Begin2.DVI

(Ben Green) #1
Express f(A)as a linear combination of the matrices {I, A, A^2 }and write

f(A) = R(A) = sin At =c 0 I+c 1 A+c 2 A^2 ,

where c 0 , c 1 and c 2 are functions of tto be determined. Since there is a repeated root,

use differentiation and write the equations

R(x) = c 0 +c 1 x+c 2 x^2
R′(x) = c 1 + 2c 2 x

to obtain the system of equations

R(λ 1 ) = f(λ 1 ) = sin t=c 0 +c 1 +c 2
R′(λ 1 ) = f′(λ 1 ) = cos t=c 1 + 2 c 2

R(λ 3 ) = f(λ 3 ) = −sin t=c 0 −c 1 +c 2

(10 .49)

These are three independent equations which can be used to solve for the coefficients

c 0 , c 1 and c 2 .Solving these equations for c 0 , c 1 and c 2 one finds

c 0 =^1
2

(sin t−cos t), c 1 = sin t, c 2 =^1
2

(cos t−sin t)

and consequently the matrix function sin At has the representation

sin At =

(
sin t−cos t
2

)
I+Asin t+

1
2 (cos t−sin t)A

(^2).


An alternate form for this result is the matrix form

sin At =^1
2



0 2 sin t cos t−sin t
cos t+ sin t cos t−sin t cos t+ sin t
2 cos t 2 cos t cos t+ sin t


 A=



0 1 0
1 0 1
1 1 1



Four-terminal Networks


Consider the electrical networks illustrated in figure 10-6. No matter how com-

plicated the circuit inside the boxes, there are only two input and two output termi-

nals. Such devices are called four terminal networks and are represented by a box

like those illustrated in figure 10-6, where the quantities Z, Z 1 ,and Z 2 are called

impedances. Impedances Z are used in alternating current (a.c.) circuits and are

analogous to the resistance Ruse in direct current (d.c.) circuits.
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