Non-Ideal Behavior of Components

advertisement
Non-Ideal Behavior of Components
Todd H. Hubing
Dept. of Electrical and Computer Engineering
Clemson, University
Clemson, SC 29634
USA
email: hubing@clemson.edu
Telephone: 1-864-656-7219
Circuit Schematics
Global EMC University
2007 IEEE International Symposium on EMC
2
Resistors
Global EMC University
2007 IEEE International Symposium on EMC
3
Resistance
l
R=
ohms
σA
Global EMC University
2007 IEEE International Symposium on EMC
4
Quiz Question
The D.C. resistance of a 5-cm trace on a printed circuit board is,
a.) about 100 ohms
b.) about 100 milliohms
c.) less than a milliohm
Global EMC University
2007 IEEE International Symposium on EMC
5
DC Resistance of a Printed Circuit Board
Trace
Trace length = 5 cm
Trace width = 0.25 mm
Trace thickness = 0.034 mm
σcu = 5.7 x 107 S/m.
0.05m
R=
= 0.10 ohms
7
−3
−3
( 5.7 × 10 S / m )( 0.25x10 m )( 0.034x10 m )
Global EMC University
2007 IEEE International Symposium on EMC
6
Skin Depth
High-frequency electric
fields and currents decay
exponentially with distance
from the surface of a good
conductor.
J ( x) = J S e
Global EMC University
− x πfμσ
2007 IEEE International Symposium on EMC
7
Skin Depth
1
δ=
π f μσ
Global EMC University
meters
2007 IEEE International Symposium on EMC
8
Resistance per unit length of a cable
At 60 Hz
δ60 Hz =
1
π ( 60 ) ( 4π × 10
Rinnerconductorat60Hz =
Routerconductorat60Hz
−7
)( 5.7 × 10 )
7
= 8.6 mm
1
1
=
= 22.3 mΩ / m
2
7
3
−
σ A ( 5.7 × 10 ) π (0.5 × 10 )
1
1
=
=
= 5.6 mΩ / m
7
−3
−3
σ A ( 5.7 × 10 ) 2π ( 5 × 10 )(0.1 × 10 )
total = 22.3 + 5.6 = 28 mΩ / m
Global EMC University
2007 IEEE International Symposium on EMC
9
Resistance per unit length of a cable
At 100 MHz
δ 100 MHz =
1
π (10 8 )( 4π × 10 −7 )( 5.7 × 107 )
= 0.0066 mm
Rinnerconductorat100MHz =
1
1
=
= 832 mΩ / m
7
−3
−6
σ A ( 5.7 × 10 ) 2π (0.5 × 10 )( 6.6 × 10 )
Routerconductorat100MHz =
1
1
=
= 85 mΩ / m
7
−3
−6
σ A ( 5.7 × 10 ) 2π ( 4.9 × 10 )( 6.6 × 10 )
total = 832 + 85 = 917 mΩ / m
Global EMC University
2007 IEEE International Symposium on EMC
10
Capacitors
Global EMC University
2007 IEEE International Symposium on EMC
11
Capacitance
Q
C=
V
E=
Q0
4πε 0 r
Vab = ∫
rb
ra
2
ra < r < rb
volts / m.
Q0
Q0 ⎡ 1 1 ⎤
dr =
− ⎥ volts.
⎢
2
4πε 0 r
4πε 0 ⎣ ra rb ⎦
Global EMC University
farads.
Cab =
Q0
4πε 0
=
Vab ⎡ 1 1 ⎤
⎢r − r ⎥
⎣ a b⎦
2007 IEEE International Symposium on EMC
farads.
12
Absolute Capacitance
Cabs = lim Cab = 4πε 0 ra
b→∞
Global EMC University
2007 IEEE International Symposium on EMC
farads.
13
Self and Mutual Capacitance
Global EMC University
2007 IEEE International Symposium on EMC
14
Self and Mutual Capacitance
Global EMC University
2007 IEEE International Symposium on EMC
15
Inductors
Global EMC University
2007 IEEE International Symposium on EMC
16
Inductance
Inductance is a property of current loops!
Ψ = ∫ B ⋅ ds
webers
S
L=
Ψ
I
henries
Global EMC University
2007 IEEE International Symposium on EMC
17
Inductance
⎡ ⎛ 8R ⎞
⎤
Lcircle ≈ N 2 Rμ ⎢ln⎜ ⎟ − 2.0⎥ henrys
⎣ ⎝ a ⎠
⎦
Global EMC University
Lsquare loop ≈ N 2
2μ 0 w ⎡ ⎛ w ⎞
⎤
−
ln
0
.
