AKTU - QUANTUM MECHANICS for Engineering Physics

PHYSICS MADE EASY(Dr. Divya Ghildyal)
10 Jun 202220:18

Summary

TLDRIn this lecture on Quantum Mechanics for first-year engineering physics students, the instructor covers key topics from the AKTU syllabus. The lecture begins with an introduction to Black Body Radiation, explaining the concept and its relation to Stephen's Law, which states that the energy radiated by a black body is proportional to the fourth power of its absolute temperature. The instructor then delves into the wave-particle duality of light and matter, emphasizing the importance of understanding the time-dependent and independent Schrödinger wave equations. The lecture concludes with a discussion on Compton Effect, providing the formula for the variation in wavelength when a particle undergoes this effect. The instructor also guides students on how to approach numerical problems in quantum physics, ensuring they understand the derivations and applications of these fundamental concepts.

Takeaways

  • 📚 The lecture focuses on Unit 3 of the AKTU Engineering Physics syllabus, specifically on quantum mechanics.
  • 🌑 Black body radiation is a central concept, with black bodies absorbing all radiation and emitting none.
  • 🔢 Several important laws related to energy were discussed: Stefan's Law, Wien's Law, Rayleigh-Jeans Law, and Planck's Law, each with its own formula and principles.
  • ⚛️ Wave-particle duality highlights that light behaves both as a wave and a particle under different conditions.
  • 📊 Wien's Law explains how the wavelength of maximum energy emitted by a black body shifts towards shorter wavelengths as temperature increases.
  • ✍️ Planck's oscillator and its average energy were derived, emphasizing the need to understand this for exams.
  • ⚙️ The Schrödinger wave equation is crucial, and students should know both the time-dependent and time-independent versions.
  • 💡 Compton effect and its impact on wavelength changes when a particle undergoes the effect were also covered.
  • 🔑 Students are advised to memorize key laws and equations, particularly Planck's Radiation Law, which has been tested in exams.
  • 📝 The lecture concluded with a review of Stefan's Law, the dual nature of light, and advice on solving numericals in quantum mechanics for exams.

Q & A

  • What are the five laws related to energy covered in the quantum mechanics unit of the AKTU Engineering Physics syllabus?

    -The five laws related to energy in the quantum mechanics unit are Black Body Radiation, Stephen's Law, Wayne's Law, Rayleigh's Law, and Planck's Law.

  • What is the significance of the term 'black body' in the context of quantum mechanics?

    -A black body is an idealized object that absorbs all incident radiation and emits no radiation. It is used as a model for understanding thermal radiation.

  • What is Stephen's Law and how is it expressed mathematically?

    -Stephen's Law states that the total radiant energy emitted by a black body is proportional to the fourth power of its absolute temperature. Mathematically, it is expressed as E = σT^4, where E is the energy, σ is Stephen's constant (5.67 x 10^-8 W/m^2K^-4), and T is the temperature in Kelvin.

  • What does the graph of energy versus wavelength according to Stephen's Law show?

    -The graph of energy versus wavelength according to Stephen's Law shows that at the peak value of energy, the wavelength is minimum, and as the energy drops, the wavelength increases.

  • What is the significance of Wien's Displacement Law in quantum mechanics?

    -Wien's Displacement Law states that the product of the wavelength corresponding to maximum energy (λm) and the temperature (T) is a constant. This law helps in understanding how the peak of the spectral distribution curve shifts towards shorter wavelengths as the temperature increases.

  • What is the mathematical expression for Rayleigh-Jeans Law?

    -Rayleigh-Jeans Law is given by Eλ = (8πkT) / (λ^4), where Eλ is the energy per unit wavelength, k is the Boltzmann constant, T is the temperature in Kelvin, and λ is the wavelength.

  • How is the average energy of a Planck's oscillator derived?

    -The average energy of a Planck's oscillator is derived by considering the total energy of the oscillators and dividing it by the total number of oscillators. The formula is given by ⟨E⟩ = (hν / (e^(hν/kT) - 1)), where h is Planck's constant, ν is the frequency, k is the Boltzmann constant, and T is the temperature.

