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SSM2275 数据表(PDF) 10 Page - Analog Devices |
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SSM2275 数据表(HTML) 10 Page - Analog Devices |
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10 / 16 page ![]() SSM2275/SSM2475 REV. A –10– This phase reversal can be prevented by limiting the input cur- rent to +1 mA. This can be done by placing a resistor in series with the input terminal that is expected to be overdriven. The series resistance should be at least: R V mA IN IN MAX = − , . 06 1 (3) An equivalent resistor should be placed in series with both in- puts to prevent offset voltages due to input bias currents, as shown in Figure 28. Output Short Circuit Protection To achieve high quality rail-to-rail performance, the output of the SSM2275/SSM2475 is not short-circuit protected. Shorting the output may damage or destroy the device when excessive voltages or currents are applied. To protect the output stage, the maximum output current should be limited to ±40 mA. Placing a resistor in series with the output of the amplifier as shown in Figure 29, the output current can be limited. The minimum value for RX can be found from Equation 4. R V mA X SY = 40 (4) For a +5 V single supply application, RX should be at least 125 Ω. Because R X is inside the feedback loop, VOUT is not affected. The trade off in using RX is a slight reduction in output voltage swing under heavy output current loads. RX will also increase the effective output impedance of the amplifier to RO + RX, where RO is the output impedance of the device. RFB FEEDBACK R X 125 VOUT A1 = 1/2 SSM2275 A1 Figure 29. Output Short Circuit Protection Configuration Power Dissipation Considerations While many designers are constrained to use very small and low profile packages, reliable operation demands that the maximum junction temperatures not be exceeded. A simple calculation will ensure that your equipment will enjoy reliable operation over a long lifetime. Modern IC design allows dual and quad amplifiers to be packaged in SOIC and microSOIC packages, but it is the responsibility of the designer to determine what the actual junction temperature will be, and prevent it from exceed- ing the 150 °C. Note that while the θ JC is similar between pack- age options, the θJA for the SOIC and TSSOP are nearly double the PDIP. The calculation of maximum ambient temperature is relatively simple to make. P TT MAX I MAX A A = − , θ J (5) For example, with the 8-lead SOIC, the calculation gives a maximum internal power dissipation (for all amplifiers, worst case) of PMAX = (150 °C – 85°C)/158°C/W = 0.41 W. For the DIP package, a similar calculation indicates that 0.63 W (ap- proximately 50% more) can be safely dissipated. Note that am- bient temperature is defined as the temperature of the PC board to which the device is connected (in the absence of radiated or convected heat loss). It is good practice to place higher power devices away from the more sensitive circuits. When in doubt, measure the temperature in the vicinity of the SSM2275 with a thermocouple thermometer. Maximizing Low Distortion Performance Because the SSM2275/SSM2475 is a very low distortion amplifier, careful attention should be given to the use of the device to prevent inadvertently introducing distortion. Source impedances seen by both inputs should be made equal, as shown in Figure 28, with RB = R1 RF for minimum distortion. This eliminates any offset voltages due to varying bias currents. Proper power supply decoupling reduces distortion due to power supply variations. Because the open loop gain of the amplifier is directly dependent on the load resistance, loads of less than 10 k Ω will increase the distortion of the amplifier. This is a trait of any rail-to-rail op amp. Increasing load capacitance will also increase distortion. It is recommended that any unused amplifiers be configured as a unity gain follower with the noninverting input tied to ground. This minimizes the power dissipation and any potential crosstalk from the unused amplifier. As with many FET-type amplifiers, the PMOS devices in the input stage exhibit a gate-to-source capacitance that varies with the common mode voltage. In an inverting configuration, the in- verting input is held at a virtual ground and the common-mode voltage does not vary. This eliminates distortion due to input capacitance modulation. In noninverting applications, the gate- to-source voltage is not constant, and the resulting capacitance modulation can cause a slight increase in distortion. Figure 30 shows a unity gain inverter and a unity gain follower configuration. Figure 31 shows an FFT of the outputs of these amplifiers with a 1 kHz sine wave. Notice how the largest har- monic amplitude (2nd harmonic) is –120 dB below the funda- mental (0.0001%) in the inverting configuration. SSM2275 RFB VOUT RL VIN R1 0.1 F 10 F V– 0.1 F 10 F V+ RB SSM2275 RFB VOUT RL VIN R1 0.1 F 10 F V– 0.1 F 10 F V+ RB Figure 30. Basic Inverting and Noninverting Amplifiers |
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