SLVAEZ0 November   2020 TPS1H000-Q1 , TPS1H100-Q1 , TPS1H200A-Q1 , TPS1HA08-Q1 , TPS1HB35-Q1 , TPS2H000-Q1 , TPS2H160-Q1 , TPS2HB16-Q1 , TPS2HB50-Q1 , TPS4H000-Q1 , TPS4H160-Q1

 

  1.   Trademarks
  2. 1Background
    1. 1.1 High-Side Switch
    2. 1.2 Thermal Modeling Using Electrical Analysis
    3. 1.3 Varying RDSON
  3. 2Using TI's SPICE Models With Incorporated Thermal Behavior
    1. 2.1 Basics of PSpice - Modifying Components
    2. 2.2 Basics of PSpice - Adding Libraries and Components
    3. 2.3 Basics of PSpice - Running Simulations
  4. 3Simulating the Junction Temperature in PSpice
  5. 4How to Leverage Thermal Simulations
  6. 5Model Limitations
  7. 6Conclusion

Varying RDSON

The on-resistance, RDSON , is the inherent resistance of the High-Side Switch device. This value depends on the temperature of the device, as well as whether the switch is in the saturation or linear region. Since RDSON is a factor in calculating an accurate power pulse and calculating the junction temperature relies heavily on inputting an accurate power pulse, varying RDSON as it varies due to temperature is an important factor to consider. The power dissipated by the switch, PDISS, can be calculated as the product of the current through the switch, IDS, and the voltage across the switch, VDS.

Equation 4. GUID-20201124-CA0I-NFZZ-7BNL-KGVHQHHKP3BK-low.gif

However, in the linear region it is easier to calculate the power dissipated by the switch, PDISS, as the product of the squared current through the switch, IDS, and the on-resistance of the switch, RDSON.

Equation 5. GUID-20201124-CA0I-XT9C-JC52-TMBKCHJRDQZW-low.gif

RDSON varies as a function of temperature, as Figure 1-2 from the TPS1H100 data sheet shows in the Typical Characteristics plot of RDSON.

GUID-4CD75C0F-D207-4649-8A2A-EBA83E98BCB3-low.pngFigure 1-2 Characteristic Plot of RDSON of TPS1H100

To account for this change in temperature, the PSpice model must recursively take into account the maximum temperature, and then recalculate using the corresponding RDSON for that temperature. Since the RDSON decreases for decreasing temperature, the RDSON will eventually converge onto a realistic RDSON value instead of the worst-case RDSON in the data sheet. The equation of the plot can be approximated as a line as Equation 6 shows.

Equation 6. GUID-20201124-CA0I-DKMT-Q60Z-CGWXG34NNQXV-low.gif

Where m is the slope of the line and b is the value of RDSON at 0°C. To account for this change in RDSON, the PSpice thermal model recursively measures the simulated junction temperature. First, the model inputs the worst-case RDSON, located in the electrical characteristics section of the high-side switch data sheet. After this initial junction temperature value is calculated, the model iterates until the temperature and RDSON converges. Figure 1-3 illustrates this behavior.

GUID-20201124-CA0I-V3J9-R7NQ-BMNXPDGN2NLK-low.pngFigure 1-3 Block Diagram of Model

With the implementation of the thermal behavior implemented within the PSpice model, the recursive calculation is automatically taken care of in the software.