LMC660_06 [NSC]

CMOS Quad Operational Amplifier; CMOS四路运算放大器
LMC660_06
型号: LMC660_06
厂家: National Semiconductor    National Semiconductor
描述:

CMOS Quad Operational Amplifier
CMOS四路运算放大器

运算放大器
文件: 总14页 (文件大小:874K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
June 2006  
LMC660  
CMOS Quad Operational Amplifier  
n Low input offset voltage: 3 mV  
General Description  
n Low offset voltage drift: 1.3 µV/˚C  
n Ultra low input bias current: 2 fA  
n Input common-mode range includes V−  
n Operating range from +5V to +15.5V supply  
n ISS = 375 µA/amplifier; independent of V+  
n Low distortion: 0.01% at 10 kHz  
n Slew rate: 1.1 V/µs  
The LMC660 CMOS Quad operational amplifier is ideal for  
operation from a single supply. It operates from +5V to  
+15.5V and features rail-to-rail output swing in addition to an  
input common-mode range that includes ground. Perfor-  
mance limitations that have plagued CMOS amplifiers in the  
past are not a problem with this design. Input VOS, drift, and  
broadband noise as well as voltage gain into realistic loads  
(2 kand 600) are all equal to or better than widely  
accepted bipolar equivalents.  
Applications  
This chip is built with National’s advanced Double-Poly  
Silicon-Gate CMOS process.  
n High-impedance buffer or preamplifier  
n Precision current-to-voltage converter  
n Long-term integrator  
See the LMC662 datasheet for a dual CMOS operational  
amplifier with these same features.  
n Sample-and-Hold circuit  
n Peak detector  
n Medical instrumentation  
n Industrial controls  
Features  
n Rail-to-rail output swing  
n Specified for 2 kand 600loads  
n High voltage gain: 126 dB  
n Automotive sensors  
Connection Diagram  
14-Pin SOIC/MDIP  
LMC660 Circuit Topology (Each Amplifier)  
00876704  
00876701  
© 2006 National Semiconductor Corporation  
DS008767  
www.national.com  
Absolute Maximum Ratings (Note 3)  
If Military/Aerospace specified devices are required,  
please contact the National Semiconductor Sales Office/  
Distributors for availability and specifications.  
Power Dissipation  
(Note 2)  
150˚C  
Junction Temperature  
ESD tolerance (Note 8)  
1000V  
Differential Input Voltage  
Supply Voltage  
Output Short Circuit to V+  
Output Short Circuit to V−  
Lead Temperature  
Supply Voltage  
16V  
Operating Ratings  
Temperature Range  
(Note 11)  
(Note 1)  
LMC660AI  
−40˚C TJ +85˚C  
0˚C TJ +70˚C  
4.75V to 15.5V  
(Note 9)  
LMC660C  
Supply Voltage Range  
Power Dissipation  
Thermal Resistance (θJA) (Note 10)  
14-Pin SOIC  
(Soldering, 10 sec.)  
260˚C  
−65˚C to +150˚C  
(V+) + 0.3V, (V) − 0.3V  
18 mA  
Storage Temp. Range  
Voltage at Input/Output Pins  
Current at Output Pin  
Current at Input Pin  
115˚C/W  
85˚C/W  
14-Pin MDIP  
5 mA  
Current at Power Supply Pin  
35 mA  
DC Electrical Characteristics  
Unless otherwise specified, all limits guaranteed for TJ = 25˚C. Boldface limits apply at the temperature extremes. V+ = 5V,  
V= 0V, VCM = 1.5V, VO = 2.5V and RL 1Munless otherwise specified.  
