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OP484EP Fiches technique(PDF) 16 Page - Analog Devices |
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OP484EP Fiches technique(HTML) 16 Page - Analog Devices |
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16 / 20 page ![]() REV. 0 –16– OP184/OP284/OP484 Obviously, it is desirable to keep this comparison voltage small, since it becomes a significant portion of the overall dropout voltage. Here, the 20 mV reference, is higher than the typical offset of the OP284, but still reasonably low as a percentage of VOUT (< 0.5%). In adapting the limiter for other ILIMIT levels, sense resistor RS should be adjusted along with R7-R8, to main- tain this threshold voltage between 20 mV and 50 mV. Performance of the circuit is excellent. For the 4.5 V output version, the measured dc output change for a 225 mA load change was on the order of a few microvolts, while the dropout voltage at this same current level was about 30 mV. The current limit as shown is 400 mA, which allows the circuit to be used at levels up to 300 mA or more. While the Q1 device can actually support currents of several amperes, a practical current rating takes into account the SO-8 device’s 2.5 W, 25 °C dissipation. A short circuit current of 400 mA at an input level of 5 V will cause a 2 W dissipation in Q1, so other input conditions should be considered carefully in terms of Q1’s potential overheating. Of course, if higher powered devices are used for Q1, this circuit can support outputs of tens of amperes as well as the higher VOUT levels noted above. The circuit shown can be used either as a standard low dropout regulator, or it can also be used with ON/OFF control. By driving Pin 3 of U1 with the optional logic control signal VC, the output is switched between ON and OFF. Note that when the output is OFF in this circuit, it is still active (i.e., not an open cir- cuit). This is because the OFF state simply reduces the voltage input to R1, leaving the U1A/B amplifiers and Q1 still active. When ON/OFF control is used, resistor R10 should be used with U1, to speed ON-OFF switching, and to allow the output of the circuit to settle to a nominal zero voltage. Components D3 and R11 also aid in speeding up the ON-OFF transition, by providing a dynamic discharge path for C2. OFF-ON transition time is less than 1 ms, while the ON-OFF transition is longer, but under 10 ms. A +3 V, 50 Hz/60 Hz Active Notch Filter with False Ground To process signals in a single-supply system, it is often best to use a false ground biasing scheme. A circuit that uses this approach is illustrated in Figure 56. In this circuit, a false-ground circuit biases an active notch filter used to reject 50 Hz/60 Hz power line interference in portable patient monitoring equip- ment. Notch filters are quite commonly used to reject power line frequency interference which often obscures low frequency physiological signals, such as heart rates, blood pressure read- ings, EEGs, EKGs, et cetera. This notch filter effectively squelches 60 Hz pickup at a filter Q of 0.75. Substituting 3.16 k Ω resistors for the 2.67 kΩ in the twin-T section (R1 through R5) configures the active filter to reject 50 Hz interference. 1 3 5 6 7 11 2 +3V R1 2.67k Ω C1 1µF C2 1µF R3 2.67k Ω C3 2µF (1µF x 2) R4 2.67k Ω R5 1.33k Ω (2.67k Ω ÷ 2) R2 2.67k Ω VO R6 10k Ω VIN R8 1k Ω A2 A1 8 A3 R7 1k Ω R11 10k Ω 4 10 9 C5 0.03µF R12 150 Ω R10 20k Ω C4 1µF R9 20k Ω +3V 1.5V C6 1µF A1, A2, A3 = OP484 Q = 0.75 NOTE: FOR 50Hz APPLICATIONS CHANGE R1–R4 TO 3.1k Ω AND R5 TO 1.58k Ω (3.16kΩ ÷ 2). Figure 56. A +3 V Single Supply, 50/60 Hz Active Notch Filter with False Ground Amplifier A3 is the heart of the false-ground bias circuit. It simply buffers the voltage developed at R9 and R10 and is the reference for the active notch filter. Since the OP484 exhibits a rail-to-rail input common-mode range, R9 and R10 are chosen to split the +3 V supply symmetrically. An in-the-loop compen- sation scheme is used around the OP484 that allows the op amp to drive C6, a 1 µF capacitor, without oscillation. C6 maintains a low impedance ac ground over the operating frequency range of the filter. The filter section uses a OP484 in a twin-T configuration whose frequency selectivity is very sensitive to the relative matching of the capacitors and resistors in the twin-T section. Mylar is the material of choice for the capacitors, and the relative matching of the capacitors and resistors determines the filter’s pass band symmetry. Using 1% resistors and 5% capacitors produces satisfactory results. |
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