STEP RESPONSES -
.
7
unit
the first
Let's function
ander
of transfer
step
see response a : fix
G the
Let's
model)
(accumulatore
known integrator
GIS) the
M/s system
as
= .
unit %
the t Y
input Step
step M/s
u(t) (t) namp(t)
(S) M/sa <y(t)
S M
as . =
= = = .
.
. .
initial
study final
and value
the
We can : ya
(ndegz1
G then strictly
(5)
(0 ) system (
+
y preopen
0
=
= him positive fore
y (0 t-
SG(s)
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) of
M M
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S st
+
+ 0
lim
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G(s) o
7 sign
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on
= M
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YIS) the
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then get time
and
Ms
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we = -
st
IST
danain m[1-expl-t/ )] step
y(H) Values
(t) .
+ :
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co
Ya
linh(s) Indegu
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y =
= limshis) positive
MIT sop
y(07) per
=
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lit blows fer
it
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(0) Tso
Y up
M
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t concluded
transient [SETTLINGTIME)
attere the phase
5T
47
os can
: we
= Mi-T/T)
=
↑
e the
③ and
Ms
Y
have in
4(s) we = -
= 1/T
s +
M[1 T
domain exp(-te)]
time
the y(t) Values
Step (t)
- :
= . Ya
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lin immediate
(0 his)
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+ ( ⑧
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y response
-
=
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s[MIT)
l()) T
tim OLT <
o
(ot)
↑ = = =
S +
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>
I
O -
him ST
o 0
= if value
initial with
the
connect
we
I TO
G(0)
(8) STATIC GAIN
M
y = stope
get
= the
the (T
point M) we
. pdes/zenos term
by
the transient
then contribute the white
phase
to
only
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given
is
g 0
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behavioure time
the needed
characterized IST
to transient
asymptotic The Ts)
is .
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by
determined pdes transient
the depends
the
white the
initial the
of
part (St o)
is Zeros
on + :
if have initial
effect undershoot (the
white
it has anticipator
>0 to we response
an
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first the value)
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starts
it
reapidly)
drops then T
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an .
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have
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al) Y(S) = and
↑ M
we
= = .
damain
the time Values
#exp1
y(t) )
in + / ya
:
+
= · uoudenchoot
response
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tim (1)
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Sim stsYs) t
PI · >
10
i )
+ - T
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= final
initial value
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connecting at
the
17
G(0)
y(x) T30
0 initial stope
the
t get
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if the of
end the
at
the the
the transient
then step
origin
in
is
os zero is
response 0
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second-order
of
switch to
Let's systems
examples
same :
M
⑤ distinct
two then
like with
poles and G(s) Ti
Tz
temos O
>
no = (1 ) STz)
(1
ST
+ +
i
M (MF
-
Y(s) = (PI
2)/(s 1/TC)
)/(s
/T ) +
+
·
= - -
.
(1 +
) sta)
(
ST T
+ + .
=
. - I expl-/Tc)Jstepit
M[1-l- (since the
and e
y(t) exp1-tT ) system
.
= Initial
exp) final
two
have of
the
ander values
second sommation and
is we
a one :
. fact
fast guides
dynamics 5T
limh(s) =
Indeg
(0+) 0
y =
= effect)
lif Tic Tz
> no
n
Y
Hat)
Starts
(response
(ndeg 2)
(0t)
y d
0 =
= M
=.. - -
line if
yj(0 MITIT2
524(s)
)
+ ps
=
= s + + o ⑧ to it
final value
(5) G(x)
y M /
=
= in t
only
10)
y <
0
0 =
= the slowest Clargest
constant
figure
matters the night
at
to term
what time time
is
It's vietul to compute
constant) the this
orle max(TI in
Tz) 5T
5
Ts
is case
.
=
: ..
; =
local
y(t) and the maximum/minimum
compute
0
= .
fasten approximate
first
than the
second pole the
it (TICLT2)
the then
much
is
oss can
one we
behaviour the fast)
of first
with (initial imentia
onder System is very
a
one .
