Class 12 Physics NCERT Solutions: Dual Nature of Radiation and Matter PDF

Physics Ncert Solutions Class 12th 2023

Pallavi Pathak
Updated on Jul 4, 2025 17:22 IST

By Pallavi Pathak, Assistant Manager Content

Class 12 Physics Chapter 11 – Dual Nature of Radiation and Matter provides detailed NCERT solutions to boost students' understanding of the key concepts. The chapter provides a clear explanation of quantum physics concepts for better board exams and competitive tests preparation, like NEET and JEE Main exams.
The NCERT solutions provide step-by-step explanations, Class 12 Physics important questions, and solved examples for concept clarity and effective revision. Students must download the free PDF for revising the Dual Nature of Matter Class 12 concepts and practicing questions.
The chapter includes the following important topics:

  • Einstein’s Photoelectric Equation
  • Photoelectric Effect
  • Wave-Particle Duality
  • Electron Emission
  • de Broglie Wavelength

For topic-wise revision through PDF & Solved Exams of Class 12 Physics, read here - NCERT Class 12 Physics Notes for CBSE.

 

Table of content
  • Quick Summary of Chapter 11 – Dual Nature of Radiation and Matter
  • NCERT Class 12 Dual Nature of Radiation and Matter: Key Topics, Weightage and Important Reactions
  • Chapter 11 Dual Nature of Radiation and Matter Important Formulas
  • NCERT Chemistry Class 12th Solution PDF - Dual Nature of Radiation and Matter Chapter Download
  • Dual Nature of Radiation and Matter Question and Answers
  • Benefits of Using NCERT Class 12 Dual Nature of Radiation and Matter Solutions
  • NCERT Solutions For Class 12 Dual Nature of Radiation and Matter- FAQ
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Quick Summary of Chapter 11 – Dual Nature of Radiation and Matter

Following is a quick overview of the Class 12 Physics Chapter 11 – Dual Nature of Radiation and Matter:

  • Chapter 11 Dual Nature of Radiation and Matter includes the light's wave nature through Maxwell's equations and Hertz’s experiments. Also, discoveries like electrons by J.J. Thomson and X-rays by Roentgen.
  • The chapter talks about the cathode rays and electrons. The streams of fast-moving negatively charged particles were identified as the Cathode rays by Thomson. Cathode rays have a universal charge-to-mass ratio irrespective of the material or gas used.
  • It talks about the electron emission in metals. To escape the surface, electrons in metals need a minimum energy called the work function.
  • Hertz discovered and Hallwachs and Lenard studied the photoelectric effect. It involves that when from a metal surface the electrons get emitted at a time when the surface is illuminated by light above a threshold frequency, the effect is dependent on frequency and not on intensity. It is instantaneous.
  • The chapter includes the concept of the wave-particle duality. It involves de Broglie’s hypothesis, which says similar to light, matter exhibits both particle and wave properties.
  • Einstein explained the photoelectric effect’s features by saying that light consists of photons i.e; energy quanta.

Related Links

NCERT Solutions Class 11 and 12  NCERT Notes for Class 11 & 12 NCERT Class 12 Notes

 

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NCERT Class 12 Dual Nature of Radiation and Matter: Key Topics, Weightage and Important Reactions

It is always a smart way to start your preparation by first knowing the topics covered in the Chapter. This chapter includes the important concept of wave-particle duality and the groundbreaking photoelectric effect. See below the topics covered in Chapter 11 – Dual Nature of Radiation and Matter.

Exercise Topics Covered
11.1 Introduction To Dual Nature Of Radiation And Matter
11.2 Electron Emission
11.3 Photoelectric Effect
11.4 Experimental Study Of Photoelectric Effect
11.5 Photoelectric Effect And Wave Theory Of Light
11.6 Einstein’s Photoelectric Equation: Energy Quantum Of Radiation
11.7 Particle Nature Of Light: The Photon
11.8 Wave Nature Of Matter

Important Topics Covered in Class 12 Chapter 11 Dual Nature of Radiation

Students must go through the following topics related to the Class 12 Physics Ch 11 Dual Nature of Radiation.

  • Photoelectric Effect: Discovery, Hertz’s Observation, Hallwachs and Lenard’s Observations
  • Einstein’s Photoelectric Equation: Work Function, Stopping Potential, Threshold Frequency
  • Experimental Verification of Photoelectric Effect: Millikan’s Experiment
  • Wave-Particle Duality: Light as a Wave and as a Particle.
  • de Broglie Hypothesis: Matter Waves and de Broglie Wavelength.
  • Davisson-Germer Experiment: Experimental Proof of de Broglie Waves.
  • Heisenberg’s Uncertainty Principle: Concept and Mathematical Expression.
  • Applications of Wave-Particle Duality: Electron Microscopes and Quantum Tunneling.

