6.002 CIRCUITS ANDELECTRONICS Incremental Analysis... Nonlinear AnalysisX Analytical method X Graphical method Today X Incremental analysis Reading: Section 4.5 Review... total variable
Trang 16.002 CIRCUITS AND
ELECTRONICS
Incremental Analysis
Trang 2Nonlinear Analysis
X Analytical method
X Graphical method
Today
X Incremental analysis
Reading: Section 4.5
Review
Trang 3Method 3: Incremental Analysis
Motivation: music over a light beam
Can we pull this off?
LED: Light Emitting expoDweep ☺
D
v
+
-)
(t
v I +–
D
i
LED
R
i
AMP
light intensity I R
in photoreceiver
R
R I
light intensity
D
D i
I
v
t
music signal
)
(t
v I i D (t) light i R (t) sound
nonlinear
linear
Trang 4The LED is nonlinear distortion
I
D v
v = v D
D
i
D
D
i
t
Trang 5D
v
D
i
D
I
D
V
DC offset
or DC bias
Trick:
d D
D I i
i = +
I
V
D
v
+
-) (t
v i +–
LED
+ –
I
v
d D
v = +
I
small region looks linear
(about V D , I D)
Trang 6very small
D
i
D
v
d
i
D
I
D
V
Trang 7t
D
v
D
V
I
D v
t
D
I
D
i
~linear!
Demo
d v
d
i
D
i
Trang 8total variable offsetDC superimposedsmall
signal
The incremental method:
(or small signal method)
1 Operate at some DC offset
or bias point V D , I D
2 Superimpose small signal v d
(music) on top of V D
3 Response i d to small signal v d
is approximately linear
Notation:
d
D
D I i
i = +
Trang 9( )D
D f v
What does this mean
mathematically?
Or, why is the small signal response linear?
We replaced
D D
using Taylor’s Expansion to expand
f(v D ) near v D =V D :
V v D
D D
dv
v
df V
f i
D D
∆
⋅ +
=
=
) (
"
+
∆
⋅
+
=
2 2
2 ( )
! 2
1
D V
v D
dv
v f d
D D
large DC
increment
about V D
nonlinear
d v
neglect higher order terms because is small∆v D
Trang 10( ) D
V v D
D D
v d
v f
d V
f i
D D
∆
⋅ +
≈
=
) (
equating DC and time-varying parts,
D V
v D
D
v d
v f
d i
D D
∆
⋅
=
∆
=
) (
constant
w.r.t ∆v D constant w.r.t ∆v slope at V D , I D D
( )D
D f V
constant w.r.t ∆v D
X :
We can write
V v D
D D
D
v d
v f
d V
f i
I
D D
∆
⋅ +
≈
∆
+
=
) (
Trang 11Equate DC and incremental terms,
D
bv
D a e
i =
From X :
constant
In our example,
d
bV
bV d
I + ≈ D + D ⋅ ⋅
D
bV
I =
d
bV
d a e b v
i = D ⋅ ⋅
operating point
d D
d I b v
behavior linear!
aka bias pt
aka DC offset
Trang 12bV
D a e
d D
d I b v
i = ⋅ ⋅
D
v
D
i
D
I
D
V
slope at
V D , I D
operating point
we are approximating
A
B
d v
d i
Graphical interpretation
Trang 13We saw the small signal
D
I
I
V
D
V
+
-+
D a e
Large signal circuit:
Small signal response: i d = I D b v d
graphically mathematically
now, circuit
small signal circuit:
Linear!
d i i
- I D b
1
+ –
behaves like: + v d
-d
i
b I
1 R
D
=