ABC of Probing
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Transcript of ABC of Probing
Overview
What is a probe?
Influence of the probing on DUT
Basic types of probe:
• Passive probes
• Active Probes
• Differential Probes
• Current Probes
Questions
What is a probe?
The probe is the most common connection method between your oscilloscope and your DUT (Device Under Test).
A cable connection such as a BNC cable is another possibility.
The probe is a physical connection between the DUT signal of interest and the oscilloscope.
In theory a probe could be a simple wire connected to a circuit, in practice it is a complex circuit along with the oscilloscope.
What happens....
...when you connect the probe to the DUT?
1. The probe cannot transfer the true shape of your waveform to the screen of your oscilloscope.
2. The probe will influence the real shape of the waveform.
2.1 You’ll observe a different waveform on your display.
2.2 Differences will depend on both probe and waveform characteristics
3. The probe can load the DUT.
3.1 The DUT may operate in a different way due to the probe load.
What happens.... in theory
CABLE Rin =
Cin = 0
Easy to connect
No affect on the
original signal
Absolute Signal Fidelity
What really happens.... DC and Low Freq
• The probe is an additional “load” driven by
the source
• Probes are designed with an high resistence
on the tip to reduce the energy drawn from the source
and reduce the load
• Mantaining high impedance across all frequencies
Is the only way to guarantee accurate, repeatable
and reliable measurements
What really happens.... AC
• High input resistance is important but only at DC or Low frequncy AC;
at higher frequencies the capacitance of a probe dominates the overall
impedance
• The resulting probe impedance can effect the signal displayed on the
oscilloscope and the signal transmitted in your device
Impedance
• Probe Impedance can be calculated as frequency increases
•This means passive probes are great at DC but have some limitations at
higher frequencies
Effects of Frequency on Probe Impedance
• At DC or low frequencies the High Input Resistance
dominates the overall impedance
• As frequency increases the capacitance dominates
the impedance and daramatically lowers the overall
impedance
At 1 Hz the impedance is 10 MΩ
At 100 Hz the impedance is 9.5 MΩ
At 100 kHz the impedance is 174 kΩ
At 1 MHz the impedance is 17.4 kΩ
At 10 MHz the impedance is 1.74 kΩ
At 100 MHz the impedance is 174 Ω
The result of high probe capacitance
shows up in the signal shape seen on the
oscilloscope
Effects of Frequency on Probe Impedance
100%
90%
10% 0%
Source Signal Effects of Input Resistance
100% 90%
10% 0%
Effects of Input Capacitance Source Signal
100% 90%
10% 0%
100% 90%
10% 0%
...what about Inductance?
• The final piece to the electrical characteristic of a probe is grounding.
• Any lead adds inductance to the probe tip or probe ground circuit.
• A lead can also act as an antenna and pick up electrical noise from the
environment. That noise is added to the signal.
• The longer the ground lead, the higher the probe inductance
Esource
RIn
CIn LGround Lead
Probe Tip Rsource
...what about Inductance?
Pulse Measured with 1:10 Passive probe
A: without Ground Lead
B: 50 cm Ground Lead
C: 10 cm Ground Lead
D: BNC Direct (true
signal shape)
...what about Inductance?
100% 90%
10% 0%
Effects of Inductance Source Signal
100% 90%
10% 0%
Signal integrity – Bandwidht Limitations
30% Frequency
10%
20%
3%
Am
pli
tud
e
Measured Signal
Real Signal
• Probe bandwidth should match oscilloscope bandwidth
A 100 MHz probe on a 600 MHz scope will degrade the
measurement bandwidth!
Oscilloscope and probe bandwidth specified as -3 dB point
At -3 dB, the measured
signal will have 30%
amplitude degradation!
FUNDAMENTAL
3° ARMONIC
5° ARMONIC
7° ARMONIC
WAVEFORM RESULT
Signal integrity – Bandwidth Limitations
5 Times Rule
BW of system > 5 x Fundamental Frequency
• Complex signals contain sine waves
at varying frequencies and amplitudes
added together.