Dual Nature of Radiation and Matter Weightage in JEE Main, NEET Exams

Exam Name No. of Questions Percentage
NEET 1-2 questions 2-3%
JEE Main 2-3 questions 2-3%

 

 

Try these practice questions

Q1:

Let K1 and K2 be the maximum kinetic energies of photo-electrons emitted when two monochromatic beams of wavelength λ1andλ2, respectively are incident on a metallic surface. If λ1=3λ2 then:

Q2:

The kinetic energy of emitted electron is E when the right incident on the metal has wavelength λ . To double the kinetic energy, the incident light must have wavelength:

Q3:

THE de Broglie wavelength for an electron and a photon are λ e a n d λ p  respectively. For the same kinetic energy of electron and photon, which of the following presents the correct relation between the de Broglie wavelengths of two

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Chapter 11 Dual Nature of Radiation and Matter Important Formulas

See below the important formulas of Chapter 11 Class 12 Physics Dual Nature of Radiation and Matter:

Important Formulae in Class 12 Physics Chapter 11 Dual Nature of Radiation

  • Photoelectric Effect:
    • Einstein’s Photoelectric Equation:

      h ν = h ν 0 + 1 2 m v max 2 h\nu = h\nu_0 + \frac{1}{2}mv^2_{\text{max}}
    • Work Function ( ϕ \phi ):

      ϕ = h ν 0 \phi = h\nu_0
    • Maximum Kinetic Energy (K.E.):

      K . E max = h ν ϕ K.E_{\text{max}} = h\nu - \phi
    • Stopping Potential (V₀):

      e V 0 = K . E max = h ν ϕ eV_0 = K.E_{\text{max}} = h\nu - \phi
  • De Broglie Wavelength (Wave Nature of Particles):
    • General Formula:

      λ = h p = h m v \lambda = \frac{h}{p} = \frac{h}{mv}
    • For a particle accelerated through potential V (like an electron):

      λ = h 2 m e V \lambda = \frac{h}{\sqrt{2meV}}
    • Numerical Form (for electrons):

      λ ( in  A ˚ ) = 12.27 V \lambda (\text{in Å}) = \frac{12.27}{\sqrt{V}}
  • Momentum of a Photon:

p = h λ p = \frac{h}{\lambda}

  •  Energy of a Photon:

E = h ν = h c λ E = h\nu = \frac{hc}{\lambda}

  • where:

h h = Planck’s constant
ν \nu = frequency of incident light
ν 0 \nu_0 = threshold frequency
m m = mass of the electron

e e = charge of the electron
v max v_{\text{max}} = maximum velocity of photoelectrons

V V = accelerating potential

 

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NCERT Chemistry Class 12th Solution PDF - Dual Nature of Radiation and Matter Chapter Download

To revise quickly and effectively, it is recommended to download the NCERT Solutions PDF for Class 12 Physics Chapter 11 – Dual Nature of Radiation and Matter. The step-by-step answers to textbook questions will provide better clarity and improve the analytical skills of students. The PDF includes the important derivations, solved numericals, and concept-based questions. The PDF is effective for last-minute revision and for your grasp of the Dual Nature of Matter Class 12.
Read here NCERT Solutions for Class 12 Physics for chapter-wise Questions with Answers PDF, Important Topics & Weightage.

NCERT Solution Class 12 Physics Dual Nature of Radiation and Matter PDF: Download Free PDF

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Dual Nature of Radiation and Matter Question and Answers

Q.11.1 Find the

(a) maximum frequency, and

(b) minimum wavelength of X-rays produced by 30 kV electrons.

Ans.11.1 Potential of the electrons, V = 30 kV = 3 × 10 4  V

Energy of the electron, E = e × V  where e = charge of an electron = 1.6 × 10 - 19 C

 

  • Maximum frequency produced by the X-ray = ν

The energy of the electron is given by the relation, E = h ν ,

where h = Planck’s constant = 6.626 × 10 - 34  Js

ν = E h = 3 × 10 4 × 1.6 × 10 - 19 6.626 × 10 - 34  = 7.244 × 10 18  Hz

H e n c e t h e m a x i u m f r e q u e n c y o f X - r a y p r o d u c e d i s 7.244 × 10 18  Hz

 

  • The minimum wavelength produced is given as

  λ = c ν where c = Speed of light in air, c = 3 × 10 18  m/s

  λ = 3 × 10 8 7.244 × 10 18 = 4.14 × 10 - 11  m = 0.0414 nm

Hence, the minimum wavelength produced is 0.414 nm.

