Sign in
12thPass logo
New chatPYQ LibraryDoubtsRank report
Sign in to see Recents

Your guest activity stays on this device

Sign in to save progress →
Sign in

Dual Nature of Radiation question

2019 · Shift 2 · Q47
Guest · filters and generic practice availableBrowsing as a guest · PYQ filters and generic practice are available. Sign in only for personalised features and saved progress.
  1. PYQ Library
  2. /JEE Advanced
  3. /Physics
  4. /Dual Nature of Radiation
  5. /2019 · Shift 2 · Q47

Dual Nature of Radiation question

2019 · Shift 2 · Q47

JEE AdvancedPhysicsDual Nature of RadiationNumerical+3 / −1
A perfectly reflecting mirror of mass M mounted on a spring constitutes a spring-mass system of angular frequency Ω\OmegaΩ such that 4πMΩh=1024m−2{{4\pi M\Omega } \over h} = {10^{24}}{m^{ - 2}}h4πMΩ​=1024m−2 with h as Planck's constant. N photons of wavelength λ\lambdaλ = 8 π×\pi \timesπ× 10 −-− 6 m strike the mirror simultaneously at normal incidence such that the mirror gets displaced by 1 μ\muμ m. If the value of N is x ×\times× 1012, then the value of x is ................ [Consider the spring as massless] JEE Advanced 2019 Paper 2 Offline Physics - Dual Nature of Radiation Question 24 English
Numerical answer
View written solutionFree

Correct answer: 1.0

Step-by-step Derivation

  1. Momentum of a single photon: The momentum p of a single photon with wavelength λ is given by the de Broglie relation: p=hλp = \frac{h}{\lambda}p=λh​ where h is Planck's constant.

  2. Momentum transferred to the mirror: The mirror is perfectly reflecting. The photons strike at normal incidence and bounce back along the same path. The initial momentum of a photon is p, and its final momentum is -p. The change in momentum for one photon is Δpphoton=pfinal−pinitial=(−p)−(p)=−2pΔp_{photon} = p_{final} - p_{initial} = (-p) - (p) = -2pΔpphoton​=pfinal​−pinitial​=(−p)−(p)=−2p. By the law of conservation of momentum, the momentum transferred to the mirror by one photon is Δpmirror=−Δpphoton=2pΔp_{mirror} = -Δp_{photon} = 2pΔpmirror​=−Δpphoton​=2p. Δpmirror=2hλΔp_{mirror} = 2 \frac{h}{\lambda}Δpmirror​=2λh​

  3. Total momentum transferred by N photons: N photons strike the mirror simultaneously. The total momentum P transferred to the mirror is the sum of the momentum transferred by each photon: P=N×Δpmirror=N(2hλ)P = N \times Δp_{mirror} = N \left( \frac{2h}{\lambda} \right)P=N×Δpmirror​=N(λ2h​)

  4. Initial velocity of the mirror: This momentum P is transferred to the mirror of mass M as an impulse, causing it to move with an initial velocity v. The mirror is initially at rest in its equilibrium position. P=MvP = MvP=Mv Equating the two expressions for P: Mv=2Nhλ(∗)Mv = \frac{2Nh}{\lambda} \quad (*)Mv=λ2Nh​(∗)

  5. Simple Harmonic Motion (SHM) of the mirror: The mirror is part of a spring-mass system. After receiving the impulse at its equilibrium position, it undergoes Simple Harmonic Motion. The velocity v it acquires at the equilibrium position is the maximum velocity (vmaxv_{max}vmax​) of the SHM. The maximum velocity in an SHM is related to the amplitude A and the angular frequency Ω by: v=vmax=AΩv = v_{max} = A\Omegav=vmax​=AΩ The problem states that the mirror gets displaced by 1 μm. This maximum displacement is the amplitude A of the oscillation. So, A=1μm=10−6mA = 1 \mu m = 10^{-6} mA=1μm=10−6m.

