
Derive the variational principle from Newton's second law for a single particle, showing the Lagrangian L = T−V yields the stationary action ∫(T−V) dt.
Derive the Lagrangian for a two-link double pendulum with masses m1, m2 and lengths L1, L2 by combining kinetic energy and gravity-based potential energy expressed in angles phi1 and phi2.
Explore invariant length element ds^2 = c^2 dt^2 − dx^2 and the moving-clock relation d tau = dt sqrt(1 − v^2/c^2). See how it underpins special relativity and general relativity.
Einstein shows the invariance of the infinitesimal volume element by relating the determinant of the metric tensor to its transformed determinant via a Jacobian, yielding sqrt(-g') = J sqrt(-g).
Derive the Laplacian in spherical coordinates by formulating the gradient with tensors and matrices, then translate to index notation and verify with a Matlab implementation.
Explains finding minimal surfaces with fixed boundary by optimizing the area functional for z(x,y). Presents two nontrivial solutions: the catenoid and the helicoid.
Explore Cauchy's integral formula and its generalization, deriving higher order derivatives as contour integrals of f(w)/(w - z)^{n+1} and noting winding number effects.
Explore Laurent series in complex calculus, a generalization of Taylor and Maclaurin series near z0, through contour integrals on gamma curves and Cauchy integral formula.
Derive the Taylor series from the Laurent expansion for a function continuous at z0 by using a contour integral around gamma once, showing that the coefficients c_n equal f^(n)(z0)/n!.
Use contour integration around the real axis with a small indentation at zero to compute the principal value of e^{i ω z}/z, yielding i π and its cos/sin implications.
Prove the Dirac delta integral representation by applying the Fourier transform to 1/(t(t - x)) and evaluating the resulting integral via contour integration, using the signum of k.
Derive a simple, intuitive method to evaluate the third Gaussian-type integral from Feynman's path integral appendix, handling a 1/x^2 term and complex numbers.
Explain notational conventions for the Fourier transform and Fourier series, including space versus time domains and conjugate variables such as k and omega.
Represent q(x,y) and w(x,y) with a double Fourier sine series for a thin plate with zero boundary loads, solving nabla^4 w = q/d and noting high modes decay.
Overview
This course brings together several advanced mathematical tools that often appear separately in physics, engineering, and applied mathematics, but which are deeply connected when studied in the right order.
We will move through the calculus of variations, integral transforms, tensor analysis, complex analysis with residue calculus, the intuition behind path integrals and quantization, and a final part on constrained optimization. Along the way, the course also touches on Hamiltonian mechanics, Poisson brackets, the Schrödinger equation, Feynman diagrams, Lorentz transformations, spinors, and Lie algebras.
The goal is not only to present formulas, but to build mathematical intuition. I try to show why these tools were introduced, how they are used, and how they connect different areas of classical and quantum physics.
This course is intended for students, professionals, researchers, and anyone with a solid mathematical background who wants to strengthen their understanding of advanced mathematical methods and their applications in physics and engineering.
What You Will Learn
Calculus of Variations
We begin with the idea of optimizing functionals, which is one of the key mathematical structures behind classical mechanics, field theory, geometry, and many engineering problems.
You will study the Euler-Lagrange equations, boundary conditions, variational principles, and applications such as geodesics and mechanical systems. The emphasis is on understanding not only how to use the equations, but also where they come from.
Integral Transforms
The course then develops important tools such as Fourier and Laplace transforms. These methods are essential for solving differential equations, studying signals, and transforming difficult problems into more manageable ones.
The aim is to make these techniques feel natural rather than purely formal, with examples showing how they simplify calculations and reveal hidden structure.
Tensor Analysis
A significant part of the course is devoted to tensors and their applications. Tensors are introduced as mathematical objects that naturally appear in geometry, continuum mechanics, relativity, and field theory.
The presentation follows a pedagogical path similar to what one might encounter in a course on General Relativity. We discuss tensor transformations, covariant notation, the metric tensor, and the role of tensors in describing physical laws independently of the chosen coordinates.
Complex Analysis and Residue Calculus
The course also includes complex analysis, with particular attention to residues and contour integration.
Residue calculus is one of the most elegant and useful tools in mathematical physics. We will see how complex functions can be used to evaluate real integrals and solve problems that would otherwise be much harder to approach directly.
Path Integrals and Quantization
Another important part of the course is devoted to the intuition behind path integrals and the quantization of classical theories.
The purpose here is not to replace a full course in quantum field theory, but to help students understand how ideas from classical mechanics can be reformulated in a way that leads naturally toward quantum mechanics and, eventually, field theory.
