Keithley _25232870_Stabilizing_AN Datasheet

Page 1
LC´, CC´, RC´/ft.
RC´ LC´
CC´
Power Supply
Source Leads (twisted pair)
Phone
Test Fixture
Mobile Phone
L, C, R
Parasitic
Fixture L, C, R
R
cable
L
cable
V
senseVout
ERR AMP
230X
C
cable
C
DUT, fixture
+
–
Sense
OUT
AMP
Number 2870
Application Note
Series
Stabilizing Fast Transient Response Power Supply/Load Circuits
Introduction
Keithley’s Series 2300 Battery/Charger Simulators (fast transient response power supplies) are specifically designed for powering RFIC power amplifiers, mobile phone handsets, and other por­table, battery-operated products in R&D and manufacturing envi­ronments. These battery-simulating power supplies are designed to recover very quickly from short-duration pulse load current changes as large as 1000% (i.e., a 10× increase in load current) and to measure the peak of the load current pulse. In order to maintain the output voltage at the programmed output level despite near instantaneous pulse load changes and to capture information on pulses as short as 600µs, the power supply must combine a fast voltage recovery time with minimal voltage droop from the transient perturbation caused by the fast load current change. Power supplies like the Series 2300 battery/charger simulators must have a fast-responding, wide-bandwidth (beyond 200kHz and up to 2MHz) output stage. While this wide-band­width supply recovers quickly from large load current changes, the wide-bandwidth output stage is much more susceptible to the impedance of the external load circuit than conventional nar­row-bandwidth DC power supplies. Certain high reactance load conditions, such as long wire runs and capacitive loads with low equivalent series resistance (ESR), can cause the power supply output to begin oscillating. This paper will describe the various load circuit conditions that can cause oscillation and provide methods for stabilizing the load circuit.
The DC Power Supply/ Load Circuit Combination
Figure 1. Typical connec tions between a power supply and a DUT. The power
supply is using remote-sense feedback.
Figure 1
supply is energizing a device under test (DUT), in this case, a
illustrates a typical load power circuit in which a power
mobile phone in a test fixture. The power supply is using a four­wire connection scheme consisting of a pair of power sourcing
wires and a pair of load voltage sensing wires. The wires in each pair are twisted together to minimize spurious voltages result­ing from induced magnetic fields. The test fixtures often employ bypass capacitors to minimize AC noise. To understand how the load circuit performs for analysis of short load current pulses (effectively an AC signal), the two pair of wires must be modeled as an AC network of distributed resistive, series inductive, and parallel capacitive components. The test fixture and DUT must be modeled as an AC network as well. The cable capacitance, the parallel capacitance between the wires, is usually much smaller than the bypass capacitors added around the DUT, which are typically on the order of 10µF or larger.
Stability Analysis of the Power Supply/Load Circuit Combination
Figure 2. Simplified Series 2300 measurement schematic with reactive load
To analyze the Series 2300 power supply/load circuit combina­tion, the overall power supply is modeled as a feedback network consisting of an ideal error-correcting amplifier, an ideal out­put amplifier stage, and an ideal feedback sense amplifier (see
Figure 2
the load to force the power supply output to increase its voltage to overcome the losses in the test leads and fixture to ensure the desired (or programmed) voltage is applied to the load. The cables and test fixture connections/DUT are modeled as lumped­element components with the DUT and test fixture as defined by the dominant component, the parallel capacitance of the DUT.
plot, which shows the gain and phase performance as a function of frequency. mance of a Model 2306 power supply into an open circuit—effec­tively, a well-behaved resistive load. The loop gain falls to 0dB (unity gain) at a frequency slightly greater than 1MHz. If the loop gain is equal to one, and the output phase is 0º (positive feedback), the output will be unstable (consult the references in notes 1 and 3 and any electronics text that discusses the theory
and remote-sense feedback
). The sense amplifier measures the voltage directly at
A feedback network’s performance is characterized by a Bode
Figure 3
shows the loop gain and phase perfor-
Page 2
of feedback circuit design for more information). In the case of
totalcable
res
CL
f
2π
1
=
Cable
cableres
R
L
Qω=
=
=
TotalCableres
CR
ω
1
Total
Cable
Cable
C
L
R
1
60
40
20
0
–20
–40
–60
1kHz 10kHz 100kHz 1MHz 10MHz 100MHz
180°
100°
0°
–100°
–180°
Phase
Gain, dB
Phase
Gain
Phase margin at Unity Gain
Frequency
phase@Unity Gai
n
Unity Ga
in
p
oi
n
t
230X
Sen+, Src+
Sen–, Src–
C
bypass
the open circuit load, the Model 2306 has a phase margin of about 90º above 0º, which ensures the output is stable. Circuit design rules recommend a phase margin greater than 45º to guarantee circuit stability under all conditions.