Q.11.2 The work function of cesium metal is 2.14 eV. When light of frequency 6  × 10 14  Hz is incident on the metal surface, photoemission of electrons occurs. What is the

(a) maximum kinetic energy of the emitted electrons,

(b) Stopping potential, and

(c) maximum speed of the emitted photoelectrons?

Ans.11.2 Work function of cesium metal,  0  = 2.14 eV

Frequency of light,  ν  = 6  × 10 14  Hz

The maximum kinetic energy is given by the photoelectric effect,  K  =  h ν - 0  ,

Where  h  = Planck’s constant = 6.626  × 10 - 34  Js, 1 eV = 1.602  × 10 - 19  J

K  =  6.626 × 10 - 34 × 6 × 10 14 1.602 × 10 - 19 - 2.14  = 0.345 eV

H e n c e t h e m a x i m u m k i n e t i c e n e r g y o f t h e e m i t t e d e l e c t r o n i s 0.3416 e V

For stopping potential  V 0  , we can write the equation for kinetic energy as:

K  =  V 0  , where e = charge of an electron =  1.6 × 10 - 19

or  V 0 = K e  =  0.345 × 1.602 × 10 - 19 1.6 × 10 - 19  = 0.345 V

Hence, the stopping potential is 0.345 V

Maximum speed of the emitted photoelectrons = v

Kinetic energy K =  1 2  m  v 2  , where m = mass of the electron = 9.1  × 10 - 31  kg

Hence, v =  2 K m  =  2 × 0.345 × 1.602 × 10 - 19 9.1 × 10 - 31  = 348.5  × 10 3  m/s = 346.8 km/s

Therefore, the maximum speed of the emitted photoelectrons is 346.8 km/s

Q.11.3 The photoelectric cut-off voltage in a certain experiment is 1.5 V. What is the maximum kinetic energy of photoelectrons emitted?

Ans.11.3 Photoelectric cut-off voltage,  V 0  = 1.5 V

Maximum kinetic energy of the photoelectrons emitted is given as

K = e V 0  , where e = charge of an electron = 1.6  × 10 - 19  C

K = 1.6  × 10 - 19 × 1.5  = 2.4  × 10 - 19  J

Hence, maximum kinetic energy of the photoelectrons emitted is 2.4  × 10 - 19  J

Q.11.4 Monochromatic light of wavelength 632.8 nm is produced by a helium-neon laser. The power emitted is 9.42 mW.

(a) Find the energy and momentum of each photon in the light beam,

(b) How many photons per second, on the average, arrive at a target irradiated by this beam? (Assume the beam to have uniform cross-section which is less than the target area), and

(c) How fast does a hydrogen atom have to travel in order to have the same momentum as that of the photon?

Ans.11.4 Wavelength of the monochromatic light,  λ = 632.8 n m  = 632.8  × 10 - 9  m

Power emitted by laser, P = 9.42 mW = 9.42  × 10 - 3  W

Planck’s constant, h = 6.626  × 10 - 34  Js

Speed of light, c = 3  × 10 8  m/s

Mass of hydrogen atom, m = 1.66  × 10 - 27  kg

The energy of each photon is given as,  E  =  h c λ  =  6.626 × 10 - 34 × 3 × 10 8 632.8 × 10 - 9  J = 3.141  × 10 - 19  J

The momentum of each photon is given by  p  =  h λ  =  6.626 × 10 - 34 632.8 × 10 - 9  = 1.047  × 10 - 27  kg-m/s

Number of photons arriving per second at a target irradiated by the beam = n

Assume that the beam has a uniform cross-section that is less than the target area.

Hence, the equation for power can be written as,  P = n E

n =  P E  =  9.42 × 10 - 3 3.141 × 10 - 19  = 3.0  × 10 16

Momentum of the hydrogen atom = momentum of the proton = 1.047  × 10 - 27  kg-m/s

The momentum of the hydrogen atom ,  p = m v  , where m = mass of hydrogen atom and v = velocity

Hence, v =  p m  =  1.047 × 10 - 27 1.66 × 10 - 27  = 0.631 m/s

 

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Commonly asked questions
Q:  

11.11 Light of wavelength 488 nm is produced by an argon laser which is used in the photoelectric effect. When light from this spectral line is incident on the emitter, the stopping (cut-off) potential of photoelectrons is 0.38 V. Find the work function of the material from which the emitter is made.

