Before embarking on the formal study of partialdifferential equations (PDEs), it is essential toequip ourselves with background materials frommultivariable calculus, geometry of curves andsurfaces, and ordinary differential equations (ODEs;including total and simultaneous total differentialequations). Selected ideas from earlier mentionedcourses play an important role in the study of PDEs.For the sake of completeness and to make our textself-contained, we briefly discuss the preliminariesas indicated earlier, which are needed in thesubsequent chapters. The approach adopted in thischapter is somewhat different from the one used inthe rest of the chapters. This chapter isdescriptive in nature, wherein the utilisedarguments are intended towards plausibility andunderstanding rather than adopting traditionalrigorous ways. The preliminaries are divided intofive sections.
1.1 Partial Derivatives and AlliedTopics
PDEs involve at least two independent variables.Consequently, the tools of the calculus of severalvariables are instrumentals in PDEs. In thefollowing lines, we recall some relevant notions andterminologies from differential calculus of two andthree variables.
Vectors: An element of Euclidean spaceℝn is ann-tuple of the formx =(x1, x2,…,xn), which is called ann-vector or simply,a vector. The real numbers x1,x2,…,xn are called components ofthis element. The sum and scalar multiplication inℝn aredefined as component-wise sum and component-wisescalar multiplication. The dot product of twoelements x = (x1, x2,…,xn) and y =(y1,y2,…,yn) isdefined as
The norm or length of a vectorx = (x1, x2,…,xn) is defined as
Thus, A vector of length 1 is called a unit vector.
Standard Basis Vectors: The two vectorse1 = (1,0) and e2 =(0, 1) are called standardbasis vectors of ℝ2. Anyvector u = (a, b) ∈ ℝ2 can bewritten as a linear combination of e1 and e2, so that
Similarly, e1= (1, 0, 0), e2 = (0, 1, 0), and e3 = (0, 0, 1)are called standard basisvectors of ℝ3.