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MCP6044-I Datasheet(PDF) 13 Page - Microchip Technology |
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MCP6044-I Datasheet(HTML) 13 Page - Microchip Technology |
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13 / 34 page ![]() © 2008 Microchip Technology Inc. DS21669C-page 13 MCP6041/2/3/4 4.2 Rail-to-Rail Output There are two specifications that describe the output swing capability of the MCP6041/2/3/4 family of op amps. The first specification (Maximum Output Voltage Swing) defines the absolute maximum swing that can be achieved under the specified load condition. Thus, the output voltage swings to within 10 mV of either sup- ply rail with a 50 k Ω load to V DD/2. Figure 2-10 shows how the output voltage is limited when the input goes beyond the linear region of operation. The second specification that describes the output swing capability of these amplifiers is the Linear Output Voltage Range. This specification defines the maxi- mum output swing that can be achieved while the amplifier still operates in its linear region. To verify linear operation in this range, the large signal DC Open-Loop Gain (AOL) is measured at points inside the supply rails. The measurement must meet the specified AOL condition in the specification table. 4.3 Output Loads and Battery Life The MCP6041/2/3/4 op amp family has outstanding quiescent current, which supports battery-powered applications. There is minimal quiescent current glitching when Chip Select (CS) is raised or lowered. This prevents excessive current draw, and reduced battery life, when the part is turned off or on. Heavy resistive loads at the output can cause excessive battery drain. Driving a DC voltage of 2.5V across a 100 k Ω load resistor will cause the supply cur- rent to increase by 25 µA, depleting the battery 43 times as fast as IQ (0.6 µA, typical) alone. High frequency signals (fast edge rate) across capacitive loads will also significantly increase supply current. For instance, a 0.1 µF capacitor at the output presents an AC impedance of 15.9 k Ω (1/2πfC) to a 100 Hz sinewave. It can be shown that the average power drawn from the battery by a 5.0 Vp-p sinewave (1.77 Vrms), under these conditions, is EQUATION 4-1: This will drain the battery 18 times as fast as IQ alone. 4.4 Capacitive Loads Driving large capacitive loads can cause stability problems for voltage feedback op amps. As the load capacitance increases, the feedback loop’s phase margin decreases and the closed-loop bandwidth is reduced. This produces gain peaking in the frequency response, with overshoot and ringing in the step response. A unity gain buffer (G = +1) is the most sensitive to capacitive loads, although all gains show the same general behavior. When driving large capacitive loads with these op amps (e.g., > 60 pF when G = +1), a small series resistor at the output (RISO in Figure 4-3) improves the feedback loop’s phase margin (stability) by making the output load resistive at higher frequencies. The bandwidth will be generally lower than the bandwidth with no capacitive load. FIGURE 4-3: Output Resistor, RISO stabilizes large capacitive loads. Figure 4-4 gives recommended RISO values for different capacitive loads and gains. The x-axis is the normalized load capacitance (CL/GN), where GN is the circuit’s noise gain. For non-inverting gains, GN and the Signal Gain are equal. For inverting gains, GN is 1+|Signal Gain| (e.g., -1 V/V gives GN =+2 V/V). FIGURE 4-4: Recommended RISO Values for Capacitive Loads. After selecting RISO for your circuit, double check the resulting frequency response peaking and step response overshoot. Modify RISO’s value until the response is reasonable. Bench evaluation and simulations with the MCP6041/2/3/4 SPICE macro model are helpful. PSupply = (VDD - VSS) (IQ + VL(p-p) f CL ) = (5V)(0.6 µA + 5.0Vp-p · 100Hz · 0.1µF) = 3.0 µW + 50 µW VIN MCP604X RISO VOUT CL 1,000 10,000 100,000 1.E+01 1.E+02 1.E+03 1.E+04 Normalized Load Capacitance; CL/GN (F) 10p 1k 100k 100p GN = +1 GN = +2 GN +5 10k 10n 1n |
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