Data Domains and Transduction
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Transcript Data Domains and Transduction
Circuit Theory 2
Topics
• Impedance matching,
• Impedance transformation,
• Bandwidth and Noise.
How you will use these topics
• Understanding the rangefinder circuits,
• Optimizing rangefinder performance,
• Understanding transducer models.
Impedance matching
What is impedance matching?
• Any signal source has an associated source impedance.
• Any “load” circuit driven at a port exhibits an
associated impedance across the terminals of the port.
• Matching these impedances optimizes the transfer of
power from the source to the load.
A source with a voltage divider:
Rsource
R1 R2
R1 R2
R1
R2
A composite load circuit:
Rload
R R R2 R3 R3 R1
1 2
R2 R3
R1
R2
R3
Thevenin’s and Norton’s Theorems
Ideal sources
• An ideal voltage source has zero source impedance.
• An ideal current source has zero source admittance.*
Thevenin’s theorem: any electrical signal source is
equivalent to an ideal voltage source in series with
a source impedance.
Norton’s theorem: any electrical signal source is
equivalent to an ideal current source in parallel
with a source admittance.*
* (Admittance is the complex reciprocal of impedance)
Thevenin and Norton example
Actual source
100
2V
Thevenin equivalent
100
50
1V
Norton equivalent
20
mA
50
DC matching: simple example and proof
A battery with voltage Vg and
internal resistance Rg is
connected to a load resistor Rl.
The power delivered to Rl is
P Vl I l
Vg Rl
Vg
Rg Rl Rg Rl
Rg
Vg
Il
Vl
V g2 Rl
( Rg Rl ) 2
The maximum deliverable power occurs for
2
2
V
R
V
( Rg Rl )
dP
d
l
g
g
0
,
2
3
dRl
dRl ( Rg Rl ) ( Rg Rl )
Rl Rg
Rl
Impedance transformation
Ideally is a lossless two-port circuit.
Conservation of energy:
V
• avg( I1V1 ) avg( I 2V2 ) 0
• Reciprocal: power can flow either way.
I1
I2
Port
1
1
I1
Realizations:
• Wideband: transformer with n1, n2 turns,
Port
2
V2
I2
V1 n1
n2 V2
V2 / V1 n2 / n1 I1 / I 2 , Z2 / Z1 (n2 / n1 )2
• Resonant “Pi” network: at resonance,
Zin R2 (C2 / C1 )2
L
Zin
C1
C2
R2
Magnetic transformers
The magnetic field H k1n1I1 is proportional to the
total primary current linking the magnetic path.
Magnetic induction B H , where is the
permeability of the magnetic path.
The voltage induced per turn is V k2dB / dt , so the
secondary voltage V2 kn1n2 dI1 / dt, where k k1k2 .
Similarly, V1 kn2dI1 / dt , so V2 / V1 n2 / n1.
Conservation of energy requires I1 / I 2 V2 / V1, so
Impedance is transformed as Z 2 / Z1 (n2 / n1 )2.
1
Pi net
C2 Ls 2+Ls+R2
Zin
C1C2 LR2 s 3+C1Ls 2+(C1+C2 )R2 s+1
L
Zin
C1
C2
R2
P lotof Z in ( f ) [] for
R2 100[k],
L 25.4 [mH],
C1 800[nF],
C2 400[pF],
f 40 60 [kHz].
(blue = real, olive = imaginary)
Bandwidth and Noise
Note the Pi net bandwidth was about 3 [kHz].
The transformer was wideband.
Why is bandwidth important?
• Response time is inversely proportional to bandwidth.
This limits the range resolution of the rangefinder.
• Noise is directly proportional to bandwidth. This limits
the maximum operational distance for the rangefinder.
Therefore, a design tradeoff exists between range
resolution and maximum range.
Impedance matching homework problem
Find the load impedance that
accepts the maximum deliverable
power from a 5 [V] sinusoidal
source Vg at 40 [kHz], having a
source impedance due to an
internal series resistance of 50
[Ohms] and inductance 500 [uH].
What components, values, and
topology will implement this load?
Rg
Vg
Lg
Sources homework problem
Show the Thevenin and
Norton equivalents of
the circuit shown.
10
20
10
10
Extra credit:
Suppose you were given a sealed box 0.05[m] x 0.05[m] x 0.02[m],
weighing 0.1[kg] with two electrical terminals. It is totally opaque,
even to x-rays and ultrasound and cannot be disassembled for
inspection. When open circuited, the voltage across the terminals is 1
[V]. When short circuited, the current between the terminals is 1 [A].
You are told this is either a Thevenin source or a Norton source. How
would you determine which? You may make any measurements you
like on the unit.