M(1 ST)
⑥ distinct like
two +
poles and then
G(s) and
zero
one = )(1
(1 STz)
ST
+ +
,
= [])
-
have =
YIS) IPI)12 4/Th)
we 17 ) +
+
- -
.
Texpl-/Tc) Jstepit)
M[1-lexp1-t/Ti)
and Values
y(t) -
= . stationary points
yn O
him Irdeg Ti
e
(0 = G11)
)
y 0 t
=
= MIT
y(0 )
+ =
=... to st
y(5) M
=... =
it the .
Stationary then
t (t)
points
compute The
plot
.
make
S can
we a
we
0
. =
initial to
compared
the
accelerates behavioure
of the
adding
effect previous
zero case
a .
=
⑦ (0)
tw then e e
like have
(SMS
pos his)
0)
h
+ we
my =
M 5 m
YIS) mi-clut]stes
function and
Ms ylt)
.
= =
13 =
-
1 + Wi
Initial final values
and Ya 5/
: ST Zwn =+ o
=
Y
limh(s) ⑧
~
Inde 1 1
(04)
y 0
=
= Indeg 2)
y(0 + ) 0 =
=... = ⑧
io Mrn
+ ) ↓
↓
=... = =
period ocillation
of T
F = oscillation
linfinite
7) (
* ...
↓ but
because
the IRelp)
theoum (daba)
IRe(p)
final have
value
cannot co
we
use o
we no =
1 -
⑧ poes have Y
of complex then
↑1
G(s)
paine we )5
= +
3
+ +
2
(1 +
wegis
Stun W time
the
= the
domain got
and in
↑ we
- zwn)
(stzwul" wa
+ +
+ 3
M[e-e-Sant)-coslut) sin(it))]Step Initial final
function values
and
(t)
y(t) + :
.
= 32
1 - damped
a oscillations
y
lin 6(s) Indez
10 )
+
y 0
=
= i
y(0 Indeg 2)
)
+ 0 =
=
=...
yj(ot) MW
=... = ⑧ > t
g PJEDO-Period
im final value it
7(s) only
his) M
= 2/weit/we
= =
time fastest
the the
settling exponential the
that
term to
part 0
is gas so we can
: and of
number
compute 5/5wn
exp1-5Ts) 5/-1Re(p)
expl-Junt)
impose Ts The
= = = ·
pseudo-periods /
-
N Ts /
is .
see
we +
= -
D M
⑨ it function
consider but with
the same
we :
3
3 ant)
m[ M
sin (wt))]Step (t)
y(7) (s(wt)
- +
e
- -
= 32
1 - but
the value
initial derivative
still have and
same
we > t
exponential diverging
envelope blows
the Toscillation up)
is diverging scillations
-
GIS)
TIME/GAIN
RESPONSES FOR
OBSERVATIONS STEP
ON behavior M
(steadystate)
represents
static the
G(0) static g =
We
gain
Ms
= can
· .
Possible
final theorem
value results 0
the box
with
it the ga
compute in
are
. : gia
amplification S
basically factor between atput
the and
It steady state.
input in
is stability
stability
about (
(IRe(p)
tell information asymptatic
615)
of
poles us < 0
· by lendogenous
poles phenomenon) when
oscillations complex
step E20
given
in 7
response are
· .