>
Parameter  
Conditions  
Typ  
LMC660AI  
LMC660C  
Units  
(Note 4)  
Limit  
(Note 4)  
3
Limit  
(Note 4)  
6
Input Offset Voltage  
1
mV  
max  
3.3  
6.3  
Input Offset Voltage  
Average Drift  
1.3  
µV/˚C  
Input Bias Current  
0.002  
0.001  
pA  
max  
pA  
4
2
2
1
Input Offset Current  
max  
TeraΩ  
dB  
>
Input Resistance  
Common Mode  
1
0V VCM 12.0V  
V+ = 15V  
5V V+ 15V  
83  
70  
68  
63  
62  
Rejection Ratio  
min  
dB  
Positive Power Supply  
Rejection Ratio  
83  
70  
63  
VO = 2.5V  
0V V−10V  
68  
62  
min  
dB  
Negative Power Supply  
Rejection Ratio  
94  
84  
74  
83  
73  
min  
V
Input Common-Mode  
Voltage Range  
V+ = 5V & 15V  
−0.4  
V+ − 1.9  
2000  
500  
−0.1  
−0.1  
For CMRR 50 dB  
0
0
max  
V
V+ − 2.3  
V+ − 2.5  
440  
400  
180  
120  
220  
200  
100  
60  
V+ − 2.3  
V+ − 2.4  
300  
200  
90  
min  
V/mV  
min  
V/mV  
min  
V/mV  
min  
V/mV  
min  
Large Signal  
Voltage Gain  
RL = 2 k(Note 5)  
Sourcing  
Sinking  
80  
RL = 600(Note 5)  
Sourcing  
1000  
250  
150  
100  
50  
Sinking  
40  
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2
DC Electrical Characteristics (Continued)  
Unless otherwise specified, all limits guaranteed for TJ = 25˚C. Boldface limits apply at the temperature extremes. V+ = 5V,  
V= 0V, VCM = 1.5V, VO = 2.5V and RL 1Munless otherwise specified.  
>
Parameter  
Conditions  
Typ  
LMC660AI  
LMC660C  
Units  
(Note 4)  
Limit  
(Note 4)  
4.82  
4.79  
0.15  
0.17  
4.41  
4.31  
0.50  
0.56  
14.50  
14.44  
0.35  
0.40  
13.35  
13.15  
1.16  
1.32  
16  
Limit  
(Note 4)  
4.78  
4.76  
0.19  
0.21  
4.27  
4.21  
0.63  
0.69  
14.37  
14.32  
0.44  
0.48  
12.92  
12.76  
1.45  
1.58  
13  
Output Swing  
V+ = 5V  
RL = 2 kto V+/2  
4.87  
0.10  
4.61  
0.30  
14.63  
0.26  
13.90  
0.79  
22  
V
min  
V
max  
V
V+ = 5V  
RL = 600to V+/2  
min  
V
max  
V
V+ = 15V  
RL = 2 kto V+/2  
min  
V
max  
V
V+ = 15V  
RL = 600to V+/2  
min  
V
max  
mA  
min  
mA  
min  
mA  
min  
mA  
min  
mA  
max  
Output Current  
V+ = 5V  
Sourcing, VO = 0V  
Sinking, VO = 5V  
Sourcing, VO = 0V  
14  
11  
21  
16  
13  
14  
11  
Output Current  
V+ = 15V  
40  
28  
23  
25  
21  
Sinking, VO = 13V  
(Note 11)  
39  
28  
23  
24  
20  
Supply Current  
All Four Amplifiers  
VO = 1.5V  
1.5  
2.2  
2.7  
2.6  
2.9  
AC Electrical Characteristics  
Unless otherwise specified, all limits guaranteed for TJ = 25˚C. Boldface limits apply at the temperature extremes. V+ = 5V,  
V= 0V, VCM = 1.5V, VO = 2.5V and RL 1Munless otherwise specified.  
>
Parameter  
Conditions  
Typ  
LMC660AI  
LMC660C  
Units  
(Note 4)  
Limit  
(Note 4)  
0.8  
Limit  
(Note 4)  
0.8  
Slew Rate  
(Note 6)  
1.1  
V/µs  
min  
MHz  
Deg  
dB  
0.6  
0.7  
Gain-Bandwidth Product  
Phase Margin  
1.4  
50  
Gain Margin  
17  
Amp-to-Amp Isolation  
Input Referred Voltage Noise  
(Note 7)  
130  
22  
dB  
F = 1 kHz  
Input Referred Current Noise  
f = 1 kHz  
0.0002  
3
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AC Electrical Characteristics (Continued)  
Unless otherwise specified, all limits guaranteed for TJ = 25˚C. Boldface limits apply at the temperature extremes. V+ = 5V,  
V= 0V, VCM = 1.5V, VO = 2.5V and RL 1Munless otherwise specified.  