774
⎜
⎟
⎥ henrys
π ⎢⎣ ⎝ a ⎠
⎦
2007 IEEE International Symposium on EMC
18
Quiz Question
The inductance of a 2-cm wide, 10-cm long ground strap is,
a.) about 10 nanohenries
b.) about 100 nanohenries
c.) undefined
Global EMC University
2007 IEEE International Symposium on EMC
19
Loop Inductances
Global EMC University
2007 IEEE International Symposium on EMC
20
Mutual Inductance
L21 =
Global EMC University
Ψ 21
I1
henries.
2007 IEEE International Symposium on EMC
21
Partial Inductance
L21 =
Ψ 21
L12
henries.
I1
∫ B i ds
1
L21 =
henries.
S2
I1
∫ ( ∇ × A )i ds ∫
=
1
L21 =
S2
L21 =
μ
4π
I1
∫∫
dl1i dl2
R
L11
A1i dl2
I1
henries
henries
A1 = ∫
μ I1
dl webers / m
4π R
μ
Lij =
4π
I
J
∑∑ l
i =0 i = 0
ij
Useful for computer modeling.
Not useful for estimating inductance.
where
lij =
∫
∫
segment i segment j
Global EMC University
2007 IEEE International Symposium on EMC
dli i dl j
Rij
22
Partial Inductance (Branch Inductance)
Lloop = Ltrace + Lvia + Lvia + Lplane
Global EMC University
2007 IEEE International Symposium on EMC
23
Resistors
Global EMC University
2007 IEEE International Symposium on EMC
24
Do Resistors Have Capacitance and
Inductance?
Global EMC University
2007 IEEE International Symposium on EMC
25
Impedance of a 50-Ohm Resistor
0.8 pF
20 nH
48 ohms
Impedance in Ohms
1000
100
10
1
10
100
1000
Frequency in MHz
Global EMC University
2007 IEEE International Symposium on EMC
26
Types of Resistors
„ Metal Film
High precision, low cost
„ Composite
Medium precision, good transient immunity
„ Wire Wound
High power, high inductance
Global EMC University
2007 IEEE International Symposium on EMC
27
Capacitors
Global EMC University
2007 IEEE International Symposium on EMC
28
Do Capacitors Have Resistance and
Inductance?
0.011 μF
Global EMC University
2 nH
15 mohms
2007 IEEE International Symposium on EMC
29
Impedance of a 0.01-μF Capacitor
0.011 μF
15 mohms
2 nH
Impedance in Ohms
100
10
1
0.1
0.01
1
10
100
1000
Frequency in MHz
Global EMC University
2007 IEEE International Symposium on EMC
30
What are ESR and ESL?
?!!
Global EMC University
2007 IEEE International Symposium on EMC
31
SMT Capacitor Connection Inductance
CB = 3.4 nF
L BULK = 5 nH
L D = 2nH
CBULK = 1μ F
C D = 10nF
Bare Board
100.
10.
Board with
decoupling
1.
0.1
0.1 MHz
Global EMC University
1 MHz
2007 IEEE International Symposium on EMC
10 MHz
100 MHz
1 GHz
32
Types of Capacitors
„ Ceramic
Low cost, stable, good precision
„ Tantalum
Polarized, good energy density
„ Other Electrolytic
Polarized, good energy density
„ Mica
High-voltage applications
Global EMC University
2007 IEEE International Symposium on EMC
33
Inductors
Global EMC University
2007 IEEE International Symposium on EMC
34
Do Inductors Have Resistance and
Capacitance?
160 pF
15 mohms
5 μH
Global EMC University
2007 IEEE International Symposium on EMC
35
Impedance of a 5-μH Inductor
160 pF
15 mohms
5 μH
Impedance in Ohms
1000
100
10
1
0.1
1
10
Frequency in MHz
Global EMC University
2007 IEEE International Symposium on EMC
36
Types of Inductors
„ Ferrite Core
High inductance in small package
„ Air Core
Linear behavior under high-current conditions
„ Common-mode
Impedes common-mode currents while
passing differential-mode currents.
Global EMC University
2007 IEEE International Symposium on EMC
37
Ferrites
Fair-Rite 2643000701
Global EMC University
2007 IEEE International Symposium on EMC
38
Non-Ideal Behavior of Active Devices
Currents on the lead frame of an RDR memory
module at the third harmonic of the clock frequency.
Global EMC University
2007 IEEE International Symposium on EMC
39
Summary
„ All components (when connected to a circuit)
have resistance, capacitance and inductance.
„ The behavior of a component at high
frequencies is usually much different than the
nominal (low-frequency) behavior.
„ The inductance of a low-inductance device is
generally determined by the connection and is
not a property of the device itself.
Global EMC University
2007 IEEE International Symposium on EMC
40
Download