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LTC2451 Datasheet(PDF) 13 Page - Linear Technology |
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LTC2451 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 16 page ![]() LTC2451 13 2451fd Figure 11. LTC2451 Input Drive Equivalent Circuit 2. The bandwidth from VSIG is reduced at the input pin. This bandwidth reduction isolates the ADC from high frequency signals, and as such provides simple anti- aliasing and input noise reduction. 3. Switching transients generated by the ADC are attenu- ated before they go back to the signal source. 4. A large CIN gives a better AC ground at the input pin, helping reduce reflections back to the signal source. 5. Increasing RS protects the ADC by limiting the current during an outside-the-rails fault condition. There is a limit to how large RS • CIN should be for a given application. Increasing RS beyond a given point increases the voltage drop across RS due to the input current, to the point that significant measurement errors exist. Additionally, for some applications, increasing the RS• CIN product too much may unacceptably attenuate the signal at frequencies of interest. For most applications, it is desirable to implement CIN as a high quality 0.1 μF ceramic capacitor and RS ≤ 1k. This capacitor should be located as close as possible to the input pin. Furthermore, the area encompassed by this circuit path, as well as the path length, should be minimized. Figure 12. Measured INL vs Input Voltage, CIN = 0.1μF, VCC = 5V, TA = 25°C In the case of a 2-wire sensor that is not remotely grounded, it is desirable to split RS and place series resistors in the ADC input line and in the sensor ground return line, which should be tied to the ADC GND pin using a star connection topology. Figure 12 shows the measured LTC2451 INL versus the input voltage as a function of RS value with an input ca- pacitor CIN = 0.1μF. In some cases, RS can be increased above these guide- lines. The input current is negligible when the ADC is either in sleep or I/O modes. Thus, if the time constant of the input RC circuit τ = RS • CIN, is of the same order of magnitude or longer than the time periods between actual conversions, then one can consider the input current to be reduced correspondingly. These considerations need to be balanced out by the input signal bandwidth. The 3dB bandwidth ≈ 1/(2 πRSCIN). Finally, if the recommended choice for CIN is unacceptable for the user’s specific application, an alternate strategy is to eliminate CIN and minimize CPAR and RS. In practical terms, this configuration corresponds to a low impedance sensor directly connected to the ADC through minimum length Figure 13. Measured INL vs Input Voltage, CIN = 0, VCC = 5V, TA = 25°C APPLICATIONS INFORMATION INPUT VOLTAGE (V) 0 –4 0 4 3 5 2451 F12 –8 –12 –16 12 4 8 12 16 RS = 10k RS = 1k RS = 0 INPUT VOLTAGE (V) 0 8 6 4 2 0 –2 –4 –6 –8 4 2451 F13 123 5 3.5 0.5 1.5 2.5 4.5 RS = 1k RS = 10k RS = 0 VSIG 2451 F11 ILEAK ILEAK RSW 15k (TYP) ICONV CIN IN VCC RS CEQ 0.35pF (TYP) CPAR + – |
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