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THS4631 参数 Datasheet PDF下载

THS4631图片预览
型号: THS4631
PDF下载: 下载PDF文件 查看货源
内容描述: 高电压,高压摆率,宽带FET输入运算放大器 [HIGH-VOLTAGE, HIGH SLEW RATE, WIDEBAND FET-INPUT OPERATIONAL AMPLIFIER]
分类和应用: 运算放大器输入元件高压
文件页数/大小: 27 页 / 1287 K
品牌: TI [ TEXAS INSTRUMENTS ]
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THS4631  
www.ti.com  
SLOS451ADECEMBER 2004REVISED MARCH 2005  
SUMMARY OF KEY DECISIONS IN  
TRANSIMPEDANCE DESIGN  
feedback resistors this large or anticipate using an  
external compensation scheme to stabilize the circuit.  
Using a simple capacitor in parallel with the feedback  
resistor makes the amplifier more stable as shown in  
the Typical Characteristics graphs.  
The following is a simplified process for basic  
transimpedance circuit design. This process gives a  
start to the design process, though it does ignore  
some aspects that may be critical to the circuit.  
NOISE ANALYSIS  
STEP 1:  
Determine the capacitance of the  
source.  
High slew rate, unity gain stable, voltage-feedback  
operational amplifiers usually achieve their slew rate  
at the expense of a higher input noise voltage. The  
7 nV/Hz input voltage noise for the THS4631 is,  
however, much lower than comparable amplifiers  
while achieving high slew rates. The input-referred  
voltage noise, and the input-referred current noise  
term, combine to give low output noise under a wide  
variety of operating conditions. Figure 42 shows the  
amplifier noise analysis model with all the noise terms  
included. In this model, all noise terms are taken to  
be noise voltage or current density terms in either  
nV/Hz or fA/Hz.  
STEP 2:  
Calculate the total source capacitance,  
including the amplifier input capaci-  
tance, CI(CM) and CI(DIFF)  
.
STEP 3:  
STEP 4:  
Determine the magnitude of the poss-  
ible current output from the source,  
including the minimum signal current  
anticipated and maximum signal current  
anticipated.  
Choose a feedback resistor value such  
that the input current levels create the  
desired output signal voltages, and  
ensure that the output voltages can  
accommodate the dynamic range of the  
input signal.  
E
NI  
+
_
E
O
R
S
I
BN  
STEP 5:  
STEP 6:  
STEP 7:  
Calculate the optimum feedback capaci-  
tance using Equation 1.  
E
RF  
E
RS  
4kTR  
R
I
S
f
Calculate the bandwidth given the  
resulting component values.  
R
g
4kT  
4kTR  
f
BI  
R
g
Evaluate the circuit to determine if all  
design goals are satisfied.  
4kT = 1.6E−20J  
at 290K  
SELECTION OF FEEDBACK RESISTORS  
Figure 42. Noise Analysis Model  
Feedback resistor selection can have a significant  
effect on the performance of the THS4631 in a given  
application, especially in configurations with low  
closed-loop gain. If the amplifier is configured for  
unity gain, the output should be directly connected to  
the inverting input. Any resistance between these two  
points interacts with the input capacitance of the  
amplifier and causes an additional pole in the fre-  
quency response. For nonunity gain configurations,  
low resistances are desirable for flat frequency re-  
sponse. However, care must be taken not to load the  
amplifier too heavily with the feedback network if  
large output signals are expected. In most cases, a  
trade off is made between the frequency response  
characteristics and the loading of the amplifier. For a  
gain of 2, a 499-feedback resistor is a suitable  
operating point from both perspectives. If resistor  
values are chosen too large, the THS4631 is subject  
to oscillation problems. For example, an inverting  
amplifier configuration with a 5-kgain resistor and a  
5-kfeedback resistor develops an oscillation due to  
the interaction of the large resistors with the input  
capacitance. In low gain configurations, avoid  
The total output noise voltage can be computed as  
the square root of all square output noise voltage  
contributors. Equation 7 shows the general form for  
the output noise voltage using the terms shown in  
Figure 42.  
2
2
ǒ
SǓ2 Ǔ2  
ǒ
) 4kTRS NG ) IBIRf ) 4kTRfNG  
+ Ǹǒ  
Ǔ
EO  
ENI ) IBN  
R
(7)  
Dividing this expression by the noise gain [NG = (1+  
Rf/Rg)] gives the equivalent input-referred spot noise  
voltage at the noninverting input, as shown in  
Equation 8:  
2
IBIRf  
4kTRf  
NG  
2
ǒ
SǓ2  
) 4kTRS )  
Ǹ
ǒ Ǔ )  
NG  
EN +  
ENI ) IBN  
R
(8)  
Using high resistor values can dominate the total  
equivalent input-referred noise. Using 3-kΩ  
a
source-resistance (RS) value adds a voltage noise  
term of approximately 7 nV/Hz. This is equivalent to  
the amplifier voltage noise term. Using higher resistor  
13  
 
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