SLUSG35 August 2026 TPS12S24F-Q1
ADVANCE INFORMATION
Resistive loads are the simplest loads to drive as they follow Ohm’s Law (V = I * R).
It's simple because the designer knows the voltage (typically 13.5V or 52V for a car battery) and the resistance of the load (by measuring it with an Ohm meter). With these two parameters they can calculate the maximum current that will be flowing through the circuit. In typical applications the current through the load needs to be varied to provide the intended output. The most basic way to vary the current through the load is through pulse width modulating (PWM).
An inductive load is any load that stores magnetic energy when connected to a supply voltage. The inductive load impedance consists of both a resistance and inductance in series. When they are switched off inductive loads can generate a transient negative voltage of hundreds of volts due to the stored magnetic energy in the inductance. This transient voltage can cause severe damage to the drive circuit. To prevent any potential damage, during switch-off the stored magnetic energy must be dissipated by clamping the voltage across the inductive load. An external TVS or standard diode is connected from output to ground (or TVS diode across drain to source) that protects the circuit by clamping the voltage over the switch to a set voltage and recirculating the current through the clamp. This causes the stored energy to be safely dissipated. With this large clamp voltage the demagnetization time is decreased leading to a safe and quick turn off time for inductive loads.
Figure shows application circuit for driving resistive or Inductive loads. Refer to Table 7-1 for all configurable parameters during this mode.