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AD1990 Scheda tecnica(PDF) 13 Page - Analog Devices |
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AD1990 Scheda tecnica(HTML) 13 Page - Analog Devices |
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13 / 16 page ![]() AD1990 Rev. 0 | Page 13 of 16 POWER STAGE The H-Bridge The output stage of the AD1990 includes four integrated MOSFET devices arranged in a full H-bridge, as shown in Figure 23. The P-Type, high-side transistor of one leg and the N-Type, low-side transistor of the opposite leg switch on and off as a pair producing a total voltage swing across the load of −PVDD to +PVDD. The drive is floating and differential, and it is important that neither output terminal be shorted to ground. The power supply for the output stage of the AD1990, PVDD, should be in the 8 V to 20 V range and should be capable of supplying enough current to drive the load. Connect the power supply across the PVDD and PGND pins. The feedback pins, NFR+, NFR−, NFL+, and NFL−, supply negative feedback to the modulator as described in the Setting the Modulator Gain section. For reactive loads, the impedance can only be below the recommended threshold over a small portion of the amplifier’s bandwidth. In these cases, the amplifier can enter overcurrent shutdown in response to even small input signals in those frequency bands. When designing a system, use the minimum load impedance over the entire range of amplified frequencies when calculating current output rather than the average or nominal load impedance ratings often cited by loudspeaker driver manufacturers. Output Transistor Nonoverlap Time The AD1990 allows the user to select from one of eight different nonoverlap times, as shown in Figure 24. Nonoverlap time prevents or minimizes the period during which both the high- side and low-side devices are on simultaneously due to propagation delays and nonzero rise and fall times. If both the upper and lower portions of a half-bridge conduct simultaneously, there is a path directly from the power supply to ground and an induced current flow known as shoot-through. However, introducing this delay increases distortion by pushing the switching pattern further from an ideal two-state waveform. Selecting the nonoverlap delay requires a compromise between distortion and efficiency. The logic levels on the three delay control pins, DCTRL2, DCTRL1, and DCTRL0, set the nonoverlap time according to Table 12. The state of DCTRL[2:0] is read on the rising edge of RESET and should not be changed while RESET is logic high. Table 12. Nonoverlap Time Settings DCTRL2 DCTRL1 DCTRL0 Nonoverlap Time (ns)1 0 0 0 62 0 0 1 49 0 1 0 37 0 1 1 24 1 0 0 15 1 0 1 13.5 1 1 0 12 1 1 1 9 1 Values are typical and are not production tested. HIGH-SIDE GATE DRIVE LOW-SIDE GATE DRIVE tNOL tNOL Figure 24. Half-Bridge Nonoverlap Delay Timing The shortest setting (DCTRL[2:0] = 111) or the second shortest setting (DCTRL[2:0] = 111) is recommended for most applications. These two settings allow a small trade-off between efficiency and distortion. Longer nonoverlap times generally increase distortion while providing little or no decrease in shoot- through current. CLOCKING The AD1990 Σ-Δ modulator requires an external clock source with a nominal frequency of 12.288 MHz. This clock can come from a crystal or from an existing clock signal in the application circuit. The discrete time portions of the modulator run internally at 6.144 MHz, corresponding to 128 × fS, where fS = 48 kHz. As mentioned in the Σ-Δ Modulator section, the modulator has a noise-shaping effect such that SNR is increased within the audio band by shifting modulator quantization noise upward in frequency. For an external clock frequency of 12.288 MHz, the modulator’s noise-shaping works in a manner that results in a flat noise floor at the amplifier output for frequencies 20 kHz and below. Above 20 kHz, the amplifier noise rises due to the spectral shaping of the modulator quantization noise. At very high frequencies, the noise floor levels off and decreases due to poles in the modulator noise-transfer function and in the external LC filter. The clock frequency does not have to be exactly equal to 12.288 kHz and can vary by up to ±10%. For other rates, the noise corner scales linearly with frequency. When the modulator runs at a rate lower than nominal, the average power stage switching frequency decreases, the efficiency increases slightly, and the noise floor begins to rise at a slightly lower frequency. Likewise, a faster clock gives slightly increased bandwidth and slightly lower efficiency. |
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