TS4909 datasheet(26/32 Pages) STMICROELECTRONICS

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Application information

TS4909

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The efficiency is the ratio between the output power and the power supply:

The maximum theoretical value is reached when VPEAK = VCC/2, so:

4.4.3

Total power dissipation

The TS4909 is a stereo (dual channel) amplifier. It has two independent power amplifiers.

Each amplifier produces heat due to its power dissipation. Therefore the maximum die

temperature is the sum of each amplifier’s maximum power dissipation. It is calculated as

follows:

●

Pdiss 1 = power dissipation due to the first channel power amplifier (Vout1).

●

Pdiss 2 = power dissipation due to the second channel power amplifier (Vout2).

●

Total Pdiss =Pdiss 1 +Pdiss 2 (W)

In most cases, Pdiss 1 = Pdiss 2, giving:

Single-ended configuration:

Phantom ground configuration:

4.5

Decoupling of the circuit

Two capacitors are needed to properly bypass the TS4909 — a power supply capacitor Cs

and a bias voltage bypass capacitor Cb.

Cs has a strong influence on the THD+N at high frequencies (above 7kHz) and indirectly on

the power supply disturbances. With 1

μF, you could expect the THD+N performance to be

similar to the values shown in this datasheet. If Cs is lower than 1 μF, THD+N increases at

high frequencies and disturbances on the power supply rail are less filtered. On the contrary,

if Cs is higher than 1 μF, those disturbances on the power supply rail are more filtered.

Cb has an influence on THD+N at lower frequencies, but its value is critical on the final result

of PSRR with inputs grounded in lower frequencies:

●

If Cb is lower than 1 μF, THD+N increases at lower frequencies and the PSRR worsens

(increases).

●

If Cb is higher than 1 μF, the benefit on THD+N and PSRR in the lower frequency range

is small.

OUT

supply

-------------------

πV

PEAK

---------------------

---

39.25%

TotalP

diss

diss1

diss2

TotalP

diss

22VCC

π R

---------------------- P

OUT

–

TotalP

diss

42VCC

π R

---------------------- P

OUT

–

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