Output Noise
Measurement
In DC/DC Converters
In
the application of DC/DC converters, conflicts often arise between the end
user's output noise measurement and the manufacturer's specification.
Typically, the end user will connect an oscilloscope across the converter's
output with a 3 or 5 inch long ground lead on the scope probe, set the input to
AC coupling, increase the gain and measure the peak-to-peak noise on a 100 MHZ
bandwidth oscilloscope. The measurement may or may not agree with the manufacturer's
published specification. Usually, it does not. What went wrong?
What
is being measured are two noise signals - the conducted noise actually on the
converter's output pins, and radiated noise picked up on the long ground lead
of the scope probe. The conducted
output noise has two components - a "low" frequency ripple, and a
high frequency burst. The low frequency ripple present at the output of
converters is at the primary switching frequency. The high frequency noise is a
burst resembling a heavily damped ringing sinusoid at 40 to 50 MHZ, and is due
to reverse recovery of the rectifying diodes. This ringing occurs at the time
the switching transistor changes state from saturation to cutoff. It is this high frequency noise that
radiates over a few inches and couples into the loop antenna formed by the
scope probe and its associated ground lead.
The
peak-to-peak amplitude of the low frequency ripple and high frequency burst
noise increase with increased output load current. As load current rises, the output filter capacitor's ripple
current rises, causing a larger drop across its ESR (Effective Series
Resistance) and, consequently, a larger output ripple voltage. The rectifying
diode's recovery time and the energy dissipated during turn off both increase,
which raises the amplitude of the high frequency burst.
Factors affecting noise
measurements:
Several
factors affect measurements of noise amplitude, including oscilloscope
bandwidth, scope probe characteristics, the type of load, the number and length
of attached leads and the method of grounding the scope probe.
The
output noise of most converters (such as the 10A48R5 or 15A/A48R5) is specified
for a bandwidth of 20 Hz to 20 MHZ. The oscilloscope's bandwidth must be
limited to 20MHz when testing them since a 100 MHZ bandwidth will measure noise
amplitude several times higher.
Oscilloscope
probes of different types do not give equal measurements of noise amplitude.
The bandwidth, input capacitance, inductance, attenuation and grounding rings
differ from one type to another. Only
10X probes should be used for measuring noise because 1X probes do not have a
wide enough bandwidth.
While
Tektronix P6103 probes are good for general measurements, they are generally
poor for noise measurement and show high noise amplitude because their ground
ring makes a poor connection at the oscilloscope. Tektronix P6105A or P6131 probes of 3-foot (1 meter) length are
best for noise measurement because they make good ground connections.
Leads
attached to the converter act as antennas which pick up radiated noise and add
this to the measurement. The longer the
lead, the more noise is added. Digital
voltmeters generate switching noise internally and this can appear on their
input leads. For these reasons, remove
all unnecessary leads from the converter. Only the input power leads and output
load leads should be attached to the converter when measuring noise.
A
converter under test is generally loaded either with a resistor or with an
electronic load such as a Kikusui PLZ-72W. A resistor used to load a converter should be non-inductive or
have low inductance because inductance presents a high impedance to high
frequencies and results in a larger amplitude of the ringing noise. Measuring noise when using an electronic
load is not as simple as with a resistor.
The difference is related to the input characteristics of the load. An electronic load can give either higher or
lower noise measurements than a resistor load, depending on the type of
converter under test. A converter such
as the 15A/A48R5 will show lower output noise when loaded with an electronic
load than when loaded by a resistor.
The 15A/A48R15-15 will show higher noise when an electronic load is
used.
Measurement technique:
The
last and most important consideration in measuring noise is the method of using
the oscilloscope probe. Contact leads
must be as short as possible. Remove
all unnecessary leads which are attached to the converter.
It
is easy to make a 10-to-1 difference in the apparent amplitude of noise by
changing the technique of measurement.
A P6105A probe with its spring-loaded tip in place and with a 3 inch
ground lead can show switching noise amplitudes of 500mV or greater on a
15A/A48R5 converter. With exactly the
same setup (and not even turning off power to the converter), removing the
ground lead and spring tip from the probe and using the exposed ground ring and
tip to make contact will show noise amplitude near 50mV. The spring-loaded tip
adds about 1 1/4" of unshielded wire to the internal tip and acts as an
antenna. The ground lead adds another 3" of antenna.
Converter output noise is measured without a ground lead or
push-on spring-loaded tip on the scope probe.
The ground connection is made by using the ring behind the probe tip to
touch the converter's output ground pin while the probe tip touches the output
pin. A Tektronix 206-114-00 hook tip
adapter may be necessary to make contact between pins on some "A"
pinout converters. This gives a true measurement of conducted output
noise. Figure 1 illustrates this
technique.

Using the illustrated technique gives the most repeatable
and accurate noise measurements available.
APP Noise Measure
Converters.doc August 16,
2001