  • What is Planck's radiation formula and how is it used?

    -Planck's radiation formula is given by u(ν)dν = (8πhν^2/c^3) dν / (e^(hν/kT) - 1), where u(ν) is the energy density per unit frequency, h is Planck's constant, ν is the frequency, c is the speed of light, and kT is the product of Boltzmann's constant and temperature. This formula is used to calculate the spectral radiance of a black body at a given temperature.

  • What is the Compton Effect and what is its significance in quantum mechanics?

    -The Compton Effect is the increase in wavelength of X-rays when they scatter off electrons. It demonstrates the particle nature of light and is significant in quantum mechanics as it provides evidence for the quantization of energy and momentum.

  • How does the lecturer suggest students approach numerical problems in quantum physics?

    -The lecturer suggests that students should approach numerical problems by showing each step of the solution, including formulating the problem, unit conversions, and applying the correct equations, to ensure they receive marks for each part of the solution.

Outlines

00:00

📚 Introduction to Quantum Mechanics

The lecture begins with an introduction to Unit 3 of the Engineering Physics syllabus for first-year BTEC students, focusing on quantum mechanics. The syllabus includes five energy laws: black body radiation, Stephen's law, Wayne's law, Rayleigh's law, and Planck's law. Students are advised to memorize these laws and understand their derivations, particularly Planck's law and the concept of energy average of a Planck's oscillator. The lecture also covers wave-particle duality, Schrödinger's wave equation, and the Compton effect. The explanation starts with the concept of a black body, which absorbs all radiation and emits none, and the construction of an approximate black body in a lab using a metallic cavity.

05:02

🌡️ Stephen's Law and Black Body Radiation

This section delves into Stephen's law, which describes the energy distribution among different wavelengths for black body radiation. It states that the total radiant energy emitted by a black body is proportional to the fourth power of its absolute temperature. The constant of proportionality, known as Stephen's constant, is introduced with a value of 5.67 x 10^-8 Wm^-2K^-4. The lecture then discusses the peculiar feature of the spectral distribution curve, which shows that at the peak energy, the wavelength is minimum, and as the energy decreases, the wavelength increases. Wayne's law is also introduced, explaining the relationship between wavelength and temperature, where the product of wavelength and temperature is a constant, indicating a shift towards shorter wavelengths as temperature increases.

10:03

🌱 Derivation of Planck's Radiation Law

The paragraph focuses on the derivation of Planck's radiation law, starting with the concept of energy levels of an oscillator and the average energy of a Planck's oscillator. The total number of oscillations and the total energy are calculated using the Boltzmann factor and the Einstein equation. The derivation involves summing geometric progressions and applying mathematical series formulas to arrive at the expression for the average energy of a Planck's oscillator. The final formula derived is E = hμ / (e^(hμ/kT) - 1), which is a key result in quantum mechanics.

15:06

🌞 Planck's Radiation Formula and Wien's Displacement Law

This part of the lecture covers Planck's radiation formula, which describes the number of oscillations per unit volume within a specific frequency range. The formula is given in terms of frequency and then converted to terms of wavelength using the relationship c = μλ, where c is the speed of light and λ is the wavelength. The lecture also discusses Wien's displacement law, which estimates the temperature of the sun based on the maximum wavelength of emitted radiation. The units of wavelength are normalized to match the units of Wien's constant to calculate the temperature.

20:08

📬 Closing Remarks and Contact Information

The lecture concludes with a summary of the key points covered, including Stephen's law, the dual character of light, Planck's radiation law, and Wien's law. The instructor invites students to subscribe to the channel for more content and provides contact information for feedback or suggestions. The instructor's email and phone number are given for direct communication.

