LMC7211BIM5/NOPB National Semiconductor, LMC7211BIM5/NOPB Datasheet - Page 9

IC COMPAR TINY R-R CMOS SOT23-5

LMC7211BIM5/NOPB

Manufacturer Part Number
LMC7211BIM5/NOPB
Description
IC COMPAR TINY R-R CMOS SOT23-5
Manufacturer
National Semiconductor
Type
General Purposer
Datasheet

Specifications of LMC7211BIM5/NOPB

Number Of Elements
1
Output Type
Push-Pull
Voltage - Supply
2.7 V ~ 15 V, ±1.35 V ~ 7.5 V
Mounting Type
Surface Mount
Package / Case
SC-74A, SOT-753
Comparator Type
General Purpose
No. Of Comparators
1
Response Time
4µs
Ic Output Type
Push Pull
Supply Current
18µA
Supply Voltage Range
2.7V To 15V
Amplifier Case Style
SOT-23
Rohs Compliant
Yes
Number Of Elements
1
Technology
CMOS
Input Offset Voltage
15mV
Input Bias Current (typ)
40pA
Single Supply Voltage (typ)
3/5/9/12V
Dual Supply Voltage (typ)
Not RequiredV
Supply Current (max)
0.014@15VmA
Power Supply Requirement
Single
Common Mode Rejection Ratio
75dB
Voltage Gain In Db
100dB
Power Supply Rejection Ratio
80dB
Single Supply Voltage (min)
2.7V
Single Supply Voltage (max)
15V
Dual Supply Voltage (min)
Not RequiredV
Dual Supply Voltage (max)
Not RequiredV
Operating Temp Range
-40C to 85C
Operating Temperature Classification
Industrial
Mounting
Surface Mount
Pin Count
5
Package Type
SOT-23
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Other names
LMC7211BIM5
LMC7211BIM5TR

Available stocks

Company
Part Number
Manufacturer
Quantity
Price
Part Number:
LMC7211BIM5/NOPB
Manufacturer:
NS/国半
Quantity:
20 000
FIGURE 1. Even at Low-Supply Voltage of 2.7V, an Input
Signal which Exceeds the Supply Voltages Produces No
At V
μs with overdrives of 100 mV.
Please refer to the performance curves for more extensive
characterization.
3.0 Shoot-Through Current
The shoot-through current is defined as the current surge,
above the quiescent supply current, between the positive and
negative supplies of a device. The current surge occurs when
the output of the device switches states. The shoot-through
current results in glitches in the supply voltages. Usually,
glitches in the supply lines are prevented by bypass capaci-
tors. When the glitches are minimal, the value of the bypass
capacitors can be reduced.
+
= 2.7V propagation delays are t
FIGURE 2. Circuit for Measurement of the
Phase Inversion at the Output
Shoot-Through Current
PLH
= 4 μs and t
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PHL
= 4
9
From
can be calculated to be 0.2 mA (typical), and the duration is
1 μs. The values needed for the bypass capacitors can be
calculated as follows:
Area of Δ
The capacitor needs to supply 100 picocolumb. To avoid large
shifts in the comparator threshold due to changes in the volt-
age level, the voltage drop at the bypass capacitor should be
limited to 100 mV or less.
The charge needed (100 picocolumb) and the allowable volt-
age drop (100 mV) will give us the minimum capacitor value
required.
ΔQ
The voltage drop of
the comparator. This threshold shift will be reduced by the
power supply rejection ratio, (PSRR). The PSRR which is ap-
plicable here is not the DC value of PSRR (
transient PSRR which will be usually about 20 dB–40 dB, de-
pending on the circuit and the speed of the transient. This will
result in an effective threshold shift of about 1 mV to 10 mV.
For precision and level sensing circuits, it is generally a good
goal to reduce the voltage delta on the power supply to a value
equal to or less than the hysteresis of the comparator circuit.
If the above circuit was to be used with 50 mV of hysteresis,
it would be reasonable to increase the bypass capacitor to
0.01 μF to reduce the voltage delta to 10 mV. Larger values
may be useful for obtaining more accurate and consistent
switching.
Note that the switching current of the comparator can spread
to other parts of the board as noise. The bypass capacitor
reduces this noise. For low noise systems this may be reason
to make the capacitor larger.
FIGURE 3. Measurement of the Shoot-Through Current
Figure
= C (ΔV)
C = ΔQ/ΔV = 100 picocolumb/100 mV
C = 10
10
-9
= 1 nF = 0.001 μF
-10
3, the shoot-through current for the LMC7211
/10
-1
= ½ (1 μs × 200 μA)
= 100 pC
= 10
100 mV will cause a threshold shift in
-9
= 1 nF = 0.001 μF
80 dB), but a
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1233707
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