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TDA8920CTH 参数 Datasheet PDF下载

TDA8920CTH图片预览
型号: TDA8920CTH
PDF下载: 下载PDF文件 查看货源
内容描述: 2 “ 110瓦特的D类功率放大器 [2 ´ 110 W class-D power amplifier]
分类和应用: 消费电路商用集成电路音频放大器视频放大器功率放大器光电二极管
文件页数/大小: 39 页 / 232 K
品牌: NXP [ NXP ]
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TDA8920C  
NXP Semiconductors  
2 × 110 W class-D power amplifier  
In the following example, a heatsink calculation is made for an 8 BTL application with a  
±30 V supply:  
The audio signal has a crest factor of 10 (the ratio between peak power and average  
power (20 dB)); this means that the average output power is 110 of the peak power.  
Thus, the peak RMS output power level is the 0.5 % THD level, i.e. 170 W.  
The average power is then 110 × 170 W = 17 W.  
The dissipated power at an output power of 17 W is approximately 7 W.  
When the maximum expected ambient temperature is 50 °C, the total Rth(j-a) becomes  
(148 50)  
= 14 K/W  
-------------------------  
7
Rth(j-a) = Rth(j-c) + Rth(c-h) + Rth(h-a)  
Rth(j-c) (thermal resistance from junction to case) = 1.1 K/W  
Rth(c-h) (thermal resistance from case to heatsink) = 0.5 K/W to 1 K/W (dependent on  
mounting)  
So the thermal resistance between heatsink and ambient temperature is:  
Rth(h-a) (thermal resistance from heatsink to ambient) = 14 (1.1 + 1) = 11.9 K/W  
The derating curves for power dissipation (for several Rth(j-a) values) are illustrated in  
Figure 9. A maximum junction temperature Tj = 150 °C is taken into account. The  
maximum allowable power dissipation for a given heatsink size can be derived, or the  
required heatsink size can be determined, at a required power dissipation level; see  
Figure 9.  
13.6 Pumping effects  
In a typical stereo single-ended configuration, the TDA8920C is supplied by a symmetrical  
supply voltage (e.g. VDD = 30 V and VSS = 30 V). When the amplifier is used in an SE  
configuration, a ‘pumping effect’ can occur. During one switching interval, energy is taken  
from one supply (e.g. VDD), while a part of that energy is returned to the other supply line  
(e.g. VSS) and vice versa. When the voltage supply source cannot sink energy, the voltage  
across the output capacitors of that voltage supply source increases and the supply  
voltage is pumped to higher levels. The voltage increase caused by the pumping effect  
depends on:  
Speaker impedance  
Supply voltage  
Audio signal frequency  
Value of supply line decoupling capacitors  
Source and sink currents of other channels  
Pumping effects should be minimized to prevent the malfunctioning of the audio amplifier  
and/or the voltage supply source. Amplifier malfunction due to the pumping effect can  
trigger UVP, OVP or UBP.  
TDA8920C_2  
© NXP B.V. 2009. All rights reserved.  
Product data sheet  
Rev. 02 — 11 June 2009  
20 of 39  
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