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CLC4011ITP14MTR 参数 Datasheet PDF下载

CLC4011ITP14MTR图片预览
型号: CLC4011ITP14MTR
PDF下载: 下载PDF文件 查看货源
内容描述: [Low Power, Low Cost, Rail-to-Rail I/O Amplifiers]
分类和应用:
文件页数/大小: 17 页 / 2334 K
品牌: EXAR [ EXAR CORPORATION ]
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CLC2011, CLC4011  
In order to determine P , the power dissipated in the load  
needs to be subtracted from the total power delivered by the  
supplies.  
D
2.5  
2
TSSOP-14  
P = P  
- P  
load  
D
supply  
SOIC-14  
1.5  
1
Supply power is calculated by the standard power equation.  
SOIC-8  
P
supply  
= V  
× I  
supply RMSsupply  
V
= V - V  
S+ S-  
supply  
0.5  
0
MSOP-8  
-20  
Power delivered to a purely resistive load is:  
-40  
0
20  
40  
60  
80  
100  
120  
2
Ambient Temperature (°C)  
P
load  
= ((V  
)
)/Rload  
eff  
load RMS  
Figure 5. Maximum Power Derating  
The effective load resistor (Rload ) will need to include  
eff  
the effect of the feedback network. For instance, Rload in  
Figure 3 would be calculated as:  
eff  
Input Common Mode Voltage  
The common mode input range extends to 250mV below  
ground and to 250mV above Vs, in single supply operation.  
Exceeding these values will not cause phase reversal.  
However, if the input voltage exceeds the rails by more  
than 0.5V, the input ESD devices will begin to conduct. The  
output will stay at the rail during this overdrive condition. If  
the absolute maximum input voltage (700mV beyond either  
rail) is exceeded, externally limit the input current to 5mA  
as shown in Figure 6.  
R || (R + R )  
L
f
g
These measurements are basic and are relatively easy to  
perform with standard lab equipment. For design purposes  
however, prior knowledge of actual signal levels and load  
impedance is needed to determine the dissipated power.  
Here, P can be found from  
D
P = P  
D
+ P  
- P  
Quiescent  
Dynamic load  
10k  
Input  
+
-
Output  
Quiescent power can be derived from the specified I values  
S
along with known supply voltage, V  
. Load power can  
supply  
be calculated as above with the desired signal amplitudes  
using:  
Figure 6. Circuit for Input Current Protection  
(V  
)
= V  
/ √2  
peak  
load RMS  
( I  
)
= ( V  
)
/ Rload  
eff  
load RMS  
load RMS  
Driving Capacitive Loads  
Increased phase delay at the output due to capacitive loading  
can cause ringing, peaking in the frequency response, and  
The dynamic power is focused primarily within the output  
stage driving the load. This value can be calculated as:  
possible unstable behavior. Use a series resistance, R ,  
S
P
= (V - V  
)
× ( I )  
load RMS  
between the amplifier and the load to help improve stability  
and settling performance. Refer to Figure 7.  
Dynamic  
S+  
load RMS  
Assuming the load is referenced in the middle of the power  
rails or V /2.  
Input  
+
-
supply  
Rs  
Output  
CL  
RL  
Rf  
The CLC2011 is short circuit protected. However, this may  
not guarantee that the maximum junction temperature  
(+150°C) is not exceeded under all conditions. Figure 5  
shows the maximum safe power dissipation in the package  
vs. the ambient temperature for the packages available.  
Rg  
Figure 7. Addition of R for Driving Capacitive Loads  
S
© 2009 - 2014 Exar Corporation  
10 / 17  
exar.com/CLC2011  
Rev 1D