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A First Course in Linear Algebra, 2017a

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386 Spectral Theory<br />

7.3.5 The Matrix Exponential<br />

The goal of this section is to use the concept of the matrix exponential to solve first order l<strong>in</strong>ear differential<br />

equations. We beg<strong>in</strong> by prov<strong>in</strong>g the matrix exponential.<br />

Suppose A is a diagonalizable matrix. Then the matrix exponential,writtene A , can be easily def<strong>in</strong>ed.<br />

Recall that if D is a diagonal matrix, then<br />

P −1 AP = D<br />

D is of the form<br />

and it follows that<br />

⎡<br />

⎢<br />

⎣<br />

D m =<br />

⎤<br />

λ 1 0<br />

. ..<br />

⎥<br />

⎦ (7.5)<br />

0 λ n<br />

⎡<br />

⎢<br />

⎣<br />

λ m 1<br />

0<br />

. ..<br />

0 λ m n<br />

⎤<br />

⎥<br />

⎦<br />

S<strong>in</strong>ce A is diagonalizable,<br />

and<br />

Recall why this is true.<br />

and so<br />

A = PDP −1<br />

A m = PD m P −1<br />

A = PDP −1<br />

{<br />

m times<br />

}} {<br />

A m = PDP −1 PDP −1 PDP −1 ···PDP −1<br />

= PD m P −1<br />

We now will exam<strong>in</strong>e what is meant by the matrix exponental e A . Beg<strong>in</strong> by formally writ<strong>in</strong>g the<br />

follow<strong>in</strong>g power series for e A :<br />

)<br />

e A D k<br />

=<br />

P −1<br />

k!<br />

(<br />

∞<br />

A<br />

∑<br />

k ∞<br />

k=0<br />

k! = PD<br />

∑ k P ∞∑ −1<br />

= P<br />

k=0<br />

k!<br />

k=0<br />

If D is given above <strong>in</strong> 7.5, the above sum is of the form<br />

⎛ ⎡<br />

1<br />

∞ k!<br />

⎜ ⎢<br />

λ 1 k 0<br />

P⎝∑<br />

⎣<br />

. ..<br />

k=0<br />

0<br />

This can be rearranged as follows:<br />

⎡<br />

e A ⎢<br />

= P⎣<br />

1<br />

k! λ k n<br />

∑ ∞ k=0 1 k! λ k 1<br />

0<br />

. ..<br />

⎤⎞<br />

⎥⎟<br />

⎦<br />

⎠P −1<br />

0 ∑ ∞ k=0 1 k! λ k n<br />

⎤<br />

⎥<br />

⎦P −1

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