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PLM393LVDR Datasheet(PDF) 17 Page - Texas Instruments

Part # PLM393LVDR
Description  LM393LV-Q1 Dual and LM339LV-Q1 Quad Low Voltage Automotive Comparators
PDF  29 Pages
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Manufacturer  TI1 [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI1 - Texas Instruments

PLM393LVDR Datasheet(HTML) 17 Page - Texas Instruments

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background image
f
1 / 2 R 4
C1 I n2
u
u
CC
2
3
A 2
1
2
3
V
(R IIR )
V
R + R IIR
CC
2
A1
2
1
3
V
R
V
R
R I IR
u
17
LM393LV-Q1
www.ti.com
SNOSDB3 – JUNE 2020
Product Folder Links: LM393LV-Q1
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Copyright © 2020, Texas Instruments Incorporated
Typical Applications (continued)
10.2.2.1 Design Requirements
The square-wave period is determined by the RC time constant of the capacitor C1 and resistor R4. The
maximum frequency is limited by propagation delay of the device and the capacitance load at the output. The low
input bias current allows a lower capacitor value and larger resistor value combination for a given oscillator
frequency, which may help to reduce BOM cost and board space. R4 should be over several kilo-ohms to
minimize loading the output.
10.2.2.2 Detailed Design Procedure
The oscillation frequency is determined by the resistor and capacitor values. The following calculation provides
details of the steps.
Figure 11. Square-Wave Oscillator Timing Thresholds
First consider the output of Figure Figure 10 as high, which indicates the inverted input VC is lower than the
noninverting input (VA). This causes the C1 to be charged through R4, and the voltage VC increases until it is
equal to the noninverting input. The value of VA at the point is calculated by Equation 7.
(7)
if R1 = R2= R3, then VA1 = 2 VCC/ 3
At this time the comparator output trips pulling down the output to the negative rail. The value of VAat this point is
calculated by Equation 8.
(8)
if R1 = R2 = R3, then VA2 = VCC/3
The C1 now discharges though the R4, and the voltage VCC decreases until it reaches VA2. At this point, the
output switches back to the starting state. The oscillation period equals to the time duration from for C1 from
2VCC/3 to VCC / 3 then back to 2VCC/3, which is given by R4C1 × ln 2 for each trip. Therefore, the total time
duration is calculated as 2 R4C1 × ln 2.
The oscillation frequency can be obtained by Equation 9:
(9)
10.2.2.3 Application Curve
Figure 12 shows the simulated results of an oscillator using the following component values:
•
R1 = R2 = R3 = R4 = 100 kΩ
•
C1 = 100 pF, CL = 20 pF
•
V+ = 5 V, V– = GND
•
Cstray (not shown) from VA TO GND = 10 pF



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