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3652

更新时间: 2024-02-05 01:06:09
品牌 Logo 应用领域
德州仪器 - TI 隔离放大器分离技术隔离技术
页数 文件大小 规格书
14页 149K
描述
Optically-Coupled Linear ISOLATION AMPLIFIERS

3652 技术参数

是否Rohs认证: 不符合生命周期:Obsolete
零件包装代码:MODULE包装说明:DIP-32
针数:32Reach Compliance Code:not_compliant
ECCN代码:EAR99HTS代码:8542.33.00.01
风险等级:5.69Is Samacsys:N
放大器类型:ISOLATION AMPLIFIER最大共模电压:2000 V
最小绝缘电压:2000 VJESD-30 代码:R-MDMA-P32
标称负供电电压 (Vsup):-15 V功能数量:1
端子数量:32最高工作温度:85 °C
最低工作温度:封装主体材料:METAL
封装代码:DIP封装等效代码:DIP32,.9
封装形状:RECTANGULAR封装形式:MICROELECTRONIC ASSEMBLY
峰值回流温度(摄氏度):NOT SPECIFIED电源:+-8/+-18 V
认证状态:Not Qualified子类别:Isolation Amplifier
标称供电电压 (Vsup):15 V表面贴装:NO
温度等级:OTHER端子形式:PIN/PEG
端子节距:2.54 mm端子位置:DUAL
处于峰值回流温度下的最长时间:NOT SPECIFIEDBase Number Matches:1

3652 数据手册

 浏览型号3652的Datasheet PDF文件第3页浏览型号3652的Datasheet PDF文件第4页浏览型号3652的Datasheet PDF文件第5页浏览型号3652的Datasheet PDF文件第7页浏览型号3652的Datasheet PDF文件第8页浏览型号3652的Datasheet PDF文件第9页 
NONLINEARITY  
DEFINITIONS  
ISOLATION-MODE VOLTAGE, VISO  
Nonlinearity is specified to be the peak deviation from a best  
straightline expressed as a percent of peak-to-peak full scale  
output (i.e. ±10mV at 20Vp-p 0.05%).  
The isolation-mode voltage is the voltage which appears  
across the isolation barrier, i.e., between the input common  
and the output common. (See Figure 1.)  
Two isolation voltages are given in the electrical specifica-  
tions: “rated continuous” and “test voltage”. Since it is  
impractical on a production basis to test a “continuous”  
voltage (infinite test time is implied), it is a generally  
accepted practice to test at a significantly higher voltage for  
some reasonable length of time. For the 3650 and 3652, the  
“test voltage” is equal to 1000V plus two times the “rated  
continuous” voltage. Thus, for a continuous rating of 2000V,  
each unit is tested at 5000V.  
THEORY OF OPERATION  
Prior to the introduction of the 3650 family optical isolation  
had not been practical in linear circuits. A single LED and  
photodiode combination, while useful in a wide range of  
digital isolation applications, has fundamental limitations—  
primarily nonlinearity and instability as a function of time  
and temperature.  
The 3650 and 3652 use a unique technique to overcome the  
limitations of the single LED and photodiode isolator.  
Figure 2 is an elementary equivalent circuit for the 3650,  
which can be used to understand the basic operation without  
considering the cluttering details of offset adjustment and  
biasing for bipolar operation.  
COMMON-MODE VOLTAGE, VCM  
The common-mode voltage is the voltage midway between  
the two inputs of the amplifier measured with respect to  
input common. It is the algebraic average of the voltage  
applied at the amplifiers’ input terminals. In the circuit in  
Figure 1, (V+ + V)/2 = VCM. (NOTE: Many applications  
involve a large system “common-mode voltage.” Usually in  
such cases the term defined here as “VCM” is negligible and  
the system “common-mode voltage” is applied to the ampli-  
fier as “VISO” in Figure 1.)  
Isolation Barrier  
RK  
CR3  
+V  
CR1  
CR2  
I1  
I2  
+
+VCC  
λ1  
λ2  
RG  
+
I2  
A2  
ISOLATION-MODE REJECTION  
A1  
IIN  
VIN  
I3  
The isolation-mode rejection is defined by the equation in  
Figure 1. The isolation-mode rejection is not infinite be-  
cause there is some leakage across the isolation barrier due  
to the isolation resistance and capacitance.  
VOUT  
–V  
–VCC  
Output Common  
Input Common  
RK  
VOUT = VIN  
RG  
Isolation Barrier  
RG1  
FIGURE 2. Simplified Equivalent Circuit of Linear Isolator.  
+
V+  
Two matched photodiodes are used—one in the input (CR3)  
and one in the output stage (CR2)—to greatly reduce  
nonlinearities and time-temperature instabilities. Amplifier  
A1, LED CR1, and photodiode CR3 are used in a negative  
feedback configuration such that I1 = IIN RG (where RG is the  
user supplied gain setting resistor). Since CR2 and CR3 are  
closely matched, and since they receive equal amounts of  
light from the LED CR1 (i.e., λ1 = λ2), I2 = I1 = IIN. Amplifier  
A2 is connected as a current-to-voltage converter with VOUT  
= I2 RK where RK is an internal 1Mscaling resistor. Thus  
the overall transfer function is:  
RIN  
VD  
RG2  
+
V–  
VOUT  
IL  
VCM  
C
C
(Input)  
(Output)  
VISO  
System  
Ground  
106  
106  
RG1 + RG2 + RIN  
VCM  
VISO  
VOUT = VIN  
, (RG in s)  
VOUT  
=
VD  
+
+
RG  
CMRR  
IMRR  
This improved isolator circuit overcomes the primary  
limitations of the single LED and photodiode combination.  
The transfer function is now virtually independent of any  
degradation in the LED output as long as the two photo-  
diodes and optics are closely matched(1). Linearity is now a  
FIGURE 1. Illustration of Isolation-Mode and Common-  
Mode Specifications.  
NOTE: (1) The only effect of decreased LED output is a slight decrease in full  
scale swing capability. See Typical Performance Curves.  
®
6
3650/52  

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