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CLC436 数据表(PDF) 5 Page - National Semiconductor (TI) |
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CLC436 数据表(HTML) 5 Page - National Semiconductor (TI) |
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5 / 6 page ![]() Figure 3: Single Supply Circuit Power Dissipation The power dissipation of an amplifier can be described in two conditions: • Quiescent Power Dissipation - PQ (No Load Condition) • Total Power Dissipation - PT (with Load Condition) The following steps can be taken to determine the power consumption of the CLC436: 1. Determine the quiescent power PQ = Icc (Vcc - Vee) 2. Determine the RMS power at the output stage PO = (Vcc - Vload) (Iload) 3. Determine the total RMS power PT = PQ + PO The maximum power that the package can dissipate at a given temperature is illustrated in the Power Derating plot in the Typical Performance Characteristics section. The power derating curve for any package can be derived by utilizing the following equation: where: Tamb = Ambient temperature in °C θ JA = Thermal resistance, from junction to ambient, for a given package in °C/W Layout Considerations A proper printed circuit layout is essential for achieving high frequency performance. Comlinear provides eval- uation boards for the CLC436 (730013 - DIP, 730027- SOIC) and suggests their use as a guide for high frequency layout and as an aid for device testing and characterization. Supply bypassing is required for optimum performance. The bypass capacitors provide a low impedance current return path at the supply pins. They also provide high frequency filtering on the power supply traces. Other layout factors also play a major role in high frequency performance. The following steps are recommended as a basis for high frequency layout: 1. Include 6.8 µF tantalum and 0.01µF ceramic bypass capacitors on both supplies. 2. Place the 6.8 µF capacitors within 0.75 inches of the power pins. 3. Place the 0.01 µF capacitors within 0.1 inches of the power pins. 4. Remove the ground plane near the input and output pins to reduce parasitic capacitance. 5. Minimize all trace lengths to reduce series inductances. State Variable Filter The filter shown on the front page offers both a band- pass and a low pass output. The design equations are shown below. The state variable filter can be modified to obtain a tunable band pass filter. This technique is shown in the CLC522, Wideband Variable Gain Amplifier, data sheet. Transimpedance Application The low 1.1pA/ √Hz input current noise and unity gain stability make the CLC436 useful as a photo diode pre- amplifier. Figure 4 illustrates a transimpedance amplifier. Rf sets the transimpedance gain. The photodiode current is multiplied by Rf to determine the output voltage. Figure 4: Transimpedance Amplifier The feedback capacitor (Cf) is required to compensate for the added input capacitance of the photodiode (Cd). The feedback capacitance reduces peaking in the fre- quency response. As the value of the feedback capac- itance increases from zero, the rolloff of the response will increase. P 175 Tamb JA = °− () θ Q R R A R R , desired mid band gain f Q 2R C , desired resonant frequency RR 1 3 v 1 4 r 1 23 = =− = = π + - CLC436 Rf Vo Vin Vcc Rg R2 R1 Vcc C1 C2 Applications Circuit Iin - + CLC436 436 Fi 5 Cd Rf Cf Photo Diode Representation Vo = Iin*Rf Vo 5 http://www.national.com |
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