
Examples 269
dλ
5
dt
= −H
rν
= λ
3
(t)
Z
Ω
cz
2
ν
2
cos z
1
dµ
t
+ λ
4
(t)
Z
Ω
cz
2
ν
2
sin z
1
dµ
t
.
Hence
λ
1
(t) = a
1
λ
2
(t) = a
2
for all t in [0, t
1
] (8.7.6)
λ
3
(t) = −a
1
t + a
3
λ
4
(t) = −a
2
t + a
4
for consta nts a
1
, a
2
, a
3
, a
4
.
Since the initial point is fixe d and the terminal set J
∞
is given by (8.7.3),
the transversality condition (6.3.24) gives that the n + 1 vector (−H
r
(π(t
1
)),
λ(t
1
)) is orthogonal to J
∞
at (t
1
, x(t
1
), y(t
1
), p(t
1
), q(t
1
), m(t
1
)). From (8.7.3)
we get that the vectors (dσ
0
, dσ
3
, dσ
4
, dσ
5
) of the form (1, 0, 0, 0), (0, 1, 0, 0),
(0, 0, 1, 0), and (0, 0, 0, 1) are a basis to the tangent space to J
1
at (t
1
, x(t
1
),
y(t
1
), p(t
1
), q(t
1
), m(t
1
)). Thus,
H(π(t
1
)) = 0 λ
3
(t
1
) = λ