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AU2902

更新时间： 2024-02-10 11:12:10
品牌 Logo 应用领域
恩智浦 - NXP 运算放大器
页数 文件大小 规格书
10页 103K
描述
Low power quad operational amplifier

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AU2902 技术参数

是否Rohs认证： 不符合生命周期：Transferred
包装说明：DIP, DIP14,.3Reach Compliance Code：unknown
风险等级：5.87Is Samacsys：N
放大器类型：OPERATIONAL AMPLIFIER架构：VOLTAGE-FEEDBACK
25C 时的最大偏置电流 (IIB)：0.25 µA频率补偿：YES
最大输入失调电压：9000 µVJESD-30 代码：R-PDIP-T14
JESD-609代码：e0低-失调：NO
微功率：YES功能数量：4
端子数量：14最高工作温度：125 °C
最低工作温度：-40 °C封装主体材料：PLASTIC/EPOXY
封装代码：DIP封装等效代码：DIP14,.3
封装形状：RECTANGULAR封装形式：IN-LINE
电源：5/30 V认证状态：Not Qualified
子类别：Operational Amplifiers最大压摆率：3 mA
供电电压上限：16 V表面贴装：NO
技术：BIPOLAR温度等级：AUTOMOTIVE
端子面层：Tin/Lead (Sn/Pb)端子形式：THROUGH-HOLE
端子节距：2.54 mm端子位置：DUAL
最小电压增益：15000Base Number Matches：1

AU2902 数据手册

 浏览型号AU2902的Datasheet PDF文件第1页浏览型号AU2902的Datasheet PDF文件第2页浏览型号AU2902的Datasheet PDF文件第3页浏览型号AU2902的Datasheet PDF文件第5页浏览型号AU2902的Datasheet PDF文件第6页浏览型号AU2902的Datasheet PDF文件第7页 
Philips Semiconductors  
Product data  
Low power quad operational amplifier  
AU2902  
DC ELECTRICAL CHARACTERISTICS  
V
CC  
= 5 V; T  
= 25 °C; unless otherwise specified.  
amb  
AU2902  
Typ  
SYMBOL  
PARAMETER  
TEST CONDITIONS  
= 0 Ω  
UNIT  
Min  
Max  
R
±2  
±3  
±5  
mV  
mV  
µV/°C  
nA  
S
1
V
OS  
Offset voltage  
R
R
= 0 Ω, over temp.  
= 0 Ω, over temp.  
S
S
∆V /∆T  
Temperature drift  
7
OS  
I
IN  
(+) or I (–)  
45  
40  
50  
±5  
250  
500  
IN  
2
I
Input current  
BIAS  
I
(+) or I (–); over temp.  
nA  
IN  
IN  
∆I  
BIAS  
/∆T  
Temperature drift  
Offset current  
Over temp.  
pA/°C  
nA  
I
IN  
(+)–I (–)  
±50  
IN  
I
OS  
I
(+) – I (–); over temp.  
±150  
nA  
IN  
IN  
∆I /∆T  
Temperature drift  
Over temp.  
10  
70  
pA/°C  
V
OS  
V
CC  
≤ 30 V  
0
V
– 1.5  
CC  
3
V
CM  
Common-mode voltage range  
V
CC  
≤ 30 V; over temp.  
0
V
– 2  
V
CC  
CMRR  
Common-mode rejection ratio  
Output voltage swing  
Output voltage high  
V
CC  
= 30 V  
65  
26  
27  
dB  
V
OUT  
V
OH  
V
OL  
R = 2 kΩ; V = 30 V; over temp.  
V
L
CC  
R ≥ 10 kΩ; V = 30 V; over temp.  
28  
5
V
L
CC  
Output voltage low  
R ≤ 10 kΩ; V = 5 V; over temp.  
20  
mV  
mA  
mA  
L
CC  
R = ∞; V = 30 V; over temp.  
1.5  
0.7  
3
L
CC  
I
Supply current  
CC  
R = ∞; V = 5 V; over temp.  
1.2  
L
CC  
V
= 15 V (for large V swing);  
O
CC  
25  
15  
100  
V/mV  
V/mV  
R ≥ 2 kΩ  
L
A
VOL  
Large-signal voltage gain  
V
= 15V (for large V swing);  
O
R ≥ 2 kΩ; over temp.  
L
CC  
5
Amplifier-to-amplifier coupling  
f = 1 kHz to 20 kHz; input referred  
= 0 Ω  
–120  
100  
40  
dB  
dB  
PSRR  
Power supply rejection ratio  
R
65  
20  
S
V
IN  
+ = +1 V; V – = 0 V; V = 15 V  
mA  
IN  
CC  
Output current,  
Source  
V
IN  
+ = +1 V; V – = 0 V; V = 15 V;  
IN  
CC  
10  
10  
5
20  
20  
8
mA  
mA  
mA  
over temp.  
V
IN  
– = +1 V, V + = 0 V; V+ = 15 V  
IN  
I
OUT  
V
IN  
– = +1 V; V + = 0 V; V = 15 V;  
Output current,  
Sink  
IN  
CC  
over temp.  
V
IN  
– = +1 V; V + = 0 V; V = 200 mV  
12  
10  
50  
40  
µA  
mA  
IN  
O
4
I
Short–circuit current  
60  
SC  
3
V
Differential input voltage  
Unity gain bandwidth  
Slew rate  
V
CC  
V
DIFF  
GBW  
SR  
1
MHz  
V/µs  
nV/√Hz  
0.3  
40  
V
NOISE  
Input noise voltage  
f = 1 kHz  
NOTES:  
1. V ≈ 1.4 V , R = 0 Ω with V from 5 V to 30 V and over full input common-mode range (0 V + to V –1.5 V).  
O
DC  
S
CC  
DC  
CC  
2. The direction of the input current is out of the IC due to the PNP input stage. This current is essentially constant, independent of the state of  
the output so no loading change exists on the input lines.  
3. The input common-mode voltage or either input signal voltage should not be allowed to go negative by more than 0.3 V. The upper end of  
the common-mode voltage range is V –1.5, but either or both inputs can go to +32 V without damage.  
CC  
4. Short-circuits from the output to V can cause excessive heating and eventual destruction. The maximum output current is approximately  
CC  
40 mA independent of the magnitude of V . At values of supply voltage in excess of +15 V , continuous short-circuits can exceed the  
CC  
DC  
power dissipation ratings and cause eventual destruction. Destructive dissipation can result from simultaneous shorts on all amplifiers.  
5. Due to proximity of external components, insure that coupling is not originating via stray capacitance between these external parts. This  
typically can be detected as this type of coupling increases at higher frequencies.  
4
2001 Aug 03  
1234567...10

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