the of (TS
rulated position
to
settling poes
time for
the (Ti) real poles on
is Smax
· =
(1/
Ts poles)
for
) just complex
5 max (IRe(P)
(Ti " iwni)
To
= . 5 max
5
:
wn max
;
, =
= . ,
the
anticipate time
if (acullerated
constant
the
zeros can response <=>
Tso zo
· delaying
initial the it Idelayed
response) have initial
zo
iso
an =>
response we
of If
the large
and if
ovenshoot
have
system) enough
is
response I io
is 0 on
we an
. 0)
assumed
for undershoot example
value (in above
of get the Ma
we
T
every we an BLOCK DIAGRAMS-
8 . ↓ d
Let's components
several
have of system each
assume a
we , ya
by function
described want
trausten Y
to
61s) We 21 52
one a > -
>
-
. -
describe of
the need
autput System We
LTI
response a :
. M
① G(s)U(s)
t Y (1)
BLOCK Y(S)
V(s)
S G(s)
= >
. >
-
. - ① Y(1)
Vill)
② =U Uz
t (1)
Y(S) >
(s)
SUMMATION >
=
NODES S -
-
,
=
. . # VIS
combine signals)
to
ander
( them in
use
we Y (s)
Vi(S) >
③ ,
Y
t
BRANCHING V
(S) Y2(s) (s)
NODE S = i
.
.
. Do
, boxes
distributes
Cit the multiple
signal to Yz(s)
same < -
function
figure
to 4
transfer
the all
need also rules system
at
We aver . St >
-
basic diagrams
Let's configurations (asculare)
block
for siso
see T
: VISI
① VIS)
have
St
CASCADED CONNECTION We an
. H(s)
G(s) Y(S)
<
> >
intermediate variable GIS)V(S)
VIS) and
= ⑭
variable
atput (G
H U)
H(s)
Y(S) V(S)
an . .
=
= U(s) YISS
1 (HG)U
(4U) HisS
G(6)
only)
for
H We
SISO > >
= can nunge
= .
·
black computing
the into ((5) H(S)
system one . Vils) Y (S)
,
4())
>
V(s)
② t have Vi()
((S)
PARALLELED CONNECTION S We Y(S)
=
= <
. . 30
and simplify
Y(s)
Uc(s) [ Y2
=Y We
(5)
(s) can
=> = , · Yz/s)
H(S)
>
and write (EGIH)U (summing
Y(s) GU HUz
= Uz
. (s)
= ⑭
the functions)
transfer V(1) Y(s)
IG(1) [H(S)
< <
③ VIS)
the VIS)
t compute
FEEDBACK CONNECTION S We can Y(S)
4())0
. . 10 >
<
⑦
functions N
Y(S) G(S) and
WIS)
VIS) HISSY(S)
= =
, H(s) <
by
simplify writing
VIS) [U(s) We WIS
#WIS) can
= . G(s)(U() ⑭
#HISSYISS)
U(S)
VIS) [ H(s) Y (S)
Y(s) <
= = 41)
limplicitegration Y(S) Gis
Y1)
in VISI
< = > Yi
G(S)H(S)
1 = 61/His)
1
U(s) = /
G(S) the
where TRANSFER
LOOP FUNCTION
is
G(S)H(S)
1 =
It's of
examples DIAGRAMS
COMPLEX
see some : VIS) Y(1)
① Als) B(S)03
the <
diagram >
· <
reduce
Let's <
system
siso &
. by
to recognising
simplem patterns
a one > ?
that know
we : C(S)
function
transfer
with 1
block
like a
UIS) U(S)
e Be
>
then 1
+
AB Y(s)
final following
and result the
the 1
VIS
is + <
>
: BC
1 + Vis
↓
VIS
② that the
know
systems for
We systems
MISO LTI 4
tut
100
co
.
superposition applies consider
(we
principle on
time)
at
input B(S)
a : <
Y(s)
Als) o
30 >
< A
V(x) V(s)
0 *
0
+ Y(S)
VIS E
= was >
, AB
1 +
By VIS)
Vis
↓ ·
Bus
VK) Vk) > j
0 cos e
0
n
= , E
by VIS
final
draw the the
system combining single A
we can >
transfer functions above
computed AB
each
in in
case 1
a Y
+
summation node : VIS) ~
Ab
there to single
possibility compute
oss is a
no ABU +
between
function two
transtin (they
the inputs VIS
Y(S) = AB
+
for
different units
have
cold instance) SHALT
THE
.
