1/4 y/x =12 and -1/y 2/x=6 form the given determinants, form the two simultaneous equations in x and y and solve them.
Answers
6.1 Introduction to Eigenvalues
Linear equations Ax D b come from steady state problems. Eigenvalues have their greatest
importance in dynamic problems. The solution of du=dt D Au is changing with time—
growing or decaying or oscillating. We can’t find it by elimination. This chapter enters a
new part of linear algebra, based on Ax D -
x. All matrices in this chapter are square.
A good model comes from the powers A; A2; A3;::: of a matrix. Suppose you need the
hundredth power A100. The starting matrix A becomes unrecognizable after a few steps,
and A100 is very close to Œ :6 :6I :4 :4 :
-
:8 :3
:2 :7 -
:70 :45
:30 :55 -
:650 :525
:350 :475
-
-
-
-
:6000 :6000
:4000 :4000
A A2 A3 A100
A100 was found by using the eigenvalues of A, not by multiplying 100 matrices. Those
eigenvalues (here they are 1 and 1=2) are a new way to see into the heart of a matrix.
To explain eigenvalues, we first explain eigenvectors. Almost all vectors change di-
rection, when they are multiplied by A. Certain exceptional vectors x are in the same
direction as Ax. Those are the “eigenvectors”. Multiply an eigenvector by A, and the
vector Ax is a number -
times the original x.
The basic equation is Ax D -
x. The number -
is an eigenvalue of A.
The eigenvalue -
tells whether the special vector x is stretched or shrunk or reversed or left
unchanged—when it is multiplied by A. We may find -
D 2 or 1
2 or 1 or 1. The eigen-
value -
could be zero! Then Ax D 0x means that this eigenvector x is in the nullspace.
If A is the identity matrix, every vector has Ax D x. All vectors are eigenvectors of I .
All eigenvalues “lambda” are -
D 1. This is unusual to say the least. Most 2 by 2 matrices
have two eigenvector directions and two eigenvalues. We will show that det.A -
I / D 0.
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