>
Parameter  
Conditions  
Typ  
LMC660AI  
LMC660C  
Units  
(Note 4)  
Limit  
Limit  
(Note 4)  
(Note 4)  
Total Harmonic Distortion  
f = 10 kHz, AV  
= −10  
0.01  
%
RL = 2 k, VO  
= 8 VPP  
V+ = 15V  
Note 1: Applies to both single supply and split supply operation. Continuous short circuit operation at elevated ambient temperature and/or multiple Op Amp shorts  
can result in exceeding the maximum allowed junction temperature of 150˚C. Output currents in excess of 30 mA over long term may adversely affect reliability.  
Note 2: The maximum power dissipation is a function of T  
, θ , and T . The maximum allowable power dissipation at any ambient temperature is P =  
A D  
J(MAX) JA  
(T  
− T )/θ .  
J(MAX)  
A JA  
Note 3: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is  
intended to be functional, but do not guarantee specific performance limits. For guaranteed specifications and test conditions, see the Electrical Characteristics. The  
guaranteed specifications apply only for the test conditions listed.  
Note 4: Typical values represent the most likely parametric norm. Limits are guaranteed by testing or correlation.  
+
Note 5: V = 15V, V  
= 7.5V and R connected to 7.5V. For Sourcing tests, 7.5V V 11.5V. For Sinking tests, 2.5V V 7.5V.  
L O O  
CM  
+
Note 6: V = 15V. Connected as Voltage Follower with 10V step input. Number specified is the slower of the positive and negative slew rates.  
+
+
Note 7: Input referred. V = 15V and R = 10 kconnected to V /2. Each amp excited in turn with 1 kHz to produce V = 13 V  
.
L
O
PP  
Note 8: Human Body Model is 1.5 kin series with 100 pF.  
Note 9: For operating at elevated temperatures the device must be derated based on the thermal resistance θ with P = (T − T )/θ .  
JA  
JA  
D
J
A
Note 10: All numbers apply for packages soldered directly into a PC board.  
+
+
Note 11: Do not connect output to V when V is greater than 13V or reliability may be adversely affected.  
Ordering Information  
Package  
Temperature Range  
Transport  
Media  
NSC  
Drawing  
Industrial  
Commercial  
0˚C to +70˚C  
LMC660CM  
LMC660CMX  
−40˚C to +85˚C  
LMC660AIM  
14-Pin  
SOIC  
Rail  
M14A  
N14A  
LMC660AIMX  
Tape and Reel  
14-Pin  
M DIP  
LMC660AIN  
LMC660CN  
Rail  
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4
Typical Performance Characteristics VS  
=
7.5V, TA = 25˚C unless otherwise specified.  
Supply Current vs. Supply Voltage  
Offset Voltage  
00876725  
00876724  
Input Bias Current  
Output Characteristics Current Sinking  
00876726  
00876727  
Output Characteristics Current Sourcing  
Input Voltage Noise vs. Frequency  
00876728  
00876729  
5
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Typical Performance Characteristics VS  
=
7.5V, TA = 25˚C unless otherwise specified. (Continued)  
CMRR vs. Frequency  
Open-Loop Frequency Response  
00876730  
00876731  
Frequency Response vs. Capacitive Load  
Non-Inverting Large Signal Pulse Response  
00876733  
00876732  
Stability vs. Capacitive Load  
Stability vs. Capacitive Load  
00876734  
00876735  
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6
Application Hints  
AMPLIFIER TOPOLOGY  
etc., and RP is the parallel combination of RF and RIN. This  
formula, as well as all formulae derived below, apply to  
inverting and non-inverting op amp configurations.  