Mindmap

Keywords

💡Black Body Radiation

Black body radiation refers to the theoretical concept of an object that absorbs all incident radiation and reflects none, emitting radiation based solely on its temperature. In the video, the lecturer explains how black bodies are idealized objects, and mentions real-world examples like carbon arc lamps and black platinum that approximate this behavior. It is a key concept in quantum mechanics for understanding energy distribution.

💡Stefan's Law

Stefan's Law, or the Stefan-Boltzmann Law, states that the total energy radiated per unit surface area of a black body is proportional to the fourth power of the absolute temperature. The video emphasizes its importance in understanding black body radiation, and how it helps calculate the energy emitted by such bodies, crucial for students studying thermodynamics and quantum mechanics.

💡Wave-Particle Duality

Wave-particle duality is a fundamental concept in quantum mechanics, stating that particles such as photons exhibit both wave-like and particle-like properties. The lecturer briefly touches on how light can behave as both a wave and a particle depending on the context, providing a foundation for understanding other quantum phenomena like the Compton effect.

💡Schrodinger Wave Equation

The Schrodinger wave equation describes how the quantum state of a physical system changes with time. In the lecture, both the time-dependent and time-independent versions of this equation are mentioned, stressing their significance in understanding the behavior of particles at the quantum level. This equation is crucial for analyzing systems like a particle in a one-dimensional box, a common example in quantum mechanics.

💡Planck's Law

Planck's Law describes the distribution of electromagnetic radiation emitted by a black body in thermal equilibrium. It marked a major breakthrough in physics, introducing the concept of quantized energy levels. The lecturer focuses on deriving the formula for the average energy of a Planck oscillator, explaining its importance in the broader context of quantum mechanics and black body radiation.

💡Compton Effect

The Compton effect refers to the increase in wavelength of X-rays or gamma rays when they are scattered by electrons. This phenomenon provides evidence for the particle nature of light, as discussed in the video. The lecturer mentions the Compton effect in the context of quantum mechanics, emphasizing its relevance to understanding light's dual nature and the behavior of photons.

💡Wien's Law

Wien's Law states that the wavelength corresponding to the maximum energy emitted by a black body is inversely proportional to its temperature. The lecture explains this law using a spectral distribution curve, illustrating how the peak of the radiation shifts toward shorter wavelengths as temperature increases. This law is essential for explaining the color of stars and other hot objects.

💡Rayleigh-Jeans Law

The Rayleigh-Jeans Law provides a classical approximation for the energy distribution in the thermal radiation of a black body. It works well at longer wavelengths but fails at shorter ones, leading to the ultraviolet catastrophe, which was later resolved by Planck's quantum theory. The lecturer briefly mentions this law as one of the fundamental equations students need to remember for exams.

💡Boltzmann Factor

The Boltzmann Factor is an exponential term that describes the probability of a system being in a certain energy state at a given temperature. In the video, the lecturer explains its role in determining the energy distribution among Planck oscillators, which are fundamental in understanding black body radiation and thermodynamic systems.

💡Geometric Progression

Geometric progression is a sequence of numbers where each term after the first is found by multiplying the previous term by a constant. The lecturer uses this mathematical concept to explain how the number of oscillations in a system can be calculated, specifically applying it to the sum of oscillations in Planck’s radiation law.

Highlights

Introduction to Quantum Mechanics unit in the AKTU Engineering Physics BTEC first year syllabus.

Explanation of the five laws related to energy: Black body radiation, Stephen's law, Wayne's law, Rayleigh-Jeans law, and Planck's law.

Emphasis on memorizing the statements and deriving expressions for energy, specifically for a Planck's oscillator.

Discussion on wave-particle duality and the concept of matter waves.

Importance of understanding both time-dependent and time-independent Schrödinger wave equations.

Detailed case study on a particle trapped in a one-dimensional box.

Definition and formula for Compton effect and its significance.

Description of a black body and its properties, including examples like carbon arc lamp and platinum black.

Stephen's law and its mathematical expression relating total radiant energy to the fourth power of absolute temperature.

Wayne's law and its displacement law, explaining the shift of maximum energy wavelength with temperature.

