
Keywords: MAX1626,MAX1627,efficiency killer,dcdc, converter circuits
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Source Resistance: The Efficiency Killer in DCDC Converter Circuits
© Apr 22, 2004, Maxim Integrated Products, Inc.


Abstract: DCDC converters, common in batterydriven, portable, and other highefficiency systems, can deliver efficiencies greater than 95% while boosting, reducing, or inverting supply voltages. Resistance
in the power source is one of the most important factors that can limit efficiency. This application note describes the effects of source resistance, how to calculate efficiency, realworld considerations, design considerations, and shows a realworld example.
DCDC converters are commonly used in batteryoperated equipment and other powerconserving applications. Like a
linear regulator, the DCDC converter can regulate to a lower
voltage. Unlike linear regulators, however, the DCDC converter can
boost an input voltage or invert it to create a negative voltage. As an added bonus, the DCDC converter boasts efficiencies greater than 95% under optimum conditions. However, this efficiency is limited by dissipative components. The main cause is resistance in the power source.
Losses due to source resistance can lower the efficiency by 10% or more, exclusive of loss in the DCDC converter! If the converter has adequate input voltage, its output will be normal and there may be no obvious indication that power is being wasted.
Fortunately, testing the input efficiency is a simple matter (see the Source section).
A large source resistance can cause other, less obvious effects. In extreme cases, the converter's input can become bistable, or its output can decrease under maximum load conditions. Bistability means that the converter exhibits two stable input conditions, each with its own efficiency. The converter output is normal, but system efficiency may be drastically affected (see How to Avoid Bistability).
Should this problem be solved simply by minimizing the source resistance? No, because the practical limits and cost/benefit tradeoffs posed by the system may suggest other solutions. A prudent selection of powersupply input voltage, for example, can considerably minimize the need for low source resistance. Higher input voltage for a DCDC converter limits the input current requirement, which in turn lessens the need for a low source resistance. From a systems standpoint, the conversion of 5V to 2.5V may be far more efficient than the conversion of 3.3V to 2.5V. Each option must be evaluated. The goal of this article is to provide analytic and intuitive tools for simplifying the evaluation task.
A Systems View
As shown in
Figure 1, any regulated powerdistribution system can be divided into three basic sections: source, regulator(s) (a DCDC converter in this case), and load(s). The source can be a battery or a DC power supply that is either regulated or unregulated. Unfortunately, the source also includes all the dissipative elements between the DC voltage and load: voltagesource output impedance; wiring resistance; and the resistance of contacts, PCboard lands, series filters, series switches,
hotswap circuits, etc. These elements can seriously degrade system efficiency.
Figure 1. A regulated powerdistribution system has three basic
sections.
Calculation and measurement of the source efficiency is very simple. EFF
_{SOURCE} equals (power delivered to the regulator)/(power provided by V
_{PS}) multiplied by 100%:
Assuming that the regulator draws a negligible amount of current when unloaded, you can measure source efficiency as the ratio of V
_{IN} with the regulator at full load to V
_{IN} with the regulator unloaded.
The regulator (DCDC converter) consists of a
controller IC and associated discrete components. Its characterization is described in the manufacturer's data sheet. Efficiency for the DCDC converter (EFF
_{DCDC}) equals (power delivered by the converter)/(power delivered to the converter) multiplied by 100%:
As specified by the manufacturer, this efficiency is a function of input voltage, output voltage, and output load current. It's not unusual for the efficiency to vary no more than a few percent over a load current range exceeding two orders of magnitude. Because the output voltage is fixed, we can say the efficiency varies only a few percent over an "outputpower range" exceeding two orders of magnitude.