The topology chosen for the LMC660, shown in Figure 1, is  
unconventional (compared to general-purpose op amps) in  
that the traditional unity-gain buffer output stage is not used;  
instead, the output is taken directly from the output of the  
integrator, to allow rail-to-rail output swing. Since the buffer  
traditionally delivers the power to the load, while maintaining  
high op amp gain and stability, and must withstand shorts to  
either rail, these tasks now fall to the integrator.  
When the feedback resistors are smaller than a few k, the  
frequency of the feedback pole will be quite high, since CS is  
generally less than 10 pF. If the frequency of the feedback  
pole is much higher than the “ideal” closed-loop bandwidth  
(the nominal closed-loop bandwidth in the absence of CS),  
the pole will have a negligible effect on stability, as it will add  
only a small amount of phase shift.  
As a result of these demands, the integrator is a compound  
affair with an embedded gain stage that is doubly fed forward  
(via Cf and Cff) by a dedicated unity-gain compensation  
driver. In addition, the output portion of the integrator is a  
push-pull configuration for delivering heavy loads. While  
sinking current the whole amplifier path consists of three  
gain stages with one stage fed forward, whereas while  
sourcing the path contains four gain stages with two fed  
forward.  
However, if the feedback pole is less than approximately 6 to  
10 times the “ideal” −3 dB frequency, a feedback capacitor,  
CF, should be connected between the output and the invert-  
ing input of the op amp. This condition can also be stated in  
terms of the amplifier’s low-frequency noise gain: To main-  
tain stability a feedback capacitor will probably be needed if  
where  
is the amplifier’s low-frequency noise gain and GBW is the  
amplifier’s gain bandwidth product. An amplifier’s low-  
frequency noise gain is represented by the formula  
00876704  
FIGURE 1. LMC660 Circuit Topology (Each Amplifier)  
regardless of whether the amplifier is being used in inverting  
or non-inverting mode. Note that a feedback capacitor is  
more likely to be needed when the noise gain is low and/or  
the feedback resistor is large.  
The large signal voltage gain while sourcing is comparable  
to traditional bipolar op amps, even with a 600load. The  
gain while sinking is higher than most CMOS op amps, due  
to the additional gain stage; however, under heavy load  
(600) the gain will be reduced as indicated in the Electrical  
Characteristics. Avoid resistive loads of less than 500, as  
they may cause instability.  
If the above condition is met (indicating a feedback capacitor  
will probably be needed), and the noise gain is large enough  
that:  
COMPENSATING INPUT CAPACITANCE  
The high input resistance of the LMC660 op amps allows the  
use of large feedback and source resistor values without  
losing gain accuracy due to loading. However, the circuit will  
be especially sensitive to its layout when these large-value  
resistors are used.  
the following value of feedback capacitor is recommended:  
Every amplifier has some capacitance between each input  
and AC ground, and also some differential capacitance be-  
tween the inputs. When the feedback network around an  
amplifier is resistive, this input capacitance (along with any  
additional capacitance due to circuit board traces, the  
socket, etc.) and the feedback resistors create a pole in the  
feedback path. In the following General Operational Amplifier  
circuit,Figure 2 the frequency of this pole is  
If  
the feedback capacitor should be:  
where CS is the total capacitance at the inverting input,  
including amplifier input capacitance and any stray capaci-  
tance from the IC socket (if one is used), circuit board traces,  
7
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Application Hints (Continued)  
Note that these capacitor values are usually significant  
smaller than those given by the older, more conservative  
formula:  
00876705  
FIGURE 3. Rx, Cx Improve Capacitive Load Tolerance  
Capacitive load driving capability is enhanced by using a pull  
up resistor to V+ (Figure 4). Typically a pull up resistor  
conducting 500 µA or more will significantly improve capaci-  
tive load responses. The value of the pull up resistor must be  
determined based on the current sinking capability of the  
amplifier with respect to the desired output swing. Open loop  
gain of the amplifier can also be affected by the pull up  
resistor (see Electrical Characteristics).  