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Q:  

11.5 The energy flux of sunlight reaching the surface of the earth is 1.388×103 W/m2. How many photons (nearly) per square meter are incident on the Earth per second? Assume that the photons in the sunlight have an average wavelength of 550 nm.

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Q:  

11.6 In an experiment on photoelectric effect, the slope of the cut-off voltage versus frequency of incident light is found to be 4.12 ×10-15 Vs. Calculate the value of Planck’s constant.

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Q:  

11.7 A 100W sodium lamp radiates energy uniformly in all directions. The lamp is located at the centre of a large sphere that absorbs all the sodium light which is incident on it. The wavelength of the sodium light is 589 nm.

(a) What is the energy per photon associated with the sodium light?

(b) At what rate are the photons delivered to the sphere?

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Q:  

11.8 The threshold frequency for a certain metal is 3.3 × 1014 Hz. If light of frequency 8.2 × 1014 Hz is incident on the metal, predict the cutoff voltage for the photoelectric emission.

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Q:  

11.9 The work function for a certain metal is 4.2 eV. Will this metal give photoelectric emission for incident radiation of wavelength 330 nm?

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Q:  

11.10 Light of frequency 7.21 × 1014 Hz is incident on a metal surface. Electrons with a maximum speed of 6.0 × 105 m/s are ejected from the surface. What is the threshold frequency for photoemission of electrons?

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Q:  

11.15 What is the de Broglie wavelength of

(a) Bullet of mass 0.040 kg travelling at the speed of 1.0 km/s,

(b) A ball of mass 0.060 kg moving at a speed of 1.0 m/s, and

(c) A dust particle of mass 1.0 × 10–9 kg drifting with a speed of 2.2 m/s?

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Q:  

11.13 What is the

(a) Momentum,

(b) Speed, and

(c) De Broglie wavelength of an electron with kinetic energy of 120 eV.

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Q:  

11.18 Show that the wavelength of electromagnetic radiation is equal to the de Broglie wavelength of its quantum (photon).

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Q:  

11.14 The wavelength of light from the spectral emission line of sodium is 589 nm. Find the kinetic energy at which

(a) An electron, and

(b) A neutron, would have the same de Broglie wavelength.

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Q:  

11.12 Calculate the

(a) Momentum, and

(b) De Broglie wavelength of the electrons accelerated through a potential difference of 56 V.

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Q:  

11.2 The work function of cesium metal is 2.14 eV. When light of frequency 6 ×1014 Hz is incident on the metal surface, photoemission of electrons occurs. What is the

(a) Maximum kinetic energy of the emitted electrons,

(b) Stopping potential, and

(c) Maximum speed of the emitted photoelectrons?

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Q:  

11.3 The photoelectric cut-off voltage in a certain experiment is 1.5 V. What is the maximum kinetic energy of photoelectrons emitted?

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Q:  

11.29 The work function for the following metals is given:

Na: 2.75 eV; K: 2.30 eV; Mo: 4.17 eV; Ni: 5.15 eV. Which of these metals will not give photoelectric emission for a radiation of wavelength 3300 Å from a He-Cd laser placed 1 m away from the photocell? What happens if the laser is brought nearer and placed 50 cm away ?

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Q:  

11.19 What is the de Broglie wavelength of a nitrogen molecule in air at 300 K? Assume that the molecule is moving with the root-mean square speed of molecules at this temperature. (Atomic mass of nitrogen = 14.0076 u)

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Q:  

11.16 An electron and a photon each have a wavelength of 1.00 nm. Find

(a) Their momentum,

(b) The energy of the photon, and

(c) The kinetic energy of electron.

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Q:  

11.17 (a) For what kinetic energy of a neutron will the associated de Broglie wavelength be 1.40 × 10–10 m?

(b) Also find the de Broglie wavelength of a neutron, in thermal equilibrium with matter, having an average kinetic energy of (3/2) k T at 300 K.

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Q:  

11.1 Find the

(a) Maximum frequency, and

(b) Minimum wavelength of X-rays produced by 30 kV electrons.

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Q:  

11.4 Monochromatic light of wavelength 632.8 nm is produced by a helium-neon laser. The power emitted is 9.42 mW.

(a) Find the energy and momentum of each photon in the light beam,

(b) How many photons per second, on the average, arrive at a target irradiated by this beam? (Assume the beam to have uniform cross-section which is less than the target area), and

(c) How fast does a hydrogen atom have to travel in order to have the same momentum as that of the photon?