The actual power supply/R-L-C load circuit combination has a multi-pole transfer function with the bandwidth and the unity gain point determined by the power supply control loop and the parameters of the R-L-C load. The L-C load components also determine the resonant frequency, which is near the frequency of oscillation. The resonant frequency (fres) is defined as follows:
If the phase margin is near 0º at this frequency, the power supply output will oscillate. Similarly, at the resonant frequency, the pole Q factor is:
To maximize the transient response and ensure stability, fres needs to be greater than the bandwidth of the power supply out­put circuit, and Q needs to be as small as possible.
The following sections describe methods to ensure a stable load circuit by effectively extending fres beyond the bandwidth of the power supply and to minimize Q. The four methods are:
1. Decreasing L
: Using good wiring techniques and low
cable
impedance cable
2. Decreasing C
: Eliminating unnecessary capacitors, typi-
Total
cally on the test fixture
3. Increasing R
: Adding resistance to the load circuit
Cable
4. Adding a compensation network to the load circuit.
Compensating for Inadequate Power Supply Transient Response with a Large Load Capacitor
When large capacitors are placed in parallel with the
DUT, the capacitance does improve stability, but there are
significant performance trade-offs involved. Prior to the avail-
ability of fast transient power supplies like the Series 2300,
manufacturers of portable devices such as mobile phones had
to work with conventional power supplies, which do not have
the bandwidth to respond effectively to large, near-instan-
taneous load current changes. The solution to maintaining
a near-constant output voltage was to put a large capacitor
in parallel with the load, essentially to add a second voltage
source in the load circuit (see
values of 100µF to 4700µF typically have a large equivalent
series resistance (ESR) that reduces the Q of the load circuit.
Furthermore, the equivalent series resistance of the capacitor
increases at higher frequencies and effectively adds additional
resistance to the circuit. The increased resistance at high fre-
quencies also acts to reduce Q and greatly enhance circuit sta-
bility. However, there are two disadvantages of using a large
capacitor at the load:
1. The power supply current readback circuit can no lon-
ger be used to measure a pulse load current because
the capacitor is supplying current to the load to hold
the voltage at the load steady.
Figure 4
). Large capacitors with
Figure 3. Model 2306 battery channel/2302 closed-loop gain and phase with
Using Good Wiring Techniques and Low Impedance Cable
Good wiring techniques minimize the coupling of external noise into a circuit and should be used in all applications. These techniques are essential for controlling instability in wide-band-
no load
2. Large electrolytic and tantalum capacitors have large
leakage currents, which prevents the power supply cur-
rent readback circuit from reading sleep mode or off-
state currents accurately.
Although adding a large capacitor at the load can increase
system stability, it is not a desirable solution. Using a fast tran-
sient power supply and removing the capacitor at the DUT
provides the best overall circuit performance.
Figure 4. The impact of a large bypass capacitor at the load when the DUT
load current increases.
Page 3
width power supply/load circuits. Twisted-pair source and sense
R
cable
R
add
R
add
L
cable
DC
230X
C
cable
C
DUT, fixture
+
–
RcCc
f
network
< f
res
π
2
1
=
leads should be used to reduce unwanted coupling from nearby interference sources and offer immunity to both electric and magnetic fields. Twisting the conductor pair between source and load minimizes the loop area, which limits the magnitude of induced voltages and cancels these noise voltages because they are of equal magnitude and opposite polarity in adjacent twists. Consequently, twisted wire pairs provide better immunity to magnetic fields than two closely spaced parallel conductors. Moreover, twisted wire pairs reduce the emission of magnetic fields. The current flow in the two close proximity wires is equal and opposite, so the resulting magnetic fields effectively cancel each other within a few inches of the pair. The twisted wire pair has lower inductance than an untwisted pair of wires of equal length. Typically, the inductance of a 15-foot-long (4.6m) twisted­pair cable is 2–4µH.
