TPA2001D1

1-W FILTERLESS MONO CLASS-D AUDIO POWER AMPLIFIER

SLOS338D – SEPTEMBER 2000 – REVISED DECEMBER 2002

6

POST OFFICE BOX 655303

APPLICATION INFORMATION

0 V

–5 V

+5 V

Current

OUTP

OUTN

Differential

Voltage

Across

Load

0 V

–5 V

+5 V

Current

OUTP

OUTN

Differential

Voltage

Across

Load

Output = 0 V

Output > 0 V

Figure 2. The TPA2001D1 Output Voltage and Current Waveforms Into an Inductive Load

efficiency: why you must use a filter with the traditional class-D modulation scheme

The main reason that the traditional class-D amplifier needs an output filter is that the switching waveform

results in maximum current flow. This causes more loss in the load, which causes lower efficiency. The ripple

current is large for the traditional modulation scheme because the ripple current is proportional to voltage

multiplied by the time at that voltage. The differential voltage swing is 2

half the period for the traditional modulation scheme. An ideal LC filter is needed to store the ripple current from

each half cycle for the next half cycle, while any resistance causes power dissipation. The speaker is both

resistive and reactive, whereas an LC filter is almost purely reactive.

The TPA2001D1 modulation scheme has very little loss in the load without a filter because the pulses are very

making the ripple current larger. Ripple current could be filtered with an LC filter for increased efficiency, but for

most applications the filter is not needed.

An LC filter with a cutoff frequency less than the class-D switching frequency allows the switching current to flow

through the filter instead of the load. The filter has less resistance than the speaker that results in less power

dissipated, which increases efficiency.