Bode 100 as Impedance Analyzer - omicron-lab.com...OMICRON Lab Webinar Series 2020 2020-05-05. Smart...
Transcript of Bode 100 as Impedance Analyzer - omicron-lab.com...OMICRON Lab Webinar Series 2020 2020-05-05. Smart...
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Bode 100 as Impedance Analyzer
OMICRON Lab Webinar Series 2020
2020-05-05
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Page 2Smart Measurement Solutions®
Webinar HintsOpen the Q&A function
Send questions to the presenters
We will record the presentation such that you can view it again later
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Page 3Smart Measurement Solutions®
Florian Hämmerle
• Studied Mechatronics at Vorarlberg University of Applied Sciences
• Working at OMICRON Lab since 2010 in:
− Technical Support & Applications
− Product management
• Contact:
− https://meet-omicron.webex.com/meet/florian.haemmerle
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Page 4Smart Measurement Solutions®
Tobias Schuster
• Completed electrical engineering college in 2013
• Studied Industrial Engineering and Management
• Working at OMICRON Lab since 2015 focusing on:− Technical Support
− Applications
− Sales
• Contact: − [email protected]
− https://meet-omicron.webex.com/meet/tobias.schuster
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Page 5Smart Measurement Solutions®
Agenda
• Passive components & equivalent circuits
• Bode 100 impedance measurement methods
• Calibration (user- & full-range)
• Why is it important to measure Cs
− Live comparison measurement
• Why should we measure Ls
− Live comparison measurement
− Leakage inductance
• Additional hands-on live measurements
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Page 6Smart Measurement Solutions®
Passive Components
• Essential parts in analog circuits
• Inductor and capacitor used e.g. to store energy or to
create filter circuits
Inductor: 𝑣 𝑡 = 𝐿𝑑𝑖 𝑡
𝑑𝑡𝑋𝐿 = 𝜔𝐿
𝑉
𝐼= 𝑍𝐿 = 𝑗𝜔𝐿
Capacitor: 𝑖 𝑡 = 𝐶𝑑𝑣 𝑡
𝑑𝑡𝑋𝐶 =
−1
𝜔𝐶
𝑉
𝐼= 𝑍𝐶 =
1
𝑗𝜔𝐶
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Page 7Smart Measurement Solutions®
Capacitor:• Plates are resistive
• Rolling of foils creates inductance
• Insulator not lossless
Theory and Reality
• Theoretically inductor and capacitor are purely reactive
elements → No resistive behavior and therefore lossless
• In reality parasitics can strongly influence the real
behavior especially at higher frequencies
Examples:
Inductor:• Wire has resistance
• Windings form electric field
• Core is not lossless
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Page 8Smart Measurement Solutions®
Equivalent Circuits
• Are used to model the real behavior of the components
• Different complexity of models
− 1st order models are valid at one particular frequency
Fixed Frequency measurement shows R, L and C at one frequency
Frequency Sweep
calculates R, L and C
over frequency
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Page 9Smart Measurement Solutions®
Equivalent Circuits
• Higher complexity models are valid for a frequency range
− 2nd Order equivalent circuits for inductor and capacitor
− 3rd Order models (e.g. quartz crystal or piezo element)
• Parameter identification requires manual
work or e.g. curve-fitting procedure
≙ ≙
see Application Note:
Equivalent Circuit Analysis of Quartz Crystals
https://www.omicron-lab.com/application-notes/
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Page 10Smart Measurement Solutions®
Bode 100 Impedance Measurement Methods
• One-Port Reflection
• Impedance Adapter (3-port technique)
• Shunt-Thru (2-port technique)
• Shunt-Thru with series resistance (similar to Shunt-Thru)
• Series-Thru (2-port technique)
• Voltage-Current Gain (3-port technique)
• External bridge (e.g. high impedance bridge)
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Page 11Smart Measurement Solutions®
Impedance Range Overview
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Page 12Smart Measurement Solutions®
One-Port
• Optimum range ≈ 0.5 Ω - 10 kΩ
• Impedance/Reflection measurement at the output port
• One point is GND
• Can be calibrated with Open/Short/Load (O/S/L)
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Page 13Smart Measurement Solutions®
One-Port (Measurement Setup)
• Solder to BNC connector
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Page 14Smart Measurement Solutions®
One-Port (Measurement Setup)
• Use BNC to 4 mm adapter
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Page 15Smart Measurement Solutions®
Impedance Adapter
• Optimum range ≈ 20 mΩ - 600 kΩ
• Impedance measurement using
the impedance adapters B-WIC or B-SMC
• DUT must not be connected to GND
• Must be calibrated with O/S/L
• Not for physically big components
or long leads
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Page 16Smart Measurement Solutions®
Impedance Adapter (Measurement Setup)
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Page 17Smart Measurement Solutions®
Shunt-Thru
• Optimum range ≈ 1 mΩ - 100 Ω
• Measure impedance using a 2 port shunt-thru setup in the 50 Ω system
• One point is GND
• Can be calibrated with Thru or O/S/L
• Attention: Ground-loop!
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Page 18Smart Measurement Solutions®
Shunt-Thru (Measurement Setup)
• with the B-LCM to suppress ground-loop error at low
frequencies (< 10 kHz to 100 kHz)
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Page 19Smart Measurement Solutions®
Shunt-Thru (Measurement Setup)
• with the B-AMP 12 to amplify the output signal of the
Bode 100 up to 25 dBm
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Page 20Smart Measurement Solutions®
Shunt-Thru (Measurement Setup)
• with the Picotest J2113A differential amplifier to suppress
ground-loop error at low frequencies
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Page 21Smart Measurement Solutions®
Shunt-Thru (Measurement Setup)
• with B-AMP12 and B-LCM
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Page 22Smart Measurement Solutions®
Shunt-Thru with series resistance
• Optimum range depends on series resistors
Rs = 200 Ω -> 5 mΩ – 1125 Ω
Rs = 499 Ω -> 11 mΩ – 2480 Ω
• One point is GND
• Must be calibrated
• Higher DC voltages possible
• Attention: Ground-loop!