FOR SYSTEMS
TRANSFER FAB
SUM FUNCTIONS +
THE MISO
NOT Y(s) AB)
1 WIS)
+
. =
NOOO
8 dumb to the
salve
system The
SIMO way
. Y (S)
< ,
it
simplify
to following
the
system is in
Ismant
atput time
at is
way
one a
way UI) BIss
Als) Yels)
< >
<
>@ o
considering Y)
B
Yz :
.
= ⑦
V(S) Y (S)
Als)
g >
> oc .
just Y A
LS) O
, <Y(s)
E UIs) < AB
1 +
BISS A Y (s)
S < ,
AB AB
1
Y2(S)
simularly
just VIS
Yzis) +
compute U(I)
we = 30
final fellowing
the
write the results
St in AB
can
we way :
. Yels)
S c
AB
1 +
VIS)
that w(s)
Odd
⑪ sove the
with
cannot roles z(s)
cases we Y(s)
//2 BIS)
All) <
& <
0
In always
these
know apply VISI
cases can
we we
. ②
the mathematical t
operations S :
. R(S) V
Os C(s) <
S(S)
S(s) W(s)
R(s)
A(s) VIS)
N(s) +
=
= (1) [Ar CY]
Y
BISSWIs) BAV
VIS) -R(s) U
V
VIS)
z(s) AND +
+ <
= =
=
=
S(s) ((s) (s)
z (1
A(s) V (s)
( B(s)((s))
V(s) 1) U(S)
+
= < +
-
=
final
lineare
solving figure
equations
the solution
of the
compute simplem
at
system We
we can a
can
.
branch solution
loops
feedback sequencially the
break
if write
the in using
we can
way one
we
: brooken loop
for
tearing (2
be .
(to explicitly) equation
expressed system)
variable VIS) every
a BLOCK STABILITY
AND
DIAGRAMS -
9
. block diagram
two-system
have
Let's where
assume a
we Biss
Ull) Als) <
<
di(s)
da Knowing that
and nB(s)
na(c) (1) Y(S)
co-prime
are
,
, . ⑭
asymptetically what
stable about
and BIS)
Als) say
can we
are <MA UB
VIS) YIS)
.
of
the stability the <
CASCADED CONNECTION : da dB
MASSUBS
Y/S)
let's Als)BLS(VII) possible
compute VIEISV) cas.
= =
① (pdes <poes Gl5
WApdes of
B(s))
co-price) of
all
cancellations of
di
(da Acs)]
no na uo :
i =
, , stable
asymptatically
of
poles the
of
also and
then the system
GIS)
set initial
is so .
asymptatically
asymptatically stable
Gls)
stable
A B
We >
say
can : , .
Al30ypdes of
Clpdes
② (pds BISS)
of his)]
cancellation
there t of of
kind 415)
in
is S
same . . asymptatically
asymptatically stable (E).
stable Gls)
A B
We =>
say
can : ,
I consider
instead PARALLELED A(S)
CONNECTION >
a ↓
we : S
U(s)
Bud
T ↳
=
1A
B(s)
=A(s)
4(s) = =
= B(S)
>
of
the the
possible the previous so
cases same ⑭
we
are ore
that BOTH PARALLELED CONNECTION
CASCADED AND VIl
say
can Y(s)
G(s)
> <
rustable
can't
PRESERVE (we make
STABILITY
ASYMDICTIC an
by
component .
it with
stable component)
connecting As
an
I consider >Y (S)
FEEDBACK-LOOP CONNECTION U() <Als)
we a >
: o
⑦
dB(s)
na(s)
na/da
FAB
4()) (InB)
= B(S)
dakdBIs) Funksul
1 ⑭
da(s)dg(s) the
known
nals)np/s)
where XIS) VIl
is
= as
= Y(s)
G(s)
> <
Possible
fed-back
polynoncial of the
characteristic cases
. : Im a
correlation
there betw
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