• The components are called
Harmonics and classified by levels
Signal integrity – Insufficient rise time
Insufficient rise time affects the acquisition
Measured rise time depends on the signal and scope rise times
Choose the right Probe
Type of signal – voltage, current, single-ended,
differential…
Signal frequency content (bandwidth issue)
Signal rise time
Source impedance (R and C)
Signal amplitudes (maximum and minimum)
Test point geometries
Basic Types of Probes
• Passive Probe Supplied as standard with the scope
No active devices, only passive parts
Physically and electrically robust – rugged mechanical design with capability to
measure several hundred volts
Bandwidth limited ( more often to 500 MHz)
Higher voltage capabilities
• Active Probe Usually an optional probe powered by the oscilloscope or by an external device
Based on an active device such as a transistor or FET
Not as robust as passive probe but much wider bandwidths and much lower
capacitance
The ideal probe for high frequency measurements
Usually with limited voltage range
Basic Types of Probes
• Differential Probe Active probe based on a differential amplifier
Measures the difference between two signals when there is no ground reference
Come in two types: • High voltage for floating measurements in a power supply, lighting ballast, motor drives, etc.
• High bandwidth for differential serial data streams
• Current Probe Active device that measures the current in a signal rather than the voltage
3 main types: • Transformer based for AC signals.
• Hall effect or combination transformer/Hall effect for AC&DC signals
• Rogowski effect for high currents (only AC signals)
Most modern clamp on current probes are combination transformer/Hall Effect
Passive Probe Basics
Probe
9 MΩ Scope
1 MΩ
Passive probes make an attenuator circuit with the
probe impedance and scope impedance
Attenuation ratio:
Passive Probe Basics.... Coupling importance
Probe
9 MΩ Scope
50 Ω
Signal is attenuated too much if coupling settings are
incorrect
Attenuation ratio:
Most modern passive probes have read-out option:
a sense pin that mates with a probe sense ring on
the oscilloscope. This automatically sets the correct
coupling and attenuation factor.
Passive Probe Basics.... No impedance matching??
Scope inputs also have resistance and capacitance
Probe
Passive Probe Basics.... No impedance matching??
Typical 10:1 Passive probes have an adjustment point that
allows the user to adjust the impedance of the passive
probe to match the impedance of the scope
Passive Probe Basics.... Compensation
Active Probe Basics
High Resistance
Low Capacitance
50 Ω
• Active probes can be based on a transistor or a FET
• Typically Active FET probes can provide higher overall
impedance – high resistance for DC and low frequencies,
low capacitance for high frequencies
• Active probes have high resistance
at the probe tip but terminate into the
scope 50 Ω input.
Active FET Probe
• Fixed or selectable attenuation - 1:1, 10:1, 100:1 (typical)
• Input capacitance - 0.5 – 3 pF (typical)
• Input resistance - 2 k – 10 MΩ (typical)
• Bandwidth - 500 MHz to 7.5 GHz (typical)
• Power source required
• Cable buffered, performance
independent of cable length
Active probes have limited input voltage range
Active or Passive?
• Both passive probes and active probes have strengths and weaknesses • Knowing when to use which probe will help make accurate and reliable measurements • Passive probes are great for low frequency measurements where high voltages may be probed • Active transistor probes are better for measurements which require the highest bandwidth possible, typically 2 GHz or greater • Active FET probes are a great general purpose probe for all frequencies from 10 kHz to 2 GHz but are not designed for signals above 8 – 12 V
Why Differential?
7-14-11 29
• General purpose oscilloscopes can only measure “Ground Referenced”
voltages however not all measurements are ground referenced
• Consider power supply measurements where the test points are referenced to
each other and there is no ground
Upper VGS measurement required
between point “A” and “B”
Differential Voltage Measurements
7-14-11 30
Methods for making differential measurements:
Float the scope
Channel “A” minus Channel “B”
Isolators
True differential
...a shocking esperience
7-14-11 32
Path to ground
UNSAFE!