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Page 23Smart Measurement Solutions®
Shunt-Thru with series resistance
(Measurement Setup)
• using Picotest PITK01 boards
series resistors
DUT
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Page 24Smart Measurement Solutions®
Series-Thru
• Optimum range ≈ 1 kΩ - 1 MΩ
• Measure impedance using a 2 port series-thru setup in
the 50 Ω system
• DUT must not be connected to GND
• Can be calibrated with Thru or O/S/L
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Page 25Smart Measurement Solutions®
Series-Thru (Measurement Setup)
• with the B-AMP 12 to amplify the output signal of the
Bode 100 up to 25 dBm
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Page 26Smart Measurement Solutions®
Voltage / Current
• Range depends on probes
• Measure impedance by using a voltage probe at CH2
and a current probe at CH1
• Can be calibrated with Thru or O/S/L
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Page 27Smart Measurement Solutions®
Voltage / Current (Measurement Setup)
• e.g. for input or output impedance measurement
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Page 28Smart Measurement Solutions®
External Bridge
• Range is variable
• Measure impedance using a custom measurement
bridge
• Must be calibrated with O/S/L
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Page 29Smart Measurement Solutions®
External Bridge (Measurement Setup)
• high impedance bridge
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Page 30Smart Measurement Solutions®
User-Range / Full-Range Calibration
• User Range Calibration
Calibrates at exactly the frequencies that are currently measured
+ No interpolation → suitable for narrowband probes
• Full-Range Calibration
calibrates at pre-defined frequencies and interpolates in-between
+ Calibration does not get lost when frequency range is changed
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Page 31Smart Measurement Solutions®
Why is it important to measure capacitors?
• A capacitor is NEVER just a capacitor
• Capacitor ESR influences the phase margin of power supplies
• Capacitor ESR influences the output ripple at the switching
frequency of a SMPS
• ESR can change over Frequency
• Capacitors are inductors above
their resonance frequency
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Page 32Smart Measurement Solutions®
What does the data sheet tell us?
220 µF aluminum capacitor
C = 220µF (± 20%)
𝐸𝑆𝑅 =tan 𝛿
𝜔𝐶=
0.12
2𝜋 ⋅ 120𝐻𝑧 ⋅ 220µF= 720 mΩ@ 120 𝐻𝑧
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Page 33Smart Measurement Solutions®
This is what the measurement tells us
Impedance
Phase
ESR
Capacitance
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Page 34Smart Measurement Solutions®
Live Comparison Measurement
Measurement of different types of 10 µF capacitors
• film (MKT / PET)
• aluminum
• film (PET)
• aluminum polymer
• tantalum
• ceramic (X5R)
• ceramic (X7R)
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Page 35Smart Measurement Solutions®
Why should we measure inductors?
• An inductor is NEVER just an inductor
• AC resistance <> DC resistance
− skin effects
− “Eddie Currents”
• Inductors have resonance frequencies
• Inductors with magnetic cores can have core losses
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Page 36Smart Measurement Solutions®
What does the data sheet tell us?
33 µH shielded power inductor
H = 33µH (± 20%) @ 1 kHz𝑅𝐷𝐶=0,049 𝛺 (𝑡𝑦𝑝.)𝑅𝐷𝐶=0,057 𝛺 (𝑚𝑎𝑥.)fres = 11 MHz
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Page 37Smart Measurement Solutions®
This is what the measurement tells us:
Impedance
Phase
ESR
Inductance
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Page 38Smart Measurement Solutions®
Live Comparison Measurement
Measurement of different types of 100 µH inductors
• SMD flat band
• litz wire
• copper wire
• planar coils(PCB winding structure)
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Page 39Smart Measurement Solutions®
Flyback Transformer Leakage Inductance
• Not all flux generated by the primary winding is coupled to the secondary winding
− some flux leaks
− some contributes to core losses
• Represented by a series inductance in the circuit
• Leakage inductance creates a voltage spike when turning off current through primary side (flyback converter)
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Page 40Smart Measurement Solutions®
Measuring Leakage Inductance
Leakage inductance is measured by shorting all other
windings except the primary winding
-110
010
110
210
310
410
510
103 104 105 106 107
TR
1/O
hm
f/HzTR1: Mag(Impedance) Memory 1 : Mag(Impedance)
0
2u
4u
6u
8u
10u
12u
103 104 105 106 107
TR
2/H
f/HzTR2: Ls(Impedance)
→ Leakage inductance is not constant over frequency
Secondary open Secondary shorted Leakage inductance
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Page 41Smart Measurement Solutions®
Additional Hands-On Live-Measurements
• Shunt-Thru measurement of
− mΩ resistor
− low ESR capacitor
• Series-Thru measurement
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Summary
• Component parasitics are
important to understand real life
circuit behavior
• Models considering parasitics
allow better simulation
• Measuring components can tell us more
than the data sheet says
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Page 43Smart Measurement Solutions®
References and Further Reading
[1] OMICRON Lab, Bode 100 User Manual, https://www.omicron-
lab.com/downloads/vector-network-analysis/bode-100/
[2] OMICRON Lab, Impedance Measurement Application Notes,
https://www.omicron-lab.com/applications/vector-network-
analysis/application-notes/#cuid1:pathGroup=.cuid10
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