

Study with the several resources on Docsity
Earn points by helping other students or get them with a premium plan
Prepare for your exams
Study with the several resources on Docsity
Earn points to download
Earn points by helping other students or get them with a premium plan
Community
Ask the community for help and clear up your study doubts
Discover the best universities in your country according to Docsity users
Free resources
Download our free guides on studying techniques, anxiety management strategies, and thesis advice from Docsity tutors
mathematical_physics_2007_6.pdf
Typology: Study Guides, Projects, Research
1 / 3
This page cannot be seen from the preview
Don't miss anything!
This chapter presents a quick review of vector and matrix algebra. The intent is not to cover these topics completely, but rather use them to introduce subscript notation and the Einstein summation convention. These tools simplify the often complicated manipulations of linear algebra.
Standard, consistent notation is a very important habit to form in mathematics. Good notation not only facilitatescalculationsbut, like dimensionalanalysis, helps to catch and correct errors. Thus, we begin by summarizing the notational conventions that
TABLE 1.1. Notational Conventions Symbol Quantity a A real number A complex number A vector component A matrix or tensor element An entire matrix A vector @, A basis vector T A tensor
1
2 A R E W W OF VECTOR AND MATRIX ALGEBRA
where the components (Vx, V,, V,) are called the Cartesian components of and (ex.e,, $) are the basis vectors of the coordinate system. This notation can be made more efficient by using subscript notation, which replaces the letters ( x , y, z ) with the numbers ( 1 , 2 , 3 ). That is, we define:
Equation 1.1 becomes
or more succinctly,
i= 1,2,
Figure 1.1 shows this notational modification on a typical Cartesian coordinate sys- tem. Although subscript notation can be used in many different types of coordinate systems, in this chapter we limit our discussion to Cartesian systems. Cartesian basis vectors are orthonormal and position independent. Orthonoml means the
Position independent means the basis vectors do not change their orientations as we move around in space. Non-Cartesian coordinate systems are covered in detail in Chapter 3. Equation 1. 4 can be compactedeven further by introducingthe Einstein summation convention, which assumes a summation any time a subscript is repeated in the same term. Therefore,
i=1,2,
I I I Y I
Figure 1.1 The Standard Cartesian System