Rayleigh-Jeans law and its formula for energy distribution in the thermal spectrum.

Planck's theory of black body radiation and the derivation of the average energy of an oscillator.

Derivation of Planck's radiation law and its significance in quantum physics.

Explanation of the derivation process for the average energy of Planck's oscillator.

Application of Planck's radiation formula in deriving Einstein's relationship in laser physics.

Numerical example using Wien's displacement law to estimate the temperature of the sun.

Final summary of the lecture's key points, including Stephen's law, Planck's radiation law, and Wien's law.

Invitation for feedback and suggestions to improve the lecture series.

Transcripts

play00:03

good afternoon dear students in

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continuation with my lecture series on

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aktu engineering physics btec first year

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syllabus today i am going to brief you

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about unit 3 quantum mechanics okay now

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first let us have a look at the syllabus

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of this unit

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quantum mechanics unit the first line

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consists of the five laws related to

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energy that is black body radiation

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stephen's law wayne's law ray league

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gene's law and planck's law you have to

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memorize the statement of these four

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laws

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and derive an expression for

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energy average energy of a planck's

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oscillator

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next wave particle duality you know

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light possesses dual character at times

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it behaves as a wave and at times it

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behaves as a particle

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matter waves which consist of

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both the wave component and the particle

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component the most important time

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dependent and independent schrodinger

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wave equation

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one year if the time independent part is

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asked the very next year you are asked

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about the time independent schrodinger

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wave equation you should be knowing

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their derivation and one study case in

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detail related to particle trapped in

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one dimensional box

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only one case and last compton effect

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the definition and the formula for

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variation of wavelength when a particle

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undergoes compton effect okay let us

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begin with the syllabus so the first

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part is black body radiation what is a

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black body a black body is one which

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absorbs all radiation and emits none a

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perfect black body is very hard to find

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but we can say carbon arc lamp black

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platinum black they can approximately be

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treated as black body if you want to

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make a black body in the lab then a very

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simple method is you take a metallic

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cavity in the form of a double wall here

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as you can see

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hollow copper sphere with lamp black

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coating inside

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and nickel outside when radiation falls

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in this cavity it will enter the

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enclosure and suffer

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multiple reflections inside at the

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interior surface

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at each reflection a part of radiation

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will be absorbed finally the incident

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beam will become weak and absorbed by

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the inner surface of the body this is an

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approximate example of black body

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not hundred percent black body now black

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body stephen's law gives you the law for

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energy distribution among different

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wavelengths according to steepen law the

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total

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radiant energy that is emitted by a

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black body

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energy emitted by a black body

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is proportional to the fourth power of

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absolute temperature

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when we remove this proportionality sign

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we introduce

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a constant here which is known as

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stephen's constant and the mathematical

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value of this defense constant is

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5.67

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into 10 to the power of minus 8 vip per

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meter square kelvin to the power of

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minus 4. stephen's law gave the total

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energy radiated by a black body one

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thing which is unique about this is that

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the spectral distribution curve

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plotted between the energy radiated by

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the black body and the wavelength

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shows one peculiar feature that is here

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have a look at this graph on the y-axis

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you are having the energy and on the

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x-axis the wavelength at the peak value

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of energy

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wavelength is minimum

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and as the energy drops the wavelength

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increases

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this is one particular feature of the

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plot of energy

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versus wavelength given by

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wayne's law which states that the

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product of

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lambda m into t is a constant that means

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the wavelength

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corresponding to

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maximum energy

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represented by

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the peak of the curve shifts towards the

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shorter wavelength as the temperature

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increases this is known as vein's

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displacement law that is lambda m into t

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is a constant and lambda m corresponds

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to

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the maximum wavelength and t corresponds

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to the temperature in kelvin so from

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wayne's law the maximum energy point

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shifts towards the shorter wavelength

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side when the temperature of body is

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raised

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by

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or it is increased so the maximum energy

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emitted by a black body is proportional

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also to the four fifth power of absolute

