In control theory , the minimum energy control is the control
u
(
t
)
{\displaystyle u(t)}
that will bring a linear time invariant system to a desired state with a minimum expenditure of energy.
Let the linear time invariant (LTI) system be
x
˙
(
t
)
=
A
x
(
t
)
+
B
u
(
t
)
{\displaystyle {\dot {\mathbf {x} }}(t)=A\mathbf {x} (t)+B\mathbf {u} (t)}
y
(
t
)
=
C
x
(
t
)
+
D
u
(
t
)
{\displaystyle \mathbf {y} (t)=C\mathbf {x} (t)+D\mathbf {u} (t)}
with initial state
x
(
t
0
)
=
x
0
{\displaystyle x(t_{0})=x_{0}}
. One seeks an input
u
(
t
)
{\displaystyle u(t)}
so that the system will be in the state
x
1
{\displaystyle x_{1}}
at time
t
1
{\displaystyle t_{1}}
, and for any other input
u
¯
(
t
)
{\displaystyle {\bar {u}}(t)}
, which also drives the system from
x
0
{\displaystyle x_{0}}
to
x
1
{\displaystyle x_{1}}
at time
t
1
{\displaystyle t_{1}}
, the energy expenditure would be larger, i.e.,
∫
t
0
t
1
u
¯
∗
(
t
)
u
¯
(
t
)
d
t
≥
∫
t
0
t
1
u
∗
(
t
)
u
(
t
)
d
t
.
{\displaystyle \int _{t_{0}}^{t_{1}}{\bar {u}}^{*}(t){\bar {u}}(t)dt\ \geq \ \int _{t_{0}}^{t_{1}}u^{*}(t)u(t)dt.}
To choose this input, first compute the controllability Gramian
W
c
(
t
)
=
∫
t
0
t
e
A
(
t
−
τ
)
B
B
∗
e
A
∗
(
t
−
τ
)
d
τ
.
{\displaystyle W_{c}(t)=\int _{t_{0}}^{t}e^{A(t-\tau )}BB^{*}e^{A^{*}(t-\tau )}d\tau .}
Assuming
W
c
{\displaystyle W_{c}}
is nonsingular (if and only if the system is controllable), the minimum energy control is then
u
(
t
)
=
−
B
∗
e
A
∗
(
t
1
−
t
)
W
c
−
1
(
t
1
)
[
e
A
(
t
1
−
t
0
)
x
0
−
x
1
]
.
{\displaystyle u(t)=-B^{*}e^{A^{*}(t_{1}-t)}W_{c}^{-1}(t_{1}).}
Substitution into the solution
x
(
t
)
=
e
A
(
t
−
t
0
)
x
0
+
∫
t
0
t
e
A
(
t
−
τ
)
B
u
(
τ
)
d
τ
{\displaystyle x(t)=e^{A(t-t_{0})}x_{0}+\int _{t_{0}}^{t}e^{A(t-\tau )}Bu(\tau )d\tau }
verifies the achievement of state
x
1
{\displaystyle x_{1}}
at
t
1
{\displaystyle t_{1}}
.
See also
Category :
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