Early rise of Quanta and Einstein's ground-breaking papers
This course focuses on the beautiful mathematical "tricks" used in the late 19th / early 20th century by Planck and that led to the discovery of a new field: Quantum Physics.
The math used by Plack and Einstein for the discovery of Quantum Physics and the foundations of thermodynamics
First part of the course:
The first part of the course showcases the beautiful mathematics that, in the late 19th century/ early 20th century, led to the discovery of a revolutionary branch in physics: Quantum Mechanics.
Planck postulated that the energy of oscillators in a black body is quantized. This postulate was introduced by Max Planck in his derivation of his law of black body radiation in 1900. This assumption allowed Planck to derive a formula for the entire spectrum of the radiation emitted by a black body (we will also derive this spectrum in this course). Planck was unable to justify this assumption based on classical physics; he considered quantization as being purely a mathematical trick, rather than (as is now known) a fundamental change in the understanding of the world.
In 1905, Albert Einstein adapted the Planck postulate to explain the photoelectric effect, but Einstein proposed that the energy of photons themselves was quantized (with photon energy given by the Planck–Einstein relation), and that quantization was not merely a "mathematical trick". Planck's postulate was further applied to understanding the Compton effect, and was applied by Niels Bohr to explain the emission spectrum of the hydrogen atom and derive the correct value of the Rydberg constant.
In addition to the very useful mathematical tools that will be presented and discussed thoroughly, the students have the opportunity to learn about the historical aspects of how Planck tackled the blackbody problem.
Calculus and multivariable Calculus are a prerequisite to the course; other important mathematical tools (such as: Fourier Series, Perseval's theorem, binomial coefficients, etc.) will be recalled, with emphasis being put on mathematical and physical insights rather than abstract rigor.
Second part of the course
By the end of June 1902, just after being accepted as Technical Assistant at the Federal Patent Office in Bern, Albert Einstein, 23, sent to the renowned journal Annalen der Physik a manuscript with the bold title “Kinetic Theory of Thermal Equilibrium and of the Second Law of Thermodynamics”. In the introduction, he explains that he wishes to fill a gap in the foundations of the general theory of heat, “for one has not yet succeeded in deriving the laws of thermal equilibrium and the second law of thermodynamics using only the equations of mechanics and the probability calculus”. He also announces “an extension of the second law that is of importance for the application of thermodynamics”. Finally, he will provide “the mathematical expression of the entropy from the standpoint of mechanics”.
In particular, in the second part of the course we will see the mathematics Einstein used in his paper from 1902.
Besides, other concepts from Classical mechanics are explained, such as Liouville's theorem (this theorem is used by Einstein in his article), as well as Hamilton equations and more.
For the second part, the student should already be familiar with phase space and other concepts from classical physics (such as Lagrange equations).
Third part of the course
In the third part of the course some of the articles of Einstein's Annus Mirabilis are explained. In particular, the article on the photoelectric effect and that on the Brownian motion.
Irrelevance of Shape of the Cavity
FREE PREVIEWWave equation for Electromagnetic Waves
FREE PREVIEWSolution to the Wave Equation
FREE PREVIEWSatisfaction of Boundary Conditions
Number of Modes per Frequency
Average Energy per Mode
Distribution of the Average Energy, Planck's idea
Systems of Particles, Binomial Coefficient
Number of Arrangements of the Particles into the Energy Levels
Sterling's Approximation
Preparing to maximize the Number of Arrangements
Maximizing the Number of Arrangements
Expression for the Energy per Mode
Planck's Mathematical Trick
Calculation of the Average Energy per Mode part 1
Calculation of the Average Energy per Mode part 2
Classical vs Quantum
Energy per Volume per Wavelength and Energy per Volume
Planck's Integral
Brief Summary of Fourier Analysis
Parseval's Theorem
Ultraviolet Catastrophe and Energy per Unit Surface
Calculation of the Series 1/n^4
Putting Results Together
Deriving the Stefan-Boltzmann Law part1
Deriving the Stefan-Boltzmann Law part2
Derivation of Maxwell Boltzmann distribution
Planck's idea for the mathematical solution to the black body problem
The mathematics that Einstein used in one of his papers on thermodynamics part 1
FREE PREVIEWThe mathematics that Einstein used in one of his papers on thermodynamics part 2
FREE PREVIEWThe mathematics that Einstein used in one of his papers on thermodynamics part 3
FREE PREVIEWThe mathematics that Einstein used in one of his papers on thermodynamics part 4
FREE PREVIEWThe mathematics that Einstein used in one of his papers on thermodynamics part 5
Mathematical proof of Liouville theorem
FREE PREVIEWCanonical transformations and generating functions
FREE PREVIEWHamilton equations from a variational principle
FREE PREVIEWVariation principle derived from Newton's second law
FREE PREVIEWSimpler proof of Liouville's theorem
FREE PREVIEWEinstein's different approach for the derivation of the entropy
FREE PREVIEWIdeal gas law derived from Statistical Mechanics
Part 1 of Einstein's article on the photoelectric effect
Part 2 of Einstein's article on the photoelectric effect
Part 3 of Einstein's article on the photoelectric effect
Part 4 of Einstein's article on the photoelectric effect
Step-by-step explanation of Einstein's article on the Brownian motion
Proof that Entropy is a Function of State and How to Derive it from Lagrange Equations (part 1)
FREE PREVIEWProof that Entropy is a Function of State and How to Derive it from Lagrange Equations (part 2)
Proof that Entropy is a Function of State and How to Derive it from Lagrange Equations (part 3)