
6
DEMO MANUAL DC193
NO DESIGN SWITCHER
OPERATIO
U
Any unshielded lead, such as a ground lead on a scope
probe, acts as an antenna for the switching noise in the
supply. Therefore, any use of ground lead will invalidate
the measurement.
Further,beextremelycarefultoensurethatothersources
of noise do not invalidate the measurement. Noise from
the60Hzpowerlinethatfeedsthebenchsupplypowering
theLTC1626demonstrationboardcancauseerrorsinthe
measurement. This noise (especially spikes) can propa-
gate through the supply and appear on the ground of the
demonstration unit. If this is a problem, a battery can be
used to power the unit for ripple tests.
Also,bewaryofgroundloops.TheDCsupplyshouldfloat,
and the only ground should be that of the scope probe.
Never float the oscilloscope, as it may present a safety
hazard.
An alternative technique is to take a 50Ωor 75Ωpiece of
coaxandsolder theleads directlyto theoutputcapacitor.
Keep the shield over the center conductor for as great a
distance as possible. The center conductor can pick up
strayradiation whennot shielded, sominimize thelength
of exposed center conductor. The other end of the coax
should have a BNC connector for attaching to the
oscilloscope.
CHECKING TRANSIENT RESPONSE
Switching regulators take several cycles to respond to a
DC(resistive)loadcurrent.Whenaloadstepoccurs,V
OUT
shifts by an amount equal to ∆I
LOAD
• ESR, where ESR is
theeffectiveseriesresistanceofC
OUT
.∆I
LOAD
alsobegins
tochargeordischargeC
OUT
untiltheregulatorloopadapts
tothecurrentchangeandreturnsV
OUT
toitssteady-state
value. During this recovery time, V
OUT
can be monitored
for overshoot or ringing, which would indicate a stability
problem.TheexternalcomponentsshowninFigure1will
prove adequate for most applications.
Asecond,moresevere,transientiscausedbyswitchingin
loads with large (>1µF) supply bypass capacitors. The
dischargedbypasscapacitorsareeffectivelyputinparallel
withC
OUT
,causingarapid dropinV
OUT
.Noregulatorcan
deliverenough current to prevent this problemif the load
switch resistance is low and it is driven quickly. The only
solutionis tolimit therise timeof the switchdrive sothat
the load rise time is limited to approximately 25 • C
LOAD
.
Thus, a 10µF capacitor would require a 250µs rise time
limiting the charging current to about 200mA.
COMPONENTS
Component selection can be very critical in switching
power supply applications. The LTC1626 data sheet de-
tailsmore specificselection criteria formost ofthe exter-
nalcomponentssurroundingtheIC.Besuretorefertothe
data sheet if changes to this demonstration board are
anticipated.
Capacitors
InthecircuitshowninFigure1,C
IN
andC
OUT
arelowESR,
high ripple-current tantalum capacitors specifically de-
signedfor use inswitching powersupplies. ESR (equiva-
lent series resistance) is the parasitic series resistance in
the capacitor. Very often this resistance is the limiting
factor in reducing ripple at the output or input of the
supply. Standard electrolytic capacitors may cause the
feedback loop to be unstable (that is, your power supply
may become an oscillator). Also, they may cause poor
transientresponseorhavelimitedoperatinglife.Standard
capacitors generally do not have an ESR specification at
highfrequencies,forexampleat100kHz.So,althoughyou
may find a capacitor that works to your satisfaction in a
prototype,
the same part may not work consistently in
production
.
Standardtantalumcapacitors(mostnotably,thelowcost
ones) are not recommended for use in LTC1626 applica-
tions as they do not have the ability to take the large peak
currents that are required for the application. Tantalum
capacitors have a failure mechanism whereby they be-
come a low value resistor or short.
One alternative to tantalum and electrolytic capacitors is
organicsemiconductortypecapacitors(OSCONs)thatare
specifically made for power supply applications. They
exhibit very low ESR and are roughly one-half the size of
an equivalent electrolytic capacitor.
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