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Q:  

11.20 (a) Estimate the speed with which electrons emitted from a heated emitter of an evacuated tube impinge on the collector maintained at a potential difference of 500 V with respect to the emitter. Ignore the small initial speeds of the electrons. The specific charge of the electron, i.e., its e/m is given to be 1.76 × 1011 C kg–1.

(b) Use the same formula you employ in (a) to obtain electron speed for a collector potential of 10 MV. Do you see what is wrong ? In what way is the formula to be modified?

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Q:  

11.21 (a) A monoenergetic electron beam with electron speed of 5.20 × 106 m s –1 is subject to a magnetic field of 1.30 × 10–4 T normal to the beam velocity. What is the radius of the circle traced by the beam, given e/m for electron equals 1.76 × 1011C kg–1.

(b) Is the formula you employ in (a) valid for calculating radius of the path of a 20 MeV electron beam? If not, in what way is it modified?

[Note: Exercises 11.20(b) and 11.21(b) take you to relativistic mechanics which is beyond the scope of this book. They have been inserted here simply to emphasize the point that the formulas you use in part (a) of the exercises are not valid at very high speeds or energies. See answers at the end to know what ‘very high speed or energy’ means.]

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Q:  

11.22 An electron gun with its collector at a potential of 100 V fires out electrons in a spherical bulb containing hydrogen gas at low pressure ( mm of Hg). A magnetic field of 2.83 × 10–4 T curves the path of the electrons in a circular orbit of radius 12.0 cm. (The path can be viewed because the gas ions in the path focus the beam by attracting electrons, and emitting light by electron capture; this method is known as the ‘fine beam tube’ method.) Determine e/m from the data.

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Q:  

11.23 (a) An X-ray tube produces a continuous spectrum of radiation with its short wavelength end at 0.45 Å. What is the maximum energy of a photon in the radiation?

(b) From your answer to (a), guess what order of accelerating voltage (for electrons) is required in such a tube?

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Q:  

11.24 In an accelerator experiment on high-energy collisions of electrons with positrons, a certain event is interpreted as annihilation of an electron-positron pair of total energy 10.2 BeV into two -rays of equal energy. What is the wavelength associated with each -ray? (1BeV = 109 eV)

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Q:  

11.25 Estimating the following two numbers should be interesting. The first number will tell you why radio engineers do not need to worry much about photons! The second number tells you why our eye can never ‘count photons’, even in barely detectable light.

(a) The number of photons emitted per second by a Medium wave transmitter of 10 kW power, emitting radio waves of wavelength 500 m.

(b) The number of photons entering the pupil of our eye per second corresponding to the minimum intensity of white light that we humans can perceive ( 10–10 W m-2). Take the area of the pupil to be about 0.4 cm2, and the average frequency of white light to be about 6 × 1014 Hz.

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Q:  

11.26 Ultraviolet light of wavelength 2271 Å from a 100 W mercury source irradiates a photo-cell made of molybdenum metal. If the stopping potential is –1.3 V, estimate the work function of the metal. How would the photo-cell respond to a high intensity ( 105 W m–2) red light of wavelength 6328 Å produced by a He-Ne laser?

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Q:  

11.27 Monochromatic radiation of wavelength 640.2 nm (1nm = 10–9 m) from a neon lamp irradiates photosensitive material made of cesium on tungsten. The stopping voltage is measured to be 0.54 V. The source is replaced by an iron source and its 427.2 nm line irradiates the same photo-cell. Predict the new stopping voltage.

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Q:  

11.28 A mercury lamp is a convenient source for studying frequency dependence of photoelectric emission, since it gives a number of spectral lines ranging from the UV to the red end of the visible spectrum. In our experiment with rubidium photo-cell, the following lines from a mercury source were used:

λ1 = 3650 Å, λ2 = 4047 Å, λ3 = 4358 Å, λ4 = 5461 Å, λ5 = 6907 Å,

The stopping voltages, respectively, were measured to be:

V01 = 1.28 V, V02 = 0.95 V, V03 = 0.74 V, V04 = 0.16 V, V05 = 0 V

Determine the value of Planck’s constant h, the threshold frequency and work function for the material.

[Note: You will notice that to get h from the data, you will need to know e (which you can take to be 1.6 ×10-19 C). Experiments of this kind on Na, Li, K, etc. were performed by Millikan, who, using his own value of e (from the oil-drop experiment) confirmed Einstein’s photoelectric equation and at the same time gave an independent estimate of the value of h.]

