Design Idea

Network linearizes dc/dc converter's current-limit characteristics

Thermistor adds to efficiency, eliminates sense resistor.

By John Guy and Lance Yang, Maxim Integrated Products Inc, Sunnyvale, CA; Edited by Brad Thompson and Fran Granville -- EDN, 10/13/2005

Recently announced versions of integrated step-down dc/dc converters have eliminated the requirement for a high-side current-sense resistor by sampling the voltage drop across an external, low-side, MOSFET synchronous rectifier. This topology eliminates the sense resistor's cost and pc-board-space requirement and also provides a modest increase in circuit efficiency. However, the MOSFET's highly temperature-dependent on-resistance dominates the current-limit value. Fortunately, certain newer dc/dc converters, such as Maxim's MAX1714, allow external adjustment of the current-limit threshold. The circuit in Figure 1 shows how a thermistor applies temperature compensation to the circuit's output-current limit.

The MAX1714's linear current-limit (ILIM) input range at Pin 6 of IC1 spans 0.5 to 2V, which corresponds to current-limit thresholds of 50 to 200 mV, respectively. For the default current-limit setting, 100 mV, the circuit imposes a 7.5A current limit at 25°C. However, Figure 2 shows that the current limit varies from 9A at –40°C to 6A at 85°C. To design the temperature-compensation network, begin by breadboarding the circuit and using an external power supply to vary the MAX1714's current-limit input volt-age such that the output-current-limit value remains constant. You repeat the measurements at 10°C intervals over the circuit's operating-temperature range.

To compensate for IC1's temperature variation, you can select from among several possible resistor-thermistor-network topologies. First, you need to select a suitable thermistor and characterize its resistance-versus-temperature variation. Because the MAX1714's current-limit input pin feeds a relatively high input-impedance voltage-follower stage, this thermistor requires a high nominal resistance of 100 kΩ. Resistance-versus-temperature characteristics of inexpensive thermistors exhibit considerable nonlinearity, but one relatively simple approach to linearization involves paralleling the thermistor with a fixed resistor equal to the thermistor's nominal resistance (Reference 1). In the network of Figure 1, R1 linearizes the thermistor, and R2 and R3, respectively, set the slope and intercept of the current-limit-voltage-versus-temperature-characteristic curve.

To arrive at optimal values for R2 and R3, we prepared a spreadsheet incorporating the original current-limit-voltage-versus-temperature data and added columns for each of the network's resistors, plus the thermistor specification sheet's resistance-versus-temperature data. While observing the circuit's temperature-versus-voltage transfer function, we varied the spreadsheet's values for R2 and R3 until the transfer function best approximated the measured current-limit-voltage-versus-temperature data. Finally, we constructed the circuit and tested it over the temperature range and noted that it yielded a reasonably flat response.


The curvature of the corrected output characteristic of Figure 2 (red trace) is intrinsic to the thermistor. Though not perfectly flat, the corrected curve represents a great improvement over the original (black trace) and is sufficient to meet the original design goal. You can achieve more precise compensation by selecting a different thermistor or by incorporating multiple thermistors.

Reference
  1. Horowitz, Paul and Winfield Hill, The Art of Electronics, ISBN 0 521 37095 7, Cambridge University Press, New York, 1980.



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