Browsing by Subject "Sobolev spaces"
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(2020)This thesis introduces the theory of conformal welding and shows that every quasisymmetric function is a welding homeomorphism. Conformal weldings appear naturally in Teichmüller theory when we consider the conditions under which two Riemann surfaces can be joined together. In the second chapter we investigate the properties of quasisymmetric and quasiconformal functions and derive various inequalities for them. Later in the chapter we define the socalled BeurlinAhlfors extension to quasisymmetric functions and show that this function is in fact quasiconformal. In the third chapter, we begin by introducing the fundamentals of Sobolev spaces and present some theorems that allow us to study the properties of compositions of quasiconformal functions. We prove Stoilow's factorization theorem and use it to show that the solution to Beltrami's equation can naturally be normalized so that the solution is unique. Using Stoilow's factorization and a few other lemmas and theorems we derived earlier, we finally show the main result of the thesis that is, we show that every quasisymmetric function is a welding homeomorphism. In the last chapter, we answer the question of whether perhaps all increasing homeomorphisms are welding homeomorphisms. The answer is no and this is shown by the counterexample invented by Bishop.

(2021)Maxwell’s equations are a set of equations which describe how electromagnetic fields behave in a medium or in a vacuum. This means that they can be studied from the perspective of partial differential equations as different kinds of initial value problems and boundary value problems. Because often in physically relevant situations the media are not regular or there can be irregular sources such as point sources, it’s not always meaningful to study Maxwell’s equations with the intention of finding a direct solution to the problem. Instead in these cases it’s useful to study them from the perspective of weak solutions, making the problem easier to study. This thesis studies Maxwell’s equations from the perspective of weak solutions. To help understand later chapters, the thesis first introduces theory related to Hilbert spaces, weak derivates and Sobolev spaces. Understanding curl, divergence, gradient and their properties is important for understanding the topic because the thesis utilises several different Sobolev spaces which satisfy different kinds of geometrical conditions. After going through the background theory, the thesis introduces Maxwell’s equations in section 2.3. Maxwell’s equations are described in both differential form and timeharmonic differential forms as both are used in the thesis. Static problems related to Maxwell’s equations are studied in Chapter 3. In static problems the charge and current densities are stationary in time. If the electric field and magnetic field are assumed to have finite energy, it follows that the studied problem has a unique solution. The thesis demonstrates conditions on what kind of form the electric and magnetic fields must have to satisfy the conditions of the problem. In particular it’s noted that the electromagnetic field decomposes into two parts, out of which only one arises from the electric and magnetic potential. Maxwell’s equations are also studied with the methods from spectral theory in Chapter 4. First the thesis introduces and defines a few concepts from spectral theory such as spectrums, resolvent sets and eigenvalues. After this, the thesis studies nonstatic problems related to Maxwell’s equations by utilising their timeharmonic forms. In timeharmonic forms the Maxwell’s equations do not depend on time but instead on frequencies, effectively simplifying the problem by eliminating the time dependency. It turns out that the natural frequencies which solve the spectral problem we study belong to the spectrum of Maxwell’s operator iA . Because the spectrum is proved to be discrete, the set of eigensolutions is also discrete. This gives the solution to the problem as the natural frequency solving the problem has a corresponding eigenvector with finite energy. However, this method does not give an efficient way of finding the explicit form of the solution.
Now showing items 12 of 2