Floating the
scope could be a
SHOCKING
experience!!!
“A” – “B” limitations
7-14-11 34
• This technique will not work when the signal of interest is much smaller than
the common mode
• Scope may not be able to obtain a stable trigger - Must trigger on either Ch A or Ch B, not the difference
• Poor high frequency CMRR restricts its use to rejecting common mode
signals at line frequency or lower
• Channel gain must be carefully calibrated to match probe attenuation - Standard probes and oscilloscope attenuators lack provision to precisely match
AC attenuation
Common Mode Rejection CMR
7-14-11 35
• Common Mode Rejection is the ability of the differential amplifier to
eliminate the common mode voltage from the output
• Real world differential almplifiers do not remove all of the common mode
signal
• The measure of how effective the differential amplifier is in removing
common mode is CMRR – Common Mode Rejection Ratio
• Why do we care about CMRR
- Common mode feedthrough sums with the signal of interest and becomes
indistinguishable from the true signal
Isolators
7-14-11 37
• An isolator allows the oscilloscope to make safe floating measurements - Consists of oscilloscope front end protected with insulation which drives a system based
on optical or transformer isolation
• Limitations od Isolators: - Unbalanced inputs
- Parasistic capacitance
- Low CMRR at high frequencies
True Differential Measurements
7-14-11 38
+175 Volts
- 175 Volts
“A”
“B”
Output
Important Characteristics:
• Common Mode Range
• Common Mode Rejection Ratio
• True Balanced Inputs
Load “sees” high Impedance
Lead parasitic effects cancel out !
True differential amplifiers – The Best Solution
7-14-11 40
• Accurate differential measurements while oscilloscope is safely grounded
• Two high impedance matched inputs
• High CMRR over wide frequency ranges
• Two types of products - High Voltage Active Differential Probes:
- Good performance, low cost but CMRR, Noise and Overdrive Recovery are
sacrificed
- CMRR up to 10.000:1
- Differential Amplifier with probe pair:
- Excellent performance, highest CMRR, low noise and excellent overdrive
recovery, cost is higher
- CMRR up to 100.000:1
How can we measure currents?
7-14-11 41
•Shunts - DC to High Frequency AC
- Embedded Sensors
•Transformers - AC Current Transformers (CT)
- AC Currents Probe
•Hall Devices - DC to Low Frequency AC
•Transformers + Hall Devices - DC to High Frequency AC
Shunts
7-14-11 42
•Advantages:
- Low inductance coaxial shunts
can be very accurate
- Wide Bandwidth – DC to High
Frequency
- Wide Dynamic range – high
crest factor
•Disadvantages:
- Requires differential voltage
measurement
- Inserts Impedance (resistence)
into Circuit Under Test
- Requires circuit to be broken
Current Transformer CT
7-14-11 43
•Advantages:
- Precision transformers can be
very accurate
- Low Cost
•Disadvantages:
- Measures only AC
- DC component moves (lowers)
the dynamic range for
measuring AC components
- Requires circuit to be broken
- Inserts Impedance into Circuit
Under Test
Transformer / Hall Device Current Probes
7-14-11 44
•Advantages:
- Measures both AC & DC
- Easy to attach to circuit
- Moderate cost
•Disadvantages:
- May require access wire to be
added to circuit
- Inserts Impedance into Circuit
Under test
Oscilloscope current probes
7-14-11 45
• Most oscilloscope current probes use the combination of
transformer and Hall technologies.
• These types of probes provide a more general purpose
solution because of the ability to measure from DC to high
frequency AC
• These types of probes also can be designed with a split core
so they can be clamped on to the circuit not requiring a break
in the wire
Best way to choose your probe
7-14-11 46
First one you find available in a drawer!
Best way to choose your probe
7-14-11 47
Distract a colleague and take theirs!