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AD816 Datasheet(PDF) 12 Page - Analog Devices |
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AD816 Datasheet(HTML) 12 Page - Analog Devices |
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12 / 16 page ![]() AD816 REV. B –12– PRINTED CIRCUIT BOARD LAYOUT CONSIDERATIONS As to be expected for a wideband amplifier, PC board parasitics can affect the overall closed-loop performance. Of concern are stray capacitances at the output and the inverting input nodes. If a ground plane is to be used on the same side of the board as the signal traces, a space (5 mm min) should be left around the signal lines to minimize coupling. POWER SUPPLY BYPASSING Adequate power supply bypassing can be critical when optimiz- ing the performance of a high frequency circuit. Inductance in the power supply leads can form resonant circuits that produce peaking in the amplifier’s response. In addition, if large current transients must be delivered to the load, then bypass capacitors (typically greater than 1 µF) will be required to provide the best settling time and lowest distortion. A parallel combination of 10.0 µF and 0.1 µF is recommended. Under some low frequency applications, a bypass capacitance of greater than 10 µF may be necessary. Due to the large load currents delivered by the AD816, special consideration must be given to careful bypassing. The ground returns on both supply bypass capacitors as well as signal common must be “star” connected as shown in Figure 44. RF RG (OPTIONAL) RF +VS +OUT –OUT –VS +IN –IN DRIVER A DRIVER B RF RG RF RG IN IN RECEIVER A RECEIVER B OUT OUT Figure 44. Signal Ground Connected in “Star” Configuration POWER CONSIDERATIONS The 500 mA drive capability of the AD816 driver enables it to drive a 50 Ω load at 40 V p-p when it is configured as a dif- ferential driver. This implies a power dissipation, PIN, of nearly 5 watts. To ensure reliability, the junction temperature of the AD816 should be maintained at less than 175 °C. For this rea- son, the AD816 will require some form of heat sinking in most applications. The thermal diagram of Figure 45 gives the basic relationship between junction temperature (TJ) and various components of θ JA. TJ = TA + PIN θJA Equation 1 θA (JUNCTION TO DIE MOUNT) θ B (DIE MOUNT TO CASE) θ A + θ B = θ JC CASE TA TJ θ JC θ CA TA θ JA TJ PIN WHERE: PIN = DEVICE POWER DISSIPATION TA = AMBIENT TEMPERATURE TJ = JUNCTION TEMPERATURE θ JC = THERMAL RESISTANCE – JUNCTION TO CASE θ CA = THERMAL RESISTANCE – CASE TO AMBIENT Figure 45. A Breakdown of Various Package Thermal Resistances Figure 46 gives the relationship between output voltage swing into various loads and the power dissipated by the AD816 (PIN). This data is given for both sine wave and square wave (worst case) conditions. It should be noted that these graphs are for mostly resistive (phase < ±10°) loads. When the power dissipation requirements are known, Equation 1 and the graph on Figure 47 can be used to choose an appropriate heat sinking configuration. 4 3 10 20 30 40 2 1 VOUT – Volts p-p RL = 50 RL = 100 RL = 200 f = 1kHz SQUARE WAVE SINE WAVE VS = 15V Figure 46. Total Power Dissipation vs Differential Driver Output Voltage |
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