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temperature

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rayleigh gene's law says that the energy

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distribution in the thermal spectrum is

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given by

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e lambda is equal to

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8 pi k t divided by lambda to the power

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of 4 where lambda is wavelength k is

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boltzmann constant these are just the

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statements of these laws please remember

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in your syllabus

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not much detail is required for you to

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learn you just remember the laws and

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their statements and their mathematical

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expressions now this derivation is

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important it has been asked in your 2022

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paper

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what is clank's theory of black body

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radiation obtain an expression for the

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average energy of the oscillator and

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derive the planck's radiation law see

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this was asked in aktu 2022 march paper

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and it was a 10 mark question from

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section c now we will derive this step

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by step please be ready with the print

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out of this page i will tell you the

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step by step derivation of this

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expression and along with me even you

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will be able to derive it see

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the frequency of radiation that is

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emitted by an oscillator is the same as

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the frequency of its vibration

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linear oscillator will have only

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discrete energy values e and discrete

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means n equal to one two three four e n

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is n h mu where n is one two three four

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also this is comes from the einstein

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equation now average energy of planck's

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oscillator

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let

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n be the total number of oscillations

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and e the total energy so how do you get

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the formula for average you take the

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total energy and divide it by the number

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of oscillations so let n naught n1 n2 be

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number of oscillations

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having energies

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0

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h mu 2 h mu where has this come from

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this has come from the expression e n is

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equal to n h mu

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when i put n equal to 0 it becomes 0

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when i put n equal to 1 it becomes h mu

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when i put n equal to 2 it becomes 2 h

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mu this way the series goes on and the

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relative probability

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that an oscillator has an energy h mu at

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a temperature t is given by boltzmann

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factor e to the power of minus h mu by

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kt number of oscillations

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having energy n h mu is given by

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n n equal to n naught e to the power of

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minus n h mu divided by k t where once

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again n is the integer 0 1 2 3 etc and

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when we keep the different values of n

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we get the energy levels for those

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specific values of n okay next step

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total number of oscillations will be

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given by

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n equal to n naught plus n one plus n

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two plus n three now in this expression

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we will start putting the values of n

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naught n one and

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n two n naught

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n 1 is n naught e to the power of minus

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h mu by k t

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n 2 is n naught e to the power of minus

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2 h mu by k t

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n naught n 3 is n naught e to the power

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of minus 3 h mu by kt now we take n

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naught common from this expression and

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inside we get 1 plus e to the power of

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minus h mu by kt plus e to the power of

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minus 2 h mu by kt plus e to the power

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of minus 3 h mu by kt and so on if you

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remember from your mathematics the sum

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of geometric progression is given by

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1 plus x plus x square so on is equal to

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1 upon 1 minus x so in this case x is

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equal to e to the power of minus h mu by

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kt so the n expression becomes

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n

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equal to here n equal to n naught into 1

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upon

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1 minus e minus

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h mu by k t that is total number of

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oscillations will be equal to this value

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now let us find the value of total

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energy why are we finding total n and

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total e because we need the average so

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we will divide e by h to get the average

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so according to the famous einstein

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equation

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e equal to n

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h mu where n is 1 2 3 4 etc

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from the einstein's expression we will

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take e equal to n naught into 0 for z 0

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state n equal to 1 n 1 into h mu n equal

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to 2 n 2 into 2 h mu n 3 into 3 h mu and

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so on using the expression n n is equal

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to n naught e to the power of minus n h

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mu by k p putting these values we get

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e is equal to h mu n naught e to the

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power of minus h mu by k t plus 2 h mu n

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naught e to the power of minus 2 h mu by

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k t plus and so on there is one more

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mathematical formula of the series 1

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plus x plus 2x square plus 3x cube etc

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equal to 1 upon 1 minus x whole square

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where x is e to the power of minus h mu

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by kt so

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this series reduces to equal to

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h mu

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n naught e to the power of minus 2 h mu

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by kt

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into 1 upon 1 minus e to the power of