DCDC converters are most efficient when the input voltage is closest to the output voltage. If the input variation is not extreme with respect to the data sheet specifications, however, the converter's efficiency can usually be approximated as a constant between 75% and 95%:
This discussion treats the DCDC converter as a twoport black box. For those interested in the nuances of DCDC converter design, see References 13. The load includes the device to be driven and all dissipative elements in series with it, such as PCtrace resistance, contact resistance,
cable resistance, etc. Because the DCDC converter's output resistance is included in the manufacturer's data sheet, that quantity is specifically excluded. Load efficiency (EFF
_{LOAD}) equals (power delivered to the load)/(power delivered by the DCDC converter) multiplied by 100%:
The key to optimum system designs is in analyzing and understanding the interaction between the DCDC converter and its source. To do this we first define an ideal converter, then calculate the source efficiency, then test our assumptions against measured data from a representative DCDC converterµin this case, the MAX1626
buck regulator.
The Ideal DCDC Converter
An ideal DCDC converter would have 100% efficiency, operate over arbitrary input and outputvoltage ranges, and supply arbitrary currents to the load. It would also be arbitrarily small and available for free! For this analysis, however, we assume only that the converter's efficiency is constant, such that input power is proportional to output power:
For a given load, this condition implies that the input currentvoltage (IV) curve is hyperbolic and exhibits a negative differentialresistance characteristic over its full range (
Figure 2). This plot presents IV curves for the DCDC converter as a function of increasing input power. For real systems with dynamic loads, these curves are also dynamic. That is, the power curve moves farther from the origin as the load demands more current. Considering a regulator from the input port instead of the output port is an unusual point of view. After all, regulators are designed to provide a constantvoltage (sometimes constantcurrent) output. Their specifications predominantly describe the output characteristics (outputvoltage range, outputcurrent range, output ripple, transient response, etc.). The input, however, displays a curious property: within its operating range it acts as a constantpower load (Reference 4). Constantpower loads are useful in the design of battery testers, among other tasks.
Figure 2. These hyperbolas represent constantpower input characteristics for a DCDC converter.
Calculating Source Efficiency
We now have enough information to calculate the source's power dissipation and therefore its efficiency. Because the opencircuit value of source voltage (V
_{PS}) is given, we need only find the DCDC converter's input voltage (V
_{IN}). From equation [5], solving for I
_{IN}:
I
_{IN} can also be solved in terms of V
_{PS}, V
_{IN}, and R
_{S}:
Equate the expressions from equations [6] and [7] and solve for V
_{IN}:
To understand their implications, it is very instructive to visualize equations [6] and [7] graphically (
Figure 3). The resistor load line is a plot of all possible solutions of equation [7], and the DCDC IV curve is a plot of all possible solutions of equation [6]. The intersections of these curves, representing solutions to the pair of simultaneous equations, define stable voltages and currents at the DCDC converter's input. Because the DCDC curve represents constant input power, (V
_{IN}+)(I
_{IN}+) = (V
_{IN}) (I
_{IN}). (The + and  suffixes refer to the two solutions predicted by equation [8], and correspond to the ± signs in the numerator.)
Figure 3. This plot superimposes a load line for source resistance on the DCDC converter's IV curve.
The optimum operating point is at V
_{IN}+/I
_{IN}+, which minimizes I
_{IN}2R
_{S} loss by drawing minimum current from the power supply. The other operating point causes large power dissipation in any dissipative components between V
_{PS} and V
_{IN}. System efficiency drops dramatically. But you can avoid such problems by keeping R
_{S} low enough. The source efficiency [(V
_{IN}/V
_{PS}) x 100%] is simply equation [8] divided by V
_{PS}:
It's easy to get lost in the equations, and therein lies the value of the loadline analysis plot of Figure 3. Note, for example, that if the series resistance (R
_{S}) equals zero, the resistor loadline slope becomes infinite. The load line would then be a vertical line passing through V
_{PS}. At this point V
_{IN+} = V
_{PS} and the efficiency would be 100%. As R
_{S} increases from 0Ω, the load line continues to pass through V
_{PS} but leans more and more to the left. Concurrently, V
_{IN+} and V
_{IN} converge on V
_{PS}/2, which is also the 50% efficiency point. When the load line is tangent to the IV curve, equation [8] has only one solution. For larger R
_{S}, the equation has no real solution and the DCDC converter no longer functions properly.