00876706  
C
consists of the amplifier’s input capacitance plus any stray capacitance  
from the circuit board and socket. C compensates for the pole caused by  
S
F
C
and the feedback resistors.  
S
FIGURE 2. General Operational Amplifier Circuit  
Using the smaller capacitors will give much higher band-  
width with little degradation of transient response. It may be  
necessary in any of the above cases to use a somewhat  
larger feedback capacitor to allow for unexpected stray ca-  
pacitance, or to tolerate additional phase shifts in the loop, or  
excessive capacitive load, or to decrease the noise or band-  
width, or simply because the particular circuit implementa-  
tion needs more feedback capacitance to be sufficiently  
stable. For example, a printed circuit board’s stray capaci-  
tance may be larger or smaller than the breadboard’s, so the  
actual optimum value for CF may be different from the one  
estimated using the breadboard. In most cases, the values  
of CF should be checked on the actual circuit, starting with  
the computed value.  
00876723  
FIGURE 4. Compensating for Large Capacitive Loads  
with a Pull Up Resistor  
PRINTED-CIRCUIT-BOARD LAYOUT  
FOR HIGH-IMPEDANCE WORK  
It is generally recognized that any circuit which must operate  
with less than 1000 pA of leakage current requires special  
layout of the PC board. When one wishes to take advantage  
of the ultra-low bias current of the LMC662, typically less  
than 0.04 pA, it is essential to have an excellent layout.  
Fortunately, the techniques for obtaining low leakages are  
quite simple. First, the user must not ignore the surface  
leakage of the PC board, even though it may sometimes  
appear acceptably low, because under conditions of high  
humidity or dust or contamination, the surface leakage will  
be appreciable.  
CAPACITIVE LOAD TOLERANCE  
Like many other op amps, the LMC660 may oscillate when  
its applied load appears capacitive. The threshold of oscilla-  
tion varies both with load and circuit gain. The configuration  
most sensitive to oscillation is a unity-gain follower. See  
Typical Performance Characteristics.  
The load capacitance interacts with the op amp’s output  
resistance to create an additional pole. If this pole frequency  
is sufficiently low, it will degrade the op amp’s phase margin  
so that the amplifier is no longer stable at low gains. As  
shown in Figure 3, the addition of a small resistor (50to  
100) in series with the op amp’s output, and a capacitor (5  
pF to 10 pF) from inverting input to output pins, returns the  
phase margin to a safe value without interfering with lower-  
frequency circuit operation. Thus larger values of capaci-  
tance can be tolerated without oscillation. Note that in all  
cases, the output will ring heavily when the load capacitance  
is near the threshold for oscillation.  
To minimize the effect of any surface leakage, lay out a ring  
of foil completely surrounding the LMC660’s inputs and the  
terminals of capacitors, diodes, conductors, resistors, relay  
terminals, etc. connected to the op amp’s inputs. SeeFigure  
5. To have a significant effect, guard rings should be placed  
on both the top and bottom of the PC board. This PC foil  
must then be connected to a voltage which is at the same  
voltage as the amplifier inputs, since no leakage current can  
flow between two points at the same potential. For example,  
a PC board trace-to-pad resistance of 1012, which is nor-  
mally considered a very large resistance, could leak 5 pA if  
the trace were a 5V bus adjacent to the pad of an input. This  
would cause a 100 times degradation from the LMC660’s  
actual performance. However, if a guard ring is held within  
5 mV of the inputs, then even a resistance of 1011would  
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8
Application Hints (Continued)  
cause only 0.05 pA of leakage current, or perhaps a minor  
(2:1) degradation of the amplifier’s performance. See Figure  
6a,Figure 6b, Figure 6c for typical connections of guard rings  
for standard op amp configurations. If both inputs are active  
and at high impedance, the guard can be tied to ground and  
still provide some protection; see Figure 6d.  