To minimize inductance in a given length of twisted-pair wire, use wire with thin Teflon® insulation. Thin insulation minimizes the loop area of the twists; and, Teflon is an insulator with a low dielectric constant, which provides the added benefit of minimizing the cable’s capacitance and reduces total cable impedance.
Adding Resistance to the Load Circuit
Increasing the resistance in the load circuit reduces Q and can enhance stability. the addition of two resistors to the load circuit. A recommended maximum value is 1Ω for each resistor. Using the least resistance necessary to achieve stability is optimal; thus, if 1Ω stabilizes the load circuit, experiment with lesser-value resistors to find the smallest acceptable value. A small additional voltage drop in each source lead can be overcome by the sense detection feedback network and the error correction circuitry that ensures the volt­age at the load is maintained at the programmed value. Another way to increase the load circuit resistance is to use thinner gauge wire. Either method for increasing R adds damping to the circuit. Therefore, although added resistance can improve stability, it also increases the load circuit time constant and the power sup­ply settling time.
Figure 5
shows the recommended location for
Another way to lower cable inductance is to keep the cable as short as possible. The closer the fixture/DUT is to the power supply, the lower the total cable inductance. Obviously, there are physical limitations on how close the DUT can be to the power supply, but routing the cabling as directly as possible to keep the cable length as short as possible helps ensure system stability.
If using twisted-pair wire and the shortest possible cables is not sufficient to ensure stability, low inductance cables can be used. Keithley’s Model SC-182 low inductance coaxial cable with Teflon insulation has a 10Ω characteristic impedance. A 4.6m length of this cable has 150–250nH of inductance. When com­pared with standard twisted cable, this is a reduction in induc­tance of an order of magnitude.
Using Teflon®-insulated twisted-pair wires, minimizing wire length, and using the SC-182 low inductance cable help reduce L
and enhance load circuit stability. However, using these
Cable
solutions does not alter the performance of the power supply/ load circuit combination.
Decreasing the Capacitance in the Load Circuit
Figure 5. Adding two resistors to Series 2300 source leads to improve
stability.
Adding a Compensation Network to the Load Circuit
A third method for improving stability involves adding two R-C compensation networks near the power supply between cor­responding sense leads and source leads (see technique bypasses the cable inductance and load capacitance of the feedback network for frequencies higher than the circuit resonant frequency (f
). The compensation capacitors (Cc) act
res
as a low impedance path for the high frequency components of the voltage waveform as it changes due to the load current tran­sitions. Compensating capacitors effectively close the feedback loop of the power supply/load circuit combination at approxi­mately fres and stabilize the circuit.
To compensate the power supply/load circuit combination with this network, the 3dB point of the low pass compensation network filter must be less than f
. Thus,
res
Figure 6
). This
Wherever possible, eliminate any capacitors in parallel with the DUT. The Series 2300 power supplies have the wide bandwidth and resulting fast transient response needed to maintain the voltage at the DUT during state transitions without the help of a parallel capacitor at the DUT. Eliminating capacitors reduces the total capacitance in the load circuit, so removing a parallel capac­itor at the DUT will improve the load circuit’s performance.
A recommended staring point is to set Rc to 100Ω, then determine an appropriate value of Cc to stop oscillation. Given that the sense feedback amplifier draws very little current, the 100Ω resistors create minimal error in the voltage at the DUT. While this is an effective method for improving stability,
Page 4
C
C
R
C
R
cable
L
cable
Sense –
R
C
Sense +
Source +
DC
230X
Source –
C
C
C
cable
C
DUT, fixture
+
–
Figure 6. Adding two compensation net works
this method reduces the effective bandwidth and the transient response of the power supply/load circuit network.
