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EUA4890 Datasheet(PDF) 12 Page - Eutech Microelectronics Inc |
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EUA4890 Datasheet(HTML) 12 Page - Eutech Microelectronics Inc |
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12 / 14 page ![]() EUA4890 DS4890 Ver 1.7 Dec. 2006 12 Application Information Bridged Configuration Explanation The structure of the EUA4890 is basically composed of two identical internal power amplifiers; the first one si externally configurable with gain-setting resistors Rin and Rf (the closed-loop gain is fixed by the ratios of theses resistors) and the second is internally fixed in an inverting unity-gain configuration by two resistors of 20kΩ. So the load is driven differentially through OUTA and OUTB outputs. This configuration eliminates the need for an output coupling capacitor. The differential-ended amplifier presents two major advantages: - The possible output power is four times larger (the output swing is doubled) as compared to single-ended amplifier under the same conditions. - Output pins (OUTA and OUTB) are biased at the same potential VDD/2, this eliminates the need for an output coupling capacitor required with a single-ended amplifier configuration. The differential closed loop-gain of the amplifier is given by Avd= Power Dissipation Power dissipation is a major concern when designing a successful amplifier, whether the amplifier is bridged or single-ended. A direct consequence of the increased power delivered to the load by a bridge amplifier is an increase in internal power dissipation. Since the EUA4890 has two operational amplifiers in one package, the maximum internal power dissipation is 4 times that of a single-ended amplifier. The maximum power dissipation for a given application can be derived from the power dissipation graphs of from equation1. ------------(1) It is critical that the maximum junction temperature TJMAX of 150°C is not exceeded. TJMAX can be determine from the power derating curves by using PDMAX and the PC board foil area. By adding additional copper foil, the thermal resistance of the application can be reduced, resulting in higher PDMAX. Additional copper foil can be added to any of the leads connected to the EUA4890.If TJMAX still exceeds 150°C, then additional changes must be made. These changes can include reduced supply voltage, higher load impedance, or reduced ambient temperature. Internal power dissipation is a function of output power. Proper Selection of External Components The EUA4890 is unity-gain stable and requires no external components besides gain-setting resistors, and input coupling capacitor and proper bypassing capacitor in the typical application. Gain-Setting Resistor Selection (Rin and Rf) Rin and Rf set the closed-loop gain of the amplifier. In order to optimize device and system performance, the EUA4890 should be used in low gain configurations. The low gain configuration minimizes THD + noise values and maximizes the signal to noise ratio, and the amplifier can still be used without running into the bandwidth limitations. Low gain configurations require large input signals to obtain a given output power. Input signals equal to or greater than 1Vrms are available from sources such as audio codecs. A closed loop gain in the range from 2 to 5 is recommended to optimize overall system performance. An input resistor (Rin) value of 20kΩ is realistic in most of applications, and does not require the use of a too large capacitor Cin. Input Capacitor Selection (Cin) The input coupling capacitor blocks the DC voltage at the amplifier input terminal. This capacitor creates a high-pass filter with Rin, the cut-off frequency is given by The size of the capacitor must be large enough to couple in low frequencies without severe attenuation. However a large input coupling capacitor requires more time to reach its quiescent DC voltage (VDD/2) and can increase the turn-on pops. An input capacitor value between 0.1µ and 0.39µF performs well in many applications (with Rin=22kΩ). Bypass Capacitor Selection (Cby) The bypass capacitor Cby provides half-supply filtering and determines how fast the EUA4890 turns on. This capacitor is critical component to minimize the turn-on pop. A 1.0µF bypass capacitor value (Cin=< 0.39µF) should produce clickless and popless shutdown transitions. The amplifier is still functional with a 0.1µF capacitor value but is more susceptible to pop and click noise. Thus, a 1.0µF bypassing capacitor is recommended. Power Supply Bypassing (CS) As with any amplifier, proper supply bypassing is critical for low noise performance and high power supply rejection. The capacitor location on both the bypass and power supply pins should be as close to the device is possible. ) R /(2π ) (V * 4 P L DD DMAX 2 2 = Vinrms Vorms in R f R 2 = × in C * in *R * 2 1 fc ∏ = |
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