
The Maximum Principle and Some of Its Applications 199
Hence
W
t
= −
1
2
hx, Xxi +
1
2
hW
x
, BR
−1
B
t
W
x
i − hW
x
, Axi. (6.9.18)
The form of Eq. (6.9.18) leads to the conjecture tha t there exists a solution
of the Hamilton-Jacobi equation (6.2.11) of the form
W (t, x) =
1
2
hx, P (t)xi, (6.9.19)
where for each t, P (t) is a symmetric ma trix. Fo r then
W
x
= P x W
t
=
1
2
hx, P
′
(t)xi, (6.9.20)
and for proper choice of P (t) we would have a quadratic form in the left equal
to a quadratic form on the right.
If we assume a solution of the form (6.9.19), substitute (6.9.20) into
(6.9.18), and r ecall that P
t
= P , we get
1
2
hx, P
′
xi = −
1
2
hx, Xxi +
1
2
hx, P BR
−1
B
t
P xi − hx, P Axi. (6.9.21) ...