10 1. INTRODUCTION
can, locally at least, be transformed into systems of ordinary diﬀerential
equations (ODE), the characteristic equations. We stipulate that once the
problem becomes “only” the question of integrating a system of ODE, it
is in principle solved, sometimes quite explicitly. The derivation of the
characteristic equations given in the text is very simple and does not require
any geometric insights. It is in truth so easy to derive the characteristic
equations that no real purpose is had by dealing with the quasilinear case
We introduce also the Hopf–Lax formula for Hamilton–Jacobi equa-
tions (§3.3) and the Lax–Oleinik formula for scalar conservation laws (§3.4).
(Some knowledge of measure theory is useful here but is not essential.) These
sections provide an early acquaintance with the global theory of these im-
portant nonlinear PDE and so motivate the later Chapters 10 and 11.
Chapter 4 is a grab bag of techniques for explicitly (or kind of explicitly)
solving various linear and nonlinear partial diﬀerential equations, and the
reader should study only whatever seems interesting. The section on the
Fourier transform is, however, essential. The Cauchy–Kovalevskaya Theo-
rem appears at the very end. Although this is basically the only general exis-
tence theorem in the subject, and thus logically should perhaps be regarded
as central, in practice these power series methods are not so prevalent.
PART II: Theory for Linear Partial Diﬀerential Equations
Next we abandon the search for explicit formulas and instead rely on
functional analysis and relatively easy “energy” estimates to prove the ex-
istence of weak solutions to various linear PDE. We investigate also the
uniqueness and regularity of such solutions and deduce various other prop-
Chapter 5 is an introduction to Sobolev spaces, the proper setting for
the study of many linear and nonlinear partial diﬀerential equations via en-
ergy methods. This is a hard chapter, the real worth of which is only later
revealed, and requires some basic knowledge of Lebesgue measure theory.
However, the requirements are not really so great, and the review in Ap-
pendix E should suﬃce. In my opinion there is no particular advantage in
considering only the Sobolev spaces with exponent p = 2, and indeed in-
sisting upon this obscures the two central inequalities, those of Gagliardo–
Nirenberg–Sobolev (§5.6.1) and of Morrey (§5.6.2).
In Chapter 6 we vastly generalize our knowledge of Laplace’s equation to
other second-order elliptic equations. Here we work through a rather com-
plete treatment of existence, uniqueness and regularity theory for solutions,
including the maximum principle, and also a reasonable introduction to the