00876717  
(a) Inverting Amplifier  
00876718  
(b) Non-Inverting Amplifier  
00876716  
FIGURE 5. Example, using the LMC660,  
of Guard Ring in P.C. Board Layout  
00876719  
(c) Follower  
00876720  
(d) Howland Current Pump  
FIGURE 6. Guard Ring Connections  
The designer should be aware that when it is inappropriate  
to lay out a PC board for the sake of just a few circuits, there  
is another technique which is even better than a guard ring  
on a PC board: Don’t insert the amplifier’s input pin into the  
board at all, but bend it up in the air and use only air as an  
insulator. Air is an excellent insulator. In this case you may  
have to forego some of the advantages of PC board con-  
struction, but the advantages are sometimes well worth the  
effort of using point-to-point up-in-the-air wiring. See Figure  
7.  
9
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Application Hints (Continued)  
A suitable capacitor for C2 would be a 5 pF or 10 pF silver  
mica, NPO ceramic, or air-dielectric. When determining the  
magnitude of Ib−, the leakage of the capacitor and socket  
must be taken into account. Switch S2 should be left shorted  
most of the time, or else the dielectric absorption of the  
capacitor C2 could cause errors.  
Similarly, if S1 is shorted momentarily (while leaving S2  
shorted)  
where Cx is the stray capacitance at the + input.  
00876721  
(Input pins are lifted out of PC board and soldered directly to components.  
All other pins connected to PC board.)  
FIGURE 7. Air Wiring  
BIAS CURRENT TESTING  
The test method of Figure 7 is appropriate for bench-testing  
bias current with reasonable accuracy. To understand its  
operation, first close switch S2 momentarily. When S2 is  
opened, then  
00876722  
FIGURE 8. Simple Input Bias Current Test Circuit  
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10  
Typical Single-Supply Applications  
(V+ = 5.0 VDC)  
Sine-Wave Oscillator  
Additional single-supply applications ideas can be found in  
the LM324 datasheet. The LMC660 is pin-for-pin compatible  
with the LM324 and offers greater bandwidth and input  
resistance over the LM324. These features will improve the  
performance of many existing single-supply applications.  
Note, however, that the supply voltage range of the LMC660  
is smaller than that of the LM324.  
Low-Leakage Sample-and-Hold  
00876709  
00876707  
Oscillator frequency is determined by R1, R2, C1, and C2:  
fosc = 1/2πRC, where R = R1 = R2 and  
C = C1 = C2.  
Instrumentation Amplifier  
This circuit, as shown, oscillates at 2.0 kHz with a peak-to-  
peak output swing of 4.5V.  
1 Hz Square-Wave Oscillator  
00876708  
If R1 = R5, R3 = R6, and R4 = R7; then  
00876710  
Power Amplifier  
AV 100 for circuit shown.  
For good CMRR over temperature, low drift resistors should  
be used. Matching of R3 to R6 and R4 to R7 affect CMRR.  
Gain may be adjusted through R2. CMRR may be adjusted  
through R7.  
00876711  
11  
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Typical Single-Supply Applications  
High Gain Amplifier with Offset  
Voltage Reduction  
(V+ = 5.0 VDC) (Continued)  
10 Hz Bandpass Filter  
00876712  
f
O
= 10 Hz  
Q = 2.1  
Gain = −8.8  
00876715  
10 Hz High-Pass Filter  
Gain = −46.8  
Output offset voltage reduced to the level of the input offset voltage of the  
bottom amplifier (typically 1 mV).  
00876713  
f
= 10 Hz  
c
d = 0.895  
Gain = 1  
2 dB passband ripple  
1 Hz Low-Pass Filter  
(Maximally Flat, Dual Supply Only)  
00876714  
f
= 1 Hz  
c
d = 1.414  
Gain = 1.57  
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12  
Physical Dimensions inches (millimeters) unless otherwise noted  
14-Pin SOIC  
NS Package Number M14A  
14-Pin MDIP  
NS Package Number N14A  
13  
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Notes  
National does not assume any responsibility for use of any circuitry described, no circuit patent licenses are implied and National reserves  
the right at any time without notice to change said circuitry and specifications.  
For the most current product information visit us at www.national.com.  
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