  6. Solving for N: Substitute v = AΩ into equation (*): M(AΩ)=2NhλM(A\Omega) = \frac{2Nh}{\lambda}M(AΩ)=λ2Nh​ Now, we rearrange this equation to solve for the number of photons, N: N=MAΩλ2hN = \frac{MA\Omega\lambda}{2h}N=2hMAΩλ​

  7. Using the given values: We are given the following values:

    • A=1μm=10−6mA = 1 \mu m = 10^{-6} mA=1μm=10−6m
    • λ=8π×10−6m\lambda = 8\pi \times 10^{-6} mλ=8π×10−6m
    • 4πMΩh=1024m−2\frac{4\pi M\Omega}{h} = 10^{24} m^{-2}h4πMΩ​=1024m−2

    To use the given expression, let's rearrange our formula for N: N=MAΩλ2h=(Aλ8π)(4πMΩh)N = \frac{MA\Omega\lambda}{2h} = \left( \frac{A\lambda}{8\pi} \right) \left( \frac{4\pi M\Omega}{h} \right)N=2hMAΩλ​=(8πAλ​)(h4πMΩ​)

  8. Calculation: Substitute the numerical values into the rearranged formula: N=((10−6m)(8π×10−6m)8π)×(1024m−2)N = \left( \frac{(10^{-6} m)(8\pi \times 10^{-6} m)}{8\pi} \right) \times (10^{24} m^{-2})N=(8π(10−6m)(8π×10−6m)​)×(1024m−2) The 8π terms in the numerator and denominator cancel out: N=(10−6×10−6m2)×(1024m−2)N = (10^{-6} \times 10^{-6} m^2) \times (10^{24} m^{-2})N=(10−6×10−6m2)×(1024m−2) N=10−12×1024N = 10^{-12} \times 10^{24}N=10−12×1024 N=1012N = 10^{12}N=1012

  9. Finding the value of x: The problem states that N=x×1012N = x \times 10^{12}N=x×1012. Comparing this with our calculated value N=1×1012N = 1 \times 10^{12}N=1×1012: x×1012=1×1012x \times 10^{12} = 1 \times 10^{12}x×1012=1×1012 Therefore, x = 1.

Final Answer

The value of x is 1.

PreviousNext

More from Dual Nature of Radiation

  • In a photoelectric experiment a parallel beam of monochromatic light with power of 200W is incident on a perfectly absorbing cathode of work function 6.25ev. The frequency of light is just above the threshold frequency so that the…2018 · Numerical
  • A photoelectric material having work-function ϕ0​ is illuminated with light of wavelength λ(λ<ϕ0​he​). The fastest photoelectron has a de-Broglic wavelength λd​. A…2017 · MCQ
  • In a historical experiment to determine Planck's constant, a metal surface was irradiated with light of different wavelengths. The emitted photoelectron energies were measured by applying a stopping potential. The relevant data for the… Includes table2016 · MCQ
  • Light of wavelength λ ph falls on a cathode plate inside a vacuum tube as shown in the figure. The work function of the cathode surface is ϕ and the anode is a wire mesh of conducting material kept at a distance d from the… Includes diagram2016 · Multiple correct
  • For photo-electric effect with incident photon wavelength λ, the stopping potential is V0. Identify the correct variation(s) of V0 with λ and λ1​.2015 · Multiple correct
  • An electron in an excited state of Li2+ ion has angular momentum 2π3h​. The de Broglie wavelength of the electron in this state is p π a0 (where a0 is the Bohr radius). The value of p is2015 · Numerical
  • A metal surface is illuminated by light of two different wavelengths 248 nm and 310 nm. The maximum speeds of the photoelectrons corresponding to these wavelengths are u1 and u2, respectively. If the ratio u1 : u2 = 2 : 1 and hc = 1240 eV…2014 · MCQ
  • The work functions of silver and sodium are 4.6 and 2.3 eV, respectively. The ratio of the slope of the stopping potential versus frequency plot for silver to that of sodium is ​.2013 · Numerical