Mathematical Connections Between Classical and Quantum Physics
The course also builds bridges between classical mechanics and quantum physics through Poisson brackets, Hamiltonian mechanics, the path integral approach, the Schrödinger equation, and the first ideas behind Feynman diagrams.
This part is especially useful for students who already know some classical mechanics and want to understand how the language of modern theoretical physics begins to emerge from it.
Lorentz Algebra, Lie Groups, and Spinors
Two recent sections have been added to the course, focusing on the Lorentz group, its Lie algebra, spinors, Pauli matrices, Dirac matrices, operators, and intrinsic angular momentum.
These topics are closely related to quantum mechanics, relativity, and quantum field theory. They also show beautifully how tensors, transformations, and symmetry ideas fit together.
Constrained Optimization
The final part of the course introduces constrained optimization problems, especially through the method of Lagrange multipliers.
Here, too, the focus is not only on the standard procedure, but also on developing the intuition behind it. The goal is to understand why the method works and how it can be applied in practical mathematical and physical problems.
Additional Comments
This course covers a broad range of topics, but the intention is not to collect unrelated material. The common thread is the use of advanced mathematical methods to understand physical systems.
We start from variational principles and classical mechanics, then move toward tensors, geometry, transforms, complex analysis, and finally some ideas that point toward quantum mechanics and quantum field theory.
Several examples are included throughout the course, such as the double pendulum, geodesics, strain tensors, Fourier transform applications, and other problems from physics and engineering. These examples are meant to make the abstract theory more concrete and to show how the same mathematical ideas appear in different contexts.
Some topics, such as Einstein’s field equations, Poisson brackets, the Maupertuis principle, and residue calculus, are treated in more detail because they are especially important for building a deeper understanding of theoretical physics.
Who Should Enroll
This course is suitable for:
Advanced undergraduate and graduate students in mathematics, physics, and engineering.
Professionals and researchers who want to strengthen their understanding of advanced mathematical methods.
Students interested in the mathematical foundations of classical mechanics, relativity, quantum mechanics, and field theory.
Anyone with a strong background in calculus, linear algebra, and differential equations who wants to study these topics in a connected and structured way.
Course Features
The course includes theoretical explanations, step-by-step derivations, worked examples, and selected applications.
Whenever possible, I try to make the lectures self-contained, so that students can follow the logic of each section without constantly needing to consult external material.
The course is also designed so that students may skip some sections or focus only on the topics that are most relevant to their own studies. For example, someone interested mainly in tensors and relativity may follow those sections directly, while another student may focus more on integral transforms, complex analysis, or path integrals.
Prerequisites
A solid understanding of undergraduate calculus, linear algebra, and differential equations is strongly recommended.
Some familiarity with classical mechanics and basic physics is helpful, especially for the sections involving variational principles, Hamiltonian mechanics, tensors, and quantum physics. However, I try to introduce the main ideas gradually and with enough context to make the material accessible to motivated students.
Note on Course Structure and Overlap
Part of the material in this course also serves as supplementary mathematical background for some of my other physics courses.
Some overlap may therefore exist between this course and those physics courses. However, the purpose here is different. In this course, the mathematical ideas are collected, organized, and developed in a more systematic way (well, this is my desire, although it is not always easy to do...), so that students can study them independently from the specific physical applications.
In other words, this course is meant to help students build a stronger mathematical foundation, while the physics courses use some of these tools in more specific physical contexts.
New Material
New material was added on 30 November 2024.
The new sections include topics such as the Lorentz group, Lie algebras, spinors, Pauli matrices, Dirac matrices, operators, and related concepts. These additions expand the connection between tensors, relativity, and quantum physics.
References
This course reflects my own way of organizing and presenting the material, with the aim of giving students a clear and logical path through several important areas of advanced mathematics and theoretical physics.
Some of the material was inspired by the following sources:
L. Landau and E. Lifshitz, Mechanics, Vol. 1
L. Landau and E. Lifshitz, The Classical Theory of Fields, Vol. 2
A. Einstein, The Foundation of the General Theory of Relativity, 1916
A. Einstein, Hamilton’s Principle and the General Theory of Relativity, 1916
A. Einstein, Cosmological Considerations on the General Theory of Relativity, 1917
B. A. Dubrovin, A. T. Fomenko, S. P. Novikov, Modern Geometry — Methods and Applications, Part 1
L. Landau and E. Lifshitz, Theory of Elasticity, Vol. 7
L. S. Schulman, Techniques and Applications of Path Integration
D. Tong, Quantum Field Theory, lecture notes, University of Cambridge
D. Skinner, Quantum Field Theory II, lecture notes, University of Cambridge