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LTC6090 Datasheet(PDF) 11 Page - Analog Devices |
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LTC6090 Datasheet(HTML) 11 Page - Analog Devices |
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11 / 18 page ![]() LT1210X 11 1210Xfa For more information www.linear.com/LT1210X APPLICATIONS INFORMATION When the LT1210X is used to drive capacitive loads, the available output current can limit the overall slew rate. In the fastest configuration, the LT1210X is capable of a slew rate of over 1V/ns. The current required to slew a capacitor at this rate is 1mA per picofarad of capacitance, so 10,000pF would require 10A! The photo (Figure 6) shows the large-signal behavior with CL = 10,000pF. The slew rate is about 150V/µs, determined by the current limit of 1.5A. Differential Input Signal Swing The differential input swing is limited to about ± 6V by an ESD protection device connected between the inputs. In normal operation, the differential voltage between the input pins is small, so this clamp has no effect; however, in the shutdown mode the differential swing can be the same as the input swing. The clamp voltage will then set the maximum allowable input voltage. To allow for some margin, it is recommended that the input signal be less than ±5V when the device is shut down. Capacitance on the Inverting Input Current feedback amplifiers require resistive feedback from the output to the inverting input for stable operation. Take care to minimize the stray capacitance between the output and the inverting input. Capacitance on the invert- ing input to ground will cause peaking in the frequency response (and overshoot in the transient response), but it does not degrade the stability of the amplifier. Power Supplies The LT1210X will operate from single or split supplies from ±5V (10V total) to ±15V (30V total). It is not neces- sary to use equal value split supplies, however the offset voltage and inverting input bias current will change. The offset voltage changes about 500µV per volt of supply mismatch. The inverting bias current can change as much as 5µA per volt of supply mismatch, though typically the change is less than 0.5µA per volt. Power Supply Bypassing To obtain the maximum output and the minimum distor- tion from the LT1210X, the power supply rails should be well bypassed. For example, with the output stage pour- ing 1A current peaks into the load, a 1 power supply impedance will cause a droop of 1V, reducing the available output swing by that amount. Surface mount tantalum and ceramic capacitors make excellent low ESR bypass elements when placed close to the chip. For frequencies above 100kHz, use 1µF and 100nF ceramic capacitors. If significant power must be delivered below 100kHz, capacitive reactance becomes the limiting factor. Larger ceramic or tantalum capacitors, such as 4.7µF, are recom- mended in place of the 1µF unit mentioned above. Inadequate bypassing is evidenced by reduced output swing and “distorted” clipping effects when the output is driven to the rails. If this is observed, check the supply pins of the device for ripple directly related to the output waveform. Significant supply modulation indicates poor bypassing. Thermal Considerations For the TSSOP16-E package, heat sinking is accomplished by using the heat spreading capabilities of the PC board and its copper traces. Experiments have shown that the heat spreading copper layer does not need to be electri- cally connected to the tab of the device. The PCB material can be very effective at transmitting heat between the pad area attached to the tab of the device, and a ground or power plane layer either inside or on the opposite side of the board. Although the actual thermal resistance of the PCB material is high, the length/area ratio of the thermal Figure 6. Large-Signal Response, CL = 10,000pF RF = RG = 3k RL = ∞ VS = ±15V 1210X F06 |
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