In addition to the external compensation network, the Model 2302 and Model 2306 power supplies offer internal bandwidth control to improve load circuit stability. The HIGH bandwidth setting produces the fastest transient response with dynamic loads. The LOW bandwidth setting (default instrument state) will have a slower response but will be more stable for most loads. The LOW bandwidth setting internally implements the compen-
sation capacitance technique shown in
Figure 6
.
Actual Instability Problem and the Stabilizing Solution
Figure 7
curve) to a 1A load current pulse. The load is resistive and cable length is negligible (the load is connected directly at the power supply output terminals). The voltage at the load exhibits a 10mV droop and 10mV overshoot in response to the rising edge and falling edge of the load current pulse. This is as close to the ideal response as can possibly be achieved.
depicts the actual system voltage response (lower
power supply/load circuit combination will be unstable and the voltage at the load will oscillate as shown in
Load Current
0.5A/Div
Load Voltage 10mV/Div
Time 0.1ms/Div
Figure 8. System instability (Lcable =1µH , C
DUT
= 2µF)
Figure 8
.
In this case, replacing the power supply load wire pair with the Keithley Model SC-182 Low Inductance Cable reduces the load impedance sufficiently to stabilize the circuit.
Figure 9
shows the resulting response to the load current pulse.
Load Current
0.5A/Div
Load Current
0.4A/Div
Load Voltage AC Response 10mV/Div
Time 0.1ms/Div
Figure 7. Transient response with resistive load and negligible cable length.
A more realistic situation involves cable lengths between the power supply and the DUT that can range from hundreds of nanohenrys to several microhenrys. In addition, the capacitance on the fixture and the DUT input capacitance can be as high as tens of microfarads. At these impedance levels, the system can be unstable. For example, with L
cable
=1µH and C
DUT
Load Voltage 10mV/Div
Time 0.1ms/Div
Figure 9. System stabilized (122cm. SC-182 cable, C = 2µF)
= 2µF, the
Page 5
Suggested Solution Sequence for Stabilizing the Power Supply/Load Circuit Combination
Following this suggested order of steps can help solve power supply/load circuit stability problems:
Eliminate any capacitors on the test fixture and across the
1. DUT wherever possible.
Reduce the inductance of the power supply wiring by using
2. wiring with Teflon insulation where possible. Alternatively, use the SC-182 coaxial cable with Teflon insulation. Use good wiring techniques and minimize the length of the wiring to the DUT.
If using either a Model 2302 or a Model 2306, try switching
3. to the LOW bandwidth setting to activate the internal com­pensation network.
If an oscillation is occurring at a frequency lower than
4. 100kHz (when using the Model 2303) or lower than 500kHz (when using the Model 2306), then try using an external compensation network.
If an oscillation is occurring at a frequency higher than
5. 100kHz (when using the Model 2303) or higher than 500kHz (when using the Model 2306), try adding resis­tance to the power supply/load circuit. Start with 1Ω in each source wire. If the 1Ω resistor stabilizes the circuit, experiment with smaller values until the circuit becomes unstable again, then choose a slightly larger value that re­stabilizes the circuit. The objective is to minimize the level of additional resistance in the circuit to optimize transient response. Remember that using a thinner gauge lead wire could add sufficient resistance to accomplish the same goal as adding resistors to the circuit.
The order of these steps is such that the initial steps have the least impact on circuit performance. Any of the techniques can be used in conjunction with others to resolve more difficult power supply/load circuit combinations.
Summary
While fast transient response power supplies provide the nec­essary performance to quickly recover from large pulse load currents, the wide bandwidth of these supplies makes them susceptible to instability in high reactance load circuits. The load circuit reactance is a function of the type of lead wire used, the length of the wire leads, components on the fixture, and the input reactance of the DUT. The combined reactance of these circuit elements must be minimized to obtain the full perfor­mance of the fast transient power supply. Methods to reduce the reactance include reducing cable inductance by minimizing the length of the cable or, for best results, using the Model SC-182 low inductance cable. Increasing the load circuit resistance is a second technique to improve stability. Using a thinner gauge cable or adding a small resistor in each source line accomplishes the objective of increasing the resistance in the load circuit. Eliminating unnecessary fixture capacitors reduces total circuit reactance and is the third technique. The fourth technique for improving stability involves adding a compensation network to the circuit to reduce the effective bandwidth of the circuit. Used individually or together, these four techniques can ensure power supply/load circuit stability and provide both a voltage output with minimal variation during dynamic load changes and mea­surements of DC and pulse load currents. The advantages of fast transient response power supplies far outweigh the additional effort in load circuit configuration to ensure stable performance.