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Q:  

11.30 Light of intensity 10–5 W m–2 falls on a sodium photo-cell of surface area 2 cm2. Assuming that the top 5 layers of sodium absorb the incident energy, estimate time required for photoelectric emission in the wave-picture of radiation. The work function for the metal is given to be about 2 eV. What is the implication of your answer?

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Q:  

11.31 Crystal diffraction experiments can be performed using X-rays, or electrons accelerated through appropriate voltage. Which probe has greater energy? (For quantitative comparison, take the wavelength of the probe equal to 1 Å, which is of the order of inter-atomic spacing in the lattice) ( = 9.11 × 10–31 kg).

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Q:  

11.32 (a) Obtain the de Broglie wavelength of a neutron of kinetic energy 150 eV. As you have seen in Exercise 11.31, an electron beam of this energy is suitable for crystal diffraction experiments. Would a neutron beam of the same energy be equally suitable? Explain. (  = 1.675 × 10–27 kg)

(b) Obtain the de Broglie wavelength associated with thermal neutrons at room temperature (27 °C). Hence explain why a fast neutron beam needs to be thermalised with the environment before it can be used for neutron diffraction experiments

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Q:  

11.33 An electron microscope uses electrons accelerated by a voltage of 50 kV. Determine the de Broglie wavelength associated with the electrons. If other factors (such as numerical aperture, etc.) are taken to be roughly the same, how does the resolving power of an electron microscope compare with that of an optical microscope which uses yellow light?

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Q:  

11.34 The wavelength of a probe is roughly a measure of the size of a structure that it can probe in some detail. The quark structure of protons and neutrons appears at the minute length-scale of 10–15 m or less. This structure was first probed in early 1970’s using high energy electron beams produced by a linear accelerator at Stanford, USA. Guess what might have been the order of energy of these electron beams. (Rest mass energy of electron = 0.511 MeV.)

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Q:  

11.35 Find the typical de Broglie wavelength associated with a He atom in helium gas at room temperature (27 °C) and 1 atm pressure; and compare it with the mean separation between two atoms under these conditions.

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Q:  

11.36 Compute the typical de Broglie wavelength of an electron in a metal at 27 °C and compare it with the mean separation between two electrons in a metal which is given to be about 2 × 10–10 m.

[Note: Exercises 11.35 and 11.36 reveal that while the wave-packets associated with gaseous molecules under ordinary conditions are non-overlapping, the electron wave-packets in a metal strongly overlap with one another. This suggests that whereas molecules in an ordinary gas can be distinguished apart, electrons in a metal cannot be distinguished apart from one another. This indistinguishibility has many fundamental implications which you will explore in more advanced Physics courses.]

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Q:  

11.37 Answer the following questions:

(a) Quarks inside protons and neutrons are thought to carry fractional charges [(+2/3)e ; (–1/3)e]. Why do they not show up in Millikan’s oil-drop experiment?

(b) What is so special about the combination e/m? Why do we not simply talk of e and m separately?

(c) Why should gases be insulators at ordinary pressures and start conducting at very low pressures?

(d) Every metal has a definite work function. Why do all photoelectrons not come out with the same energy if incident radiation is monochromatic? Why is there an energy distribution of photoelectrons?

(e) The energy and momentum of an electron are related to the frequency and wavelength of the associated matter wave by the relations:

E = h ν , p = h λ , But while the value of  is physically significant, the value of  (and therefore, the value of the phase speed  ) has no physical significance. Why?

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Benefits of Using NCERT Class 12 Dual Nature of Radiation and Matter Solutions

Here are the key benefits of using NCERT Class 12 Dual Nature of Radiation and Matter Solutions, read below;

  • NCERT Solutions for Dual Nature of Radiation and Matter covers detailed explanations for all concepts like photoelectric effect, de Broglie wavelength, and Einstein’s photoelectric equation for Class 12 students.
  • Our solutions follow the latest CBSE Class 12 Physics syllabus and cover all NCERT textbook exercise questions. We have designed our answers to provide numerical solutions in our Dual Nature of Radiation and Matter NCERT Solutions.
  • One important benefit is accessibility of a free downloadable PDF of NCERT Solutions, allowing to study offline without any internet connection.
  • Students can use NCERT Dual Nature of Radiation and Matter Solutions to practice questions exactly like the CBSE Exams, since CBSE and other boards also design their exam based on NCERT Textbooks.

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