一种121dB DR, 0.0017% THD+N, 8倍抖动效果降低的数字输入d类音频放大器,具有电源电压缩放音量控制和串联DSM

Wei-Hao Sun, Shih-Hsiung Chien, T. Kuo
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引用次数: 3

摘要

d类音频放大器已逐渐成为移动设备的标准组件,在大音量范围内需要更好的音频质量和更高的输出功率$(\ mathm {P}_{\ mathm {O}\ mathm {U}\ mathm {T}})$。然而,在移动设备中,$\ mathm {P}_{\ mathm {O}\ mathm {U}\ mathm {T}}$是有限的,因为锂离子电池的工作电压为3到4.2V。为了提高$\ mathm {P}_{\ mathm {O}\ mathm {U}\ mathm {T}}$,先前的出版物[1]-[3]已经开发了嵌入式升压转换器,以将升压电源电压$\ mathm {V}_{\ mathm {P}\ mathm {V}\ mathm {D}}$调节到5V或更高,以降低效率为代价。图31.3.1的顶部显示了一个典型的数字输入开环d类音频放大器,其中升压转换器仅在需要高$\ mathm {P}_{\ mathm {O}\ mathm {U}\ mathm {T}}$时才工作。输入信号首先乘以数字音量电平,然后通过插值器和δ - σ调制器(DSM)进行处理,以实现高信噪比(SQNR)。接下来,DSM输出通过pcm -PWM转换器转换成384kHz开关频率$\mathrm{f}_{\mathrm{S}\mathrm{W},\text{Class}}$)的PWM信号来驱动功率级。图31.3.1底部为不同$\ mathm {P}_{\ mathm {O}\ mathm {U}\ mathm {T}}$区域THD+N的主导因素。在$\mathrm{l}\mathrm{o}\mathrm{w}-\mathrm{P}_{\mathrm{o}\mathrm{U}\mathrm{T}}$区域,为了实现高动态范围(DR), DSM环路阶数应足够高,以获得更强的噪声整形能力,从而抑制DSM形量化噪声。然而,当DSM输入接近满量幅时,这往往会使DSM的量化器过载,导致由于$\text{high}-\ mathm {P}_{\ mathm {O}\ mathm {U}\ mathm {T}}$区域的剪切误差而导致THD+N快速增加。因此,THD+N< 1%时,最大的$\ mathm {P}_{\ mathm {O}\ mathm {U}\ mathm {T}}$会减少,这会浪费增强的$\ mathm {V}_{\ mathm {P}\ mathm {V}\ mathm {D}}$。除了sm型噪声外,当PWM脉冲在$\mathrm{l}\mathrm{o}\mathrm{w}-\mathrm{P}_{\mathrm{o}\mathrm{U}\mathrm{T}}$区域较窄时,pcm -PWM变换器的时钟(CLK)抖动噪声更为显著。$\text{medium}-\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$区域通常是THD+N的最小值所在,THD+N以d类幂级非线性为主。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A 121dB DR, 0.0017% THD+N, 8× Jitter-Effect Reduction Digital-Input Class-D Audio Amplifier with Supply-Voltage-Scaling Volume Control and Series-Connected DSM
Class-D audio amplifiers have gradually become standard components in mobile devices, where better audio quality over a wide volume range and higher output power $(\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}})$ are desired. However, in mobile devices, the $\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ is limited since Li-ion batteries operate at 3 to 4.2V. To increase $\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$, prior publications [1]–[3] have developed embedded boost converters to regulate boosted supply voltage $\mathrm{V}_{\mathrm{P}\mathrm{V}\mathrm{D}\mathrm{D}}$ to 5V or higher for the Class-D power stage at the expense of efficiency degradation. The top of Fig. 31.3.1 shows a typical digital-input open-loop Class-D audio amplifier, where the boost converter is operated only when high $\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ is required. The input signal is first multiplied by the digital volume level, and then processed by an interpolator and a delta-sigma modulator (DSM) to achieve a high signal-to-quantization-noise ratio (SQNR). Next, the DSM output is converted into a PWM signal with a 384kHz switching frequency $\mathrm{f}_{\mathrm{S}\mathrm{W},\text{Class}}$) by the PCM-to-PWM converter to drive the power stage. The bottom of Fig. 31.3.1 illustrates the dominant factors of the THD+N in different $\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ regions. In the $\mathrm{l}\mathrm{o}\mathrm{w}-\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ region, to achieve a high dynamic range (DR), the DSM loop order should be sufficiently high for more aggressive noise-shaping ability so as to suppress the DSM-shaped quantization noise. However, this tends to overload the DSM's quantizer when the DSM input is close to full scale, resulting in a rapidly increasing THD+N due to the clipping error in the $\text{high}-\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ region. As such, the maximum $\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ with THD+N<1 % is decreased, which squanders the boosted $\mathrm{V}_{\mathrm{P}\mathrm{V}\mathrm{D}\mathrm{D}}$. In addition to the DSM-shaped noise, the PCM-to-PWM converter's clock (CLK) jitter noise is more significant when PWM pulses are narrower in the $\mathrm{l}\mathrm{o}\mathrm{w}-\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ region. As for the $\text{medium}-\mathrm{P}_{\mathrm{O}\mathrm{U}\mathrm{T}}$ region, where the minimum THD+N is usually located, the THD+N is dominated by the Class-D power-stage nonlinearities.
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