SNOS998I February 2002 – October 2015 LMV761 , LMV762 , LMV762Q-Q1

PRODUCTION DATA.

- 1 Features
- 2 Applications
- 3 Description
- 4 Revision History
- 5 Pin Configuration and Functions
- 6 Specifications
- 6.1 Absolute Maximum Ratings
- 6.2 ESD Ratings: LMV761, LMV762
- 6.3 ESD Ratings: LMV762Q-Q1
- 6.4 Recommended Operating Conditions
- 6.5 Thermal Information
- 6.6 2.7-V Electrical Characteristics
- 6.7 5-V Electrical Characteristics
- 6.8 2-V Switching Characteristics
- 6.9 5-V Switching Characteristics
- 6.10Typical Characteristics

- 7 Detailed Description
- 8 Application and Implementation
- 9 Power Supply Recommendations
- 10Layout
- 11Device and Documentation Support
- 12Mechanical, Packaging, and Orderable Information

NOTE

Information in the following applications sections is not part of the TI component specification, and TI does not warrant its accuracy or completeness. TI’s customers are responsible for determining suitability of components for their purposes. Customers should validate and test their design implementation to confirm system functionality.

The LMV76x are single-supply comparators with 120 ns of propagation delay and 300 µA of supply current.

A typical application for a LMV76x comparator is a programmable square-wave oscillator.

The circuit in Figure 23 generates a square wave whose period is set by the RC time constant of the capacitor C_{1} and resistor R_{4}. V^{+} = 5 V unless otherwise specified.

The maximum frequency is limited by the large signal propagation delay of the comparator and by the capacitive loading at the output, which limits the output slew rate.

Consider the output of Figure 23 is high to analyze the circuit. That implies that the inverted input (V_{C}) is lower than the noninverting input (V_{A}). This causes the C_{1} to be charged through R_{4}, and the voltage V_{C} increases until it is equal to the noninverting input. The value of V_{A} at this point is calculated by Equation 4:

Equation 4.

If R_{1} = R_{2} = R_{3}, then V_{A1} = 2 V_{CC} / 3

At this point the comparator switches pulling down the output to the negative rail. The value of V_{A} at this point is calculated by Equation 5:

Equation 5.

If R_{1} = R_{2} = R_{3}, then V_{A2} = V_{CC} / 3.

The capacitor C_{1} now discharges through R_{4}, and the voltage V_{C} decreases until it is equal to V_{A2}, at which point the comparator switches again, bringing it back to the initial stage. The time period is equal to twice the time it takes to discharge C_{1} from 2 V_{CC} / 3 to V_{CC} / 3, which is given by R_{4}C_{1} × ln2. Hence, the formula for the frequency is calculated by Equation 6:

Equation 6. F = 1 / (2 × R_{4} × C_{1} × ln2)

Figure Figure 25 shows the simulated results of an oscillator using the following values:

- R
_{1}= R_{2}= R_{3}= R_{4}= 100 kΩ - C
_{1}= 100 pF, C_{L}= 20 pF - V+ = 5 V, V– = GND
- C
_{STRAY}(not shown) from V_{a}to GND = 10 pF