DCDC ConvertersTheory vs. Practice
How do these idealinput curves compare with those of an actual DCDC converter? To examine this question, a standard MAX1626
evaluation kit (
Figure 4) was configured for an output voltage of 3.3V and a load resistor of 6.6Ω. We then measured the input's IV curve (
Figure 5). Several nonideal characteristics were evident immediately. Note, for example, that for very low input voltages the input current is zero. A builtin undervoltage lockout (denoted as V
_{L}) ensures that the DCDC converter is off for all input voltages below V
_{L}. Otherwise, large input currents could be drawn from the power supply during startup.
Figure 4. A standard DCDC converter circuit illustrates the ideas of Figure 3.
Figure 5. Above V_{MIN}, the MAX1626 input IV characteristic closely matches that of a 90%efficient ideal device.
When V
_{IN} exceeds V
_{L}, the input current climbs toward a maximum that occurs when V
_{OUT} first reaches the preset output voltage (3.3V). The corresponding input voltage (V
_{MIN}) is the minimum required by the DCDC converter to produce the preset output voltage. For V
_{IN} > V
_{MIN}, the constantpower curve for 90% efficiency closely matches the MAX1626 input curve. Variations from the ideal are caused primarily by small variations in DCDC converter efficiency as a function of its input voltage.
How to Avoid Bistability
The powersupply designer must also guarantee that the DCDC converter never becomes bistable. Bistability is possible in systems for which the load line intersects the DCDC converter curve at or below V
_{MIN}/I
_{MAX} (
Figure 6).
Figure 6. A closer look at the intersection points indicates a possibility of bistable and even tristable operation.
Depending on the load line's slope and position, a system can be bistable or even tristable. Note that a lower V
_{PS} value can allow the load line to intersect at a single point between V
_{L} and V
_{MIN}, resulting in a system that is stable, but nonfunctional! As a rule, therefore, the load line must not touch the cusp of the DCDC converter curve and must not move below it.
In Figure 6, the loadline resistance (R
_{S}, which has a value of 1/slope) has an upper limit called R
_{BISTABLE}:
The source resistance (R
_{S}) should always be smaller than R
_{BISTABLE}. If this rule is broken, you risk highly inefficient operation or a complete
shutdown of the DCDC converter.
An Actual Case
It might be helpful to plot, for an actual system, the relationship shown in equation [9] between source efficiency and source resistance (
Figure 7). Assume the following conditions:
Figure 7. This plot of source efficiency vs. source resistance indicates multiple values of efficiency for a given R_{S}.
V
_{PS} = 10V Opencircuit powersupply voltage
V
_{MIN} = 2V Minimum input voltage that ensures proper operation
P
_{IN} = 50W Power to the DCDC converter's input (P
_{OUT}/EFF
_{DCDC}).
Using equation [12], R
_{BISTABLE} can be calculated as 0.320Ω. Subsequently, a plot of equation [9] shows that source efficiency drops as R
_{S} increases, losing 20% at R
_{S} = R
_{BISTABLE}. Note: this result cannot be generalized. You must perform the calculations for each application. One component of R
_{S} is the finite output resistance found in all power supplies, determined by the
load regulation and usually defined as:
Load Regulation =
Therefore,
A 5V/10A power supply with 1% load regulation, for example, would have only 5.0mΩ of output resistance not much for a 10A load.
Source Efficiency for Common Applications
It's useful to know how much source resistance (R
_{S}) can be tolerated and how this parameter affects system efficiency. R
_{S} must be less than R
_{BISTABLE}, as stated earlier, but how much lower should it be? To answer this question, solve equation [9] for R
_{S} in terms of EFF
_{SOURCE}, for EFF
_{SOURCE} values of 95%, 90%, and 85%. R
_{S}95 is the R
_{S} value that yields a 95% source efficiency for the given input and output conditions. Consider the following four example applications using common DCDC converter systems.
Example 1 derives 3.3V from 5V with a load current of 2A. For 95% source efficiency, be careful to keep the resistance between the 5V source and the DCDC converter's input well under 162m½. Notice that R
_{S}90 = R
_{BISTABLE}, by coincidence. This value of R
_{S}90 also implies that the efficiency could as easily be 10% as 90%! Note that system efficiency (as opposed to source efficiency) is the product of source efficiency, DCDC converter efficiency, and load efficiency.
