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TPA2000D4 Datasheet(PDF) 17 Page - Texas Instruments |
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TPA2000D4 Datasheet(HTML) 17 Page - Texas Instruments |
17 / 27 page TPA2000D4 STEREO 2W CLASSD AUDIO POWER AMPLIFIER WITH STEREO HP AMPLIFIER SLOS337B − DECEMBER 2000 − REVISED NOVEMBER 2005 17 WWW.TI.COM APPLICATION INFORMATION effects of applying a square wave into a speaker Audio specialists have said for years not to apply a square wave to speakers. If the amplitude of the waveform is high enough and the frequency of the square wave is within the bandwidth of the speaker, the square wave could cause the voice coil to jump out of the air gap and/or scar the voice coil. A 250-kHz switching frequency, however, is not significant because the speaker cone movement is proportional to 1/f2 for frequencies beyond the audio band. Therefore, the amount of cone movement at the switching frequency is very small. However, damage could occur to the speaker if the voice coil is not designed to handle the additional power. To size the speaker for added power, the ripple current dissipated in the load needs to be calculated by subtracting the theoretical supplied power, PSUP THEORETICAL, from the actual supply power, PSUP, at maximum output power, POUT. The switching power dissipated in the speaker is the inverse of the measured efficiency, ηMEASURED, minus the theoretical efficiency, ηTHEORETICAL. (1) PSPKR = PSUP – PSUP THEORETICAL (at max output power) (2) PSPKR = PSUP / POUT – PSUP THEORETICAL / POUT (at max output power) (3) PSPKR = 1/ηMEASURED – 1/ηTHEORETICAL (at max output power) The maximum efficiency of the TPA2000D4 with an 8- Ω load is 85%. Using equation 3 with the efficiency at maximum power from Figure 2 (78%), we see that there is an additional 106 mW dissipated in the speaker. The added power dissipated in the speaker is not an issue as long as it is taken into account when choosing the speaker. when to use an output filter Design the TPA2000D4 without the filter if the traces from amplifier to speaker are short. The TPA2000D4 passed FCC and CE radiated emissions with no shielding with speaker wires 8 inches long or less. Notebook PCs and powered speakers where the speaker is in the same enclosure as the amplifier are good applications for class-D without a filter. A ferrite bead filter can often be used if the design is failing radiated emissions without a filter, and the frequency sensitive circuit is greater than 1 MHz. This is good for circuits that just have to pass FCC and CE because FCC and CE only test radiated emissions greater than 30 MHz. If choosing a ferrite bead, choose one with high impedance at high frequencies, but very low impedance at low frequencies. Use an output filter if there are low frequency (< 1 MHz) EMI sensitive circuits and/or there are long leads from amplifier to speaker. gain setting via GAIN0 and GAIN1 inputs The gain of the TPA2000D4 is set by two input terminals, GAIN0 and GAIN1. The gains listed in Table 1 are realized by changing the taps on the input resistors inside the amplifier. This causes the input impedance, ZI, to be dependent on the gain setting. The actual gain settings are controlled by ratios of resistors, so the actual gain distribution from part-to-part is quite good. However, the input impedance may shift by 30% due to shifts in the actual resistance of the input resistors. For design purposes, the input network (discussed in the next section) should be designed assuming an input impedance of 20 k Ω, which is the absolute minimum input impedance of the TPA2000D4. At the higher gain settings, the input impedance could increase as high as 115 k Ω. |
Similar Part No. - TPA2000D4_07 |
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Similar Description - TPA2000D4_07 |
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