Biomedical Engineering Reference
In-Depth Information
7.4.2
Power-Law Deceleration
This law has the form
⎧
⎨
1
1
/(
1
−
β)
A
t
β
−
β
−
if 0
≤
t
≤
t
∗
=
,
u
=
A
(7.62)
⎩
0
if
t > t
∗
,
where
A
and
β
are parameters,
A >
0and
β<
1 [for
β
≥
1 the right-hand
side of Eq. (7.62) has a nonintegrable singularity at
t
0]. When subjected
to the control of Eq. (7.62), the object decelerates from the initial velocity
v
0
=
=
1 to a complete stop at the time instant
t
∗
in the position
β)
(
2
−
β)/(
1
−
β)
A
1
/(
1
−
β)
(
2
(
1
−
J
1
=
x(t
∗
)
=
.
(7.63)
−
β)
The parameters
A
and
β
should be determined to minimize the quantity of
J
1
of Eq. (7.63) under the constraint
J
2
1.
Substituting the control of Eq. (7.62) into the right-hand side of Eq. (7.9)
and calculating the maximum of the expression in the curly brackets with
respect to
t
1
and
t
2
(0
≤
≤
−
≤
t
2
t
1
)give
⎧
⎨
2
.
5
1
1
/(
1
−
β)
A
−
β
1
−
2
.
5
β
if
≤
,
1
−
β
A
=
J
2
(7.64)
1
.
5
/(
1
−
β)
if
>
1
1
/(
1
−
β)
⎩
−
A
β
1
−
β
A
for
2
β
≤
5
.
(7.65)
for
β >
5
.
To find the minimum of the function
J
1
of Eq. (7.63) with respect to
A
and
β
under the constraints
A
It can be shown that
J
2
=∞
2
≥
≤
5
,and
J
2
<
1, where
J
2
is
defined by Eq. (7.64), first calculate the minimum with respect to
A
for
fixed
β
.Since
J
1
decreases whereas
J
2
increases as
A
increases, the desired
minimum is attained when
J
2
0,
β
=
1. In accordance with Eq. (7.64),
⎨
β)
(
2
.
5
β
−
1
)/
2
.
5
(
1
−
if
<
1
,
A
=
(7.66)
⎩
A
=
1
−
β
if
≥
1
,
⎧
⎨
⎩
−
β
1
β
(
1
−
2
.
5
β)/
[2
.
5
(
1
−
β)
]
if
<
1
,
2
−
J
1
=
(7.67)
1
−
β
if
≥
1
.
2
−
β
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