)^{1/2}$
B. $c(2mE)^{1/2}$
C. $\frac{1}{c}\left(\frac{2m}{E}\right)^{1/2}$
D. $\frac{1}{c}\left(\frac{E}{2m}\right)^{1/2}$ ✓ Correct
Solution: Electron: $\lambda_e = \frac{h}{\sqrt{2mE}}$; photon: $\lambda_p = \frac{hc}{E}$
$\frac{\lambda_e}{\lambda_p} = \frac{h}{\sqrt{2mE}} \cdot \frac{E}{hc} = \frac{1}{c}\sqrt{\frac{E}{2m}}$
Q9 — Wave Nature of Light · hard · numerical
Electrons of mass m with de-Broglie wavelength $\lambda$ fall on the target in an X-ray tube. The cut-off wavelength ($\lambda_0$) of the emitted X-ray is
A. $\lambda_0 = \frac{2mc\lambda^2}{h}$ ✓ Correct
B. $\lambda_0 = \frac{2h}{mc}$
C. $\lambda_0 = \frac{2m^2c^2\lambda^3}{h^2}$
D. $\lambda_0 = \lambda$
Solution: Kinetic energy of the electron: $\frac{p^2}{2m} = \frac{h^2}{2m\lambda^2}$
At cut-off, all this energy becomes one X-ray photon: $\frac{hc}{\lambda_0} = \frac{h^2}{2m\lambda^2}$
$\lambda_0 = \frac{2mc\lambda^2}{h}$
Q10 — Wave Nature of Light · medium · numerical
If the kinetic energy of the particle is increased to 16 times its previous value, the percentage change in the de-Broglie wavelength of the particle is
A. 25
B. 75 ✓ Correct
C. 60
D. 50
Solution: $\lambda = \frac{h}{\sqrt{2mK}}$
$\lambda_2 = \frac{h}{\sqrt{2m \times 16K}} = \frac{\lambda_1}{4}$ — i.e. 25% of the original
So the wavelength decreases by 75%.
Q11 — Wave Nature of Light · medium · numerical
The wavelength $\lambda_e$ of an electron and $\lambda_p$ of a photon of same energy E are related by
A. $\lambda_p \propto \lambda_e^2$ ✓ Correct
B. $\lambda_p \propto \lambda_e$
C. $\lambda_p \propto \sqrt{\lambda_e}$
D. $\lambda_p \propto \frac{1}{\sqrt{\lambda_e}}$
Solution: Electron: $\lambda_e = \frac{h}{\sqrt{2mE}} \Rightarrow \lambda_e^2 = \frac{h^2}{2mE}$
Photon: $E = \frac{hc}{\lambda_p}$
Substituting: $\lambda_e^2 = \frac{h\lambda_p}{2mc} \Rightarrow \lambda_p \propto \lambda_e^2$
Q12 — Wave Nature of Light · medium · numerical
A particle of mass 1 mg has the same wavelength as an electron moving with a velocity of $3 \times 10^6$ ms⁻¹. The velocity of the particle is (mass of electron $= 9.1 \times 10^{-31}$ kg)
A. $2.7 \times 10^{-18}$ ms⁻¹ ✓ Correct
B. $9 \times 10^{-2}$ ms⁻¹
C. $3 \times 10^{-31}$ ms⁻¹
D. $2.7 \times 10^{-21}$ ms⁻¹
Solution: Equal wavelengths mean equal momenta: $mv = m_e v_e$
$v = \frac{9.1 \times 10^{-31} \times 3 \times 10^6}{1 \times 10^{-6}} = 2.7 \times 10^{-18}$ ms⁻¹
Q13 — Wave Nature of Light · easy · theory
The following particles are moving with the same velocity, then maximum de-Broglie wavelength will be for
A. proton
B. $\alpha$-particle
C. neutron
D. $\beta$-particle ✓ Correct
Solution: $\lambda = \frac{h}{mv}$; for the same velocity, $\lambda \propto \frac{1}{m}$
The $\beta$-particle (an electron) has the smallest mass, so its de-Broglie wavelength is maximum.
Q14 — Wave Nature of Light · easy · numerical
The energy of a photon of light is 3 eV. Then the wavelength of photon must be
A. 4125 nm
B. 412.5 nm ✓ Correct
C. 41250 nm
D. 4 nm
Solution: $\lambda = \frac{12375}{E(\text{eV})}$ Å $= \frac{12375}{3} = 4125$ Å $= 412.5$ nm
Q15 — Wave Nature of Light · medium · numerical
The wavelength associated with an electron, accelerated through a potential difference of 100 V, is of the order of
A. 1000 Å
B. 100 Å
C. 10.5 Å
D. 1.2 Å ✓ Correct
Solution: $\lambda = \frac{12.27}{\sqrt{V}}$ Å $= \frac{12.27}{\sqrt{100}} \approx 1.2$ Å
Q16 — Wave Nature of Light · easy · theory
The de-Broglie wave corresponding to a particle of mass m and velocity v has a wavelength associated with it
A. $\frac{h}{mv}$ ✓ Correct
B. $hmv$
C. $\frac{mh}{v}$
D. $\frac{m}{hv}$
Solution: The de-Broglie wavelength of a moving particle is
$\lambda = \frac{h}{mv}$
where h is Planck's constant.