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EL6203 Datasheet(PDF) 9 Page - Intersil Corporation |
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EL6203 Datasheet(HTML) 9 Page - Intersil Corporation |
9 / 10 page 9 Supply Bypassing and Grounding The resistance of bypass-capacitors and the inductance of bonding wires prevent perfect bypass action, and 150mVP-P noise on the power lines is common. There needs to be a lossy bead inductance and secondary bypass on the supply side to control signals from propagating down the wires. Figure 20 shows the typical connection. Also important is circuit-board layout. At the EL6203's operating frequencies, even the ground plane is not low- impedance. High frequency current will create voltage drops in the ground plane. Figure 21 shows the output current loops. For the pushing current loop, the current flows through the bypass capacitor, into the EL6203 supply pin, out the IOUT pin to the laser, and from the laser back to the decoupling capacitor. This loop should be small. For the pulling current loop, the current flows into the IOUT pin, out of the ground pin, to the laser cathode, and from the laser diode back to the IOUT pin. This loop should also be small. Power Dissipation With the high output drive capability, the EL6203 is possible to exceed the 125°C “absolute-maximum junction temperature” under certain conditions. Therefore, it is important to calculate the maximum junction temperature for the application to determine if the conditions need to be modified for the oscillator to remain in the safe operating area. The maximum power dissipation allowed in a package is determined according to: where PDMAX = Maximum power dissipation in the package TJMAX = Maximum junction temperature TAMAX = Maximum ambient temperature θJA = Thermal resistance of the package The supply current of the EL6203 depends on the peak-to- peak output current and the operating frequency which are determined by resistors RAMP and RFREQ. The supply current can be predicted approximately by the following equation: The power dissipation can be calculated from the following equation: Here, VSUP is the supply voltage. Figures 22 and 23 provide a convenient way to see if the device will overheat. The maximum safe power dissipation can be found graphically, based on the package type and the ambient temperature. By using the previous equation, it is a simple matter to see if PD exceeds the device's power derating curve. To ensure proper operation, it is important to observe the recommended derating curve shown in Figures 22 and 23. A flex circuit may have a higher θ JA, and lower power dissipation would then be required. FIGURE 20. RECOMMENDED SUPPLY BYPASSING +5V VS L Series: 70 Ω reactance at 300MHz 0.1µF CHIP EL6203 GND 0.1µF CHIP FIGURE 21. OUTPUT CURRENT LOOPS SINKING CURRENT LOOP SOURCING CURRENT LOOP SUPPLY BYPASS LASER DIODE RFREQ RAMP GND P DMAX T JMAX - TAMAX Θ JA --------------------------------------------- = I SUP 31.25mA 1k Ω × R AMP ------------------------------------------- 30mA 1k Ω × R FREQ ---------------------------------- 0.6mA ++ = P D V SUP I SUP × = FIGURE 22. PACKAGE POWER DISSIPATION vs AMBIENT TEMPERATURE 0.6 0.5 0.4 0.3 0.2 0.1 0 0 25 50 75 100 125 150 AMBIENT TEMPERATURE (°C) 85 JEDEC JESD51-3 LOW EFFECTIVE THERMAL CONDUCTIVITY TEST BOARD 488mW 5-P in SO T-2 3 θ JA = 25 6°C /W EL6203 |
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