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minus h mu by kt whole square where have

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we got this from

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this is the formula for sum of series

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and x has been put as e to the power of

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minus h mu by kt so the total energy

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comes out as e equal to n naught e to

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the power of minus h mu by kt

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into h mu upon 1 minus e to the power of

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minus h mu by kt whole square now we

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have an expression for e we have an

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expression for n what do we want we want

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the average so we are going to divide e

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by n to get the average energy of the

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planck's oscillator here e bar is equal

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to e upon n you put these values n

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naught n naught gets cancelled cross

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multiply this expression and you get e

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equal to

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h mu upon e to the power of h mu by kt

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minus 1 this is average energy of

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planck's oscillator it was a 10 mark

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question of section c

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okay now planck's radiation formula what

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the why are we always using the word

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planck because it is related to your

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planck scientist so planck's radiation

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formula you just only need to remember

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the formula there are no derivations no

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details in your aktu syllabus the number

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of oscillations per unit volume lying in

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the frequency range mu

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and mu plus d mu from rayleigh gene's

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law is given by 8 pi mu square square d

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mu divided by c cube where c is the

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velocity of light and u mu d mu is

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number of oscillators per unit volume

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into average velocity so the planck's

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radiation formula is given by

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u mu d mu is equal to 8 pi h upon c cube

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into mu cube d mu upon e to the power of

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h mu by kt minus 1 this has been used in

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deriving einstein's relationship in

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laser okay so from planck's radiation

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formula we in terms of frequency we get

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velocity is equal to frequency into

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wavelength so c is equal to mu into

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lambda you put this value in the above

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expression and you can also write this

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in terms of lambda

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numerical on veins displacement law

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estimates the temperature of sun

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given lambda m is equal to 4900 angstrom

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and veins constant is

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0.292 centimeter per kelvin

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what was wayne's law lambda m into t is

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equal to a constant

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now we cannot equate any equation as per

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unit and dimension unless and until the

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units or the dimensions on both sides of

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the equation are not same let us have a

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closer look at the values that have been

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given to us in the question we note that

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wavelength has been given in terms of

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angstrom

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and wayne's constant is in terms of

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centimeter so our first target is to

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normalize these units either change

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angstrom to centimeter or change

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centimeter to angstrom

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so

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for writing this formula in a tu exam i

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will get one mark if this is a five mark

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question

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now i am changing angstrom to centimeter

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we know that one angstrom is equal to 10

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to the power of minus 10 meter

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and 100 centimeters equal to 1 meter so

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1 angstrom is 10 to the power of minus 8

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centimeter so given lambda m 4900

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angstrom is equal to 4900

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into 10 to the power of minus 8

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centimeter b

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0.292 centimeter per kelvin so your

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temperature of sun comes out as b by

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lambda m putting the value

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0.292 divided by 4900 into 10 to the

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power of minus 8 we get

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5.95 into 10 to the power of 3 so this

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was this numerical is going to be of 5

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marks you will be getting marks

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as per step by step solution which you

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are going to show in your exam like you

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will get one mark if you write this

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formula lambda m equal to uh lambda m

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into t is equal to b

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one mark if you convert angstrom to

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centimeter another one mark for

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normalizing the units one mark again if

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you keep the numerical values properly

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and last one mark for the correct answer

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this is how you have to approach the

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numericals in

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quantum physics okay let me quickly

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revise with you what did i teach you

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today i told you about stephen's law e

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equal to sigma t to the power of 4 i

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told you that

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light has a dual character and i told

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you about planck's radiation law and

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wayne's law thank you please subscribe

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to my channel for any suggestions or

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feedback please mail to me at divya

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gildial

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gmail.com or my number nine eight one

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zero three two zero three zero three

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your suggestions are always welcome

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thank you

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Related Tags
Quantum MechanicsPhysics LectureBlack BodyPlanck's LawWave-Particle DualitySchrodinger EquationCompton EffectEngineering PhysicsAKTU SyllabusEducational Content