Endnotes
1. Keithley Instruments W hite Paper, Optimizing Test Performance Of Digital Cellular Products With Ultra-High Speed Power Supplies, 2001, available at
ww w.keithley.com/data?asset=4643, retrieved July 26, 2007.
2. Campbell Scientific, Inc. White Paper, Preventing and Attacking Measurement Noise Problems, 2001, available at ww w.campbellsci.com/documents/
whitepapers/mnoise.pdf, retrieved July 26, 2007.
3. Spectrum Software, Plotting Loop Gain And Phase Margin, available at
http://www.spectrum-soft.com/news/winter2001/loopgain.shtm, 2001,
retrieved July 26, 2007.
Page 6
All Keithley trademarks and trade names are the property of Keithley Instr uments, Inc .
All other trademarks and trade names are the propert y of their respective companies.
Specifica tions are subject to change without no tice.
A G R E A T E R M E A S U R E O F C O N F I D E N C E
KEI TH LEY INSTRUMEN TS, INC. ■ 28775 AUR OR A ROAD ■ CLEV ELAND , OHI O 44139 -1891 ■ 440- 248 -04 00 ■ Fax: 440-2 48- 6168 ■ 1- 888-K EIT HL EY ■ ww w.ke ithle y.com
BE LG IUM
Sint-P ie te rs -L ee uw Ph : 02-363 00 40 Fax: 02-363 00 6 4 www .kei th le y.nl
CH INA
Be ij in g Ph : 8610 -822 55010 Fax: 8610- 82 255 018 www .kei th le y.com.cn
FI NLA ND
Es po o Ph : 09 -88171661 Fax: 09- 881716 62 www .kei th le y.com
FR ANC E
Sa in t- Au bi n Ph : 01-64 53 20 20 Fax: 01- 60 -11-77-2 6 www .kei th le y.fr
GE RMA NY
Ge rm er in g Ph : 089- 84 93 07- 40 Fax: 089-8 4 93 07- 34 www .kei th le y.de
IN DIA
Ba ng al ore Ph: 080-26771071-73 Fax: 080-26771076 www .kei th le y.com
ITALY
Mi lano Ph: 02-553842.1 Fax: 02-55384228 www .kei th le y.it
JA PA N
Tok yo Ph: 81-3-5733-7555 Fax: 81-3-5733-7556 www .kei th le y.j p
SW EDEN
So ln a Ph: 08-50 90 46 00 Fax: 08 -655 26 10 www .kei th le y.com
KORE A
Se ou l Ph: 82-2-574-7778 Fax: 82-2-574-7838 www .kei th le y.co.k r
SW ITZ ER L AN D
Zü ri ch Ph: 044-821 94 44 Fax: 41-44-820 30 81 www .kei th le y.ch
MA LAYS IA
Kuala Lumpu r Ph : 60 -3 -4 041-0 899 Fax: 60- 3- 40 42-0 899 www .kei th le y.com
TAIWAN
Hs in chu Ph: 886 -3-572-9077 Fax: 886 -3-572-9031 www .kei th le y.com.tw
NE THE RL AND S
Go ri nc he m Ph: 0183-63 53 33 Fax: 0183-63 08 21 www .kei th le y.nl
UN ITE D KI NGDOM
Th ea le Ph : 0118-929 75 0 0 Fax: 0118-929 75 19 www .kei th le y.co.uk
SI NG APO RE
Singapore Ph: 65-6747-9077 Fax: 65-6747-2991 www .kei th le y.com.sg
© Copyright 2007 Keithley Instruments, Inc. Printed in the U.S.A. No. 2870 0807
Loading...