Example 1. Application Using a MAX797 or MAX1653 DCDC Converter (I_{OUT} = 2A)
V_{PS} 
V_{OUT} 
I_{OUT} 
V_{MIN} 
EFF_{DCDC} 
P_{OUT} 
R_{BISTABLE} 
R_{S}95 
R_{S}90 
R_{S}85 
5V 
3.3V 
2A 
4.5V 
90% 
6.6W 
0.307Ω 
0.162Ω 
0.307Ω 
0.435Ω 
Example 2 is similar to Example 1 except for outputcurrent capability (20A vs. 2A). Notice that the seriesresistance requirement for 95% source efficiency is 10 times lower (16mΩ vs. 162mΩ). To achieve this low resistance, use 2oz. copper PC traces.
Example 2. Application Using a MAX797 or MAX1653 DCDC Converter (I_{OUT} = 20A)
V_{PS} 
V_{OUT} 
I_{OUT} 
V_{MIN} 
EFF_{DCDC} 
P_{OUT} 
R_{BISTABLE} 
R_{S}95 
R_{S}90 
R_{S}85 
5V 
3.3V 
20A 
4.5V 
90% 
66W 
0.031Ω 
0.016Ω 
0.031Ω 
0.043Ω 
Example 3 derives 1.6V at 5A from a source voltage of 4.5V (i.e., 5V10%). The system requirement of 111mΩ for R
_{S}95 can be met, but not easily.
Example 3. Application Using a MAX1710 DCDC Converter with Separate +5V Supply (V_{PS} = 4.5V)
V_{PS} 
V_{OUT} 
I_{OUT} 
V_{MIN} 
EFF_{DCDC} 
P_{OUT} 
R_{BISTABLE} 
R_{S}95 
R_{S}90 
R_{S}85 
4.5V 
1.6V 
5A 
2.5V 
92% 
8W 
0.575Ω 
0.111Ω 
0.210Ω 
0.297Ω 
Example 4 is the same as Example 3, but with higher supply voltage (V
_{PS} = 15V instead of 4.5V). Notice the useful tradeoff: a substantial increase in the difference between input and output voltages has caused an efficiency drop for the DCDC converter alone, but the overall system efficiency is improved. R
_{S} is no longer an issue because the large R
_{S}95 value (>1Ω) is easily met. A system with an input filter and long input lines, for example, can maintain a source efficiency of 95% or more without special attention to line widths and connector resistances.
Example 4. Application Using a MAX1710 DCDC Converter with Separate +5V Supply (V_{PS} = 15V)
V_{PS} 
V_{OUT} 
I_{OUT} 
V_{MIN} 
EFF_{DCDC} 
P_{OUT} 
R_{BISTABLE} 
R_{S}95 
R_{S}90 
R_{S}85 
15V 
1.6V 
5A 
2.5V 
86% 
8W 
3.359Ω 
1.149Ω 
2.177Ω 
3.084Ω 
Conclusion
When looking at DCDC converter specifications, it is tempting to maximize efficiency by setting the supply voltage as close to the output voltage as possible. This strategy, however, can increase costs by placing unnecessary limitations on elements such as the wiring, connectors, and trace layout. System efficiency may even suffer. The analytic tools presented in this article should make such powersystem tradeoffs more intuitive and obvious.
References
 Erickson, Robert W. Fundamentals of Power Electronics. Chapman and Hall, 1997.
 Lenk, Ron. Practical Design of Power Supplies. IEEE Press & McGraw Hill, 1998.
 Gottlieb, Irving M. Power Supplies, Switching Regulators, Inverters and Converters. Second Edition, TAB Books, 1994.
 Wettroth, John. "Controller Provides Constant Power Load." EDN, March 14, 1997.
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APP 3166: Apr 22, 2004
APPLICATION NOTE 3166,
AN3166,
AN 3166,
APP3166,
Appnote3166,
Appnote 3166
