欢迎访问ic37.com |
会员登录 免费注册
发布采购

ADL5513ACPZ-R2 参数 Datasheet PDF下载

ADL5513ACPZ-R2图片预览
型号: ADL5513ACPZ-R2
PDF下载: 下载PDF文件 查看货源
内容描述: 1 MHz至4 GHz的, 80分贝对数检测器/控制器 [1 MHz to 4 GHz, 80 dB Logarithmic Detector/Controller]
分类和应用: 模拟计算功能信号电路控制器放大器
文件页数/大小: 28 页 / 1283 K
品牌: ADI [ ADI ]
 浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第12页浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第13页浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第14页浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第15页浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第17页浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第18页浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第19页浏览型号ADL5513ACPZ-R2的Datasheet PDF文件第20页  
ADL5513  
Figure 31 shows a plot of the error at 25°C, the temperature at  
which the device is calibrated. Error is not 0 dB over the full  
dynamic range. This is because the log amp does not perfectly  
follow the ideal VOUT vs. PIN equation, even within its operating  
range. The error at the calibrating points of −20 dBm and −40 dBm  
is equal to 0 dB by definition.  
ERROR CALCULATIONS  
The measured transfer function of the ADL5513 at 100 MHz is  
shown in Figure 31. The figure shows plots of measured output  
voltage, calculated error, and an ideal line. The input power and  
output voltage are used to calculate the slope and intercept values.  
The slope and intercept are calculated using linear regression  
over the input range from −40 dBm to −20 dBm. The slope and  
intercept terms are used to generate an ideal line. The error is  
the difference in measured output voltage compared to the ideal  
output line.  
Figure 31 also shows error plots for output voltages measured at  
−40°C and 85°C. These error plots are calculated using slope  
and intercept at 25°C, which is consistent in a mass-production  
environment, where calibration over temperature is not practical.  
This is a measure of the linearity of the device. Error from the  
linear response to the CW waveform is not a measure of absolute  
accuracy because it is calculated using the slope and intercept of  
each device. However, error verifies the linearity of the devices.  
Similarly, at temperature extremes, error represents the output  
voltage variations from the 25°C ideal line performance. Data  
presented in the graphs are the typical error distributions observed  
during characterization of the ADL5513. Device performance  
was optimized for operation at 85°C; this can be changed by  
changing the voltage at TADJ.  
2.4  
2.2  
2.0  
1.8  
1.6  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
3.0  
IDEAL LINE  
2.5  
V
V
V
AND ERROR @ +25°C  
AND ERROR @ –40°C  
AND ERROR @ +85°C  
OUT  
OUT  
OUT  
2.0  
1.5  
1.0  
V
OUT1  
0.5  
0
V
OUT2  
–0.5  
–1.0  
–1.5  
–2.0  
–2.5  
–3.0  
ADJUSTING ACCURACY THROUGH CHOICE OF  
CALIBRATION POINTS  
P
P
IN1  
IN2  
Choose calibration points to suit the specific application, but  
usually they should be in the linear range of the log amp.  
P
(dBm)  
IN  
Figure 31. Typical Output Voltage vs. Input Signal  
In some applications, very high accuracy is required at a reduced  
input range; in other applications, good linearity is necessary over  
the full power input range. The linearity of the transfer function  
can be adjusted by choice of calibration points. Figure 32 and  
Figure 33 show plots for a typical device at 3600 MHz as an exam-  
ple of adjusting accuracy through choice of calibration points.  
The equation for output voltage can be written as  
V
OUT = Slope × (PIN Intercept)  
where:  
Slope is the change in output voltage divided by the change in  
input power, PIN. Slope is expressed in volts per decibel (V/dB).  
Intercept is the calculated power in decibels (dB) at which the  
output voltage is 0 V. Note that VOUT = 0 V can never be achieved.  
2.50  
2.25  
2.00  
1.75  
1.50  
1.25  
1.00  
0.75  
0.50  
0.25  
0
2.5  
2.0  
1.5  
Calibration is performed by applying two known signal levels to  
the ADL 5513 and measuring the corresponding voltage outputs.  
The calibration points are in general chosen to be within the  
linear-in-dB range of the device.  
1.0  
0.5  
0
Calculation of the slope and intercept are accomplished by  
using the following equations:  
–0.5  
–1.0  
–1.5  
–2.0  
–2.5  
+25°C  
–40°C  
+85°C  
+125°C  
VOUT(MEASURED)1 VOUT(MEASURED)2  
Slope   
P
IN1 P  
IN2  
VOUT(MEASURED)  
Slope  
–70 –65 –60 –55 –50 –45 –40 –35 –30 –25 –20 –15 –10 –5  
0
5 10  
Intercept PIN1   
P
(dBm)  
IN  
Figure 32. Typical Device at 3600 MHz, Calibration Points at PIN = −20 dBm  
and −40 dBm  
Once the slope and intercept are calculated, VOUT(IDEAL) can be  
calculated, and the error is determined using the following  
equation:  
(VOUT(MEASURED) VOUT(IDEAL))  
Error   
Slope  
Rev. 0 | Page 16 of 28  
 
 
 
 
 复制成功!