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5962-9559801MRA 参数 Datasheet PDF下载

5962-9559801MRA图片预览
型号: 5962-9559801MRA
PDF下载: 下载PDF文件 查看货源
内容描述: 250 MHz的解调对数放大器 [250 MHz Demodulating Logarithmic Amplifier]
分类和应用: 放大器
文件页数/大小: 16 页 / 259 K
品牌: ADI [ ADI ]
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AD641  
2.5  
2.0  
1.5  
1.0  
Transistors Q3 through Q6 form the full wave detector, whose  
output is buffered by the cascodes Q9 and Q10. For zero input  
Q3 and Q5 conduct only a small amount (a total of about 32 µA)  
of the 565 µA tail currents supplied to pairs Q3–Q4 and Q5–Q6.  
This “pedestal” current flows in output cascode Q9 to the LOG  
OUT node (Pin 14). When driven to the peak output of the  
preceding stage, Q3 or Q5 (depending on signal polarity) con-  
ducts most of the tail current, and the output rises to 532 µA.  
The LOG OUT current has thus changed by 500 µA as the  
input has changed from zero to its maximum value. Since the  
detectors are spaced at 10 dB intervals, the output increases by  
50 µA/dB, or 1 mA per decade. This scaling parameter is trimmed  
to absolute accuracy using a 2 kHz square wave. At frequencies  
near the system bandwidth, the slope is reduced due to the  
reduced output of the limiter stages, but it is still relatively in-  
sensitive to temperature variations so that a simple external  
slope adjustment can restore scaling accuracy.  
1
0
+25؇C  
–55؇C  
–1  
–2  
+85؇C  
+125؇C  
0.5  
0
–0.5  
0.1  
10  
100  
INPUT VOLTAGE – mV  
1000  
10000  
Figure 19. Logarithmic Output and Absolute Error vs. DC  
or Square Wave Input at TA = –55°C, +25°C, +85°C and  
+125°C. Input via On-Chip Attenuator  
The intercept position bias generator (Figure 17) removes the  
pedestal current from the summed detector outputs. It is ad-  
justed during manufacture such that the output (flowing into  
Pin 14) is 1 mA when a 2 kHz square-wave input of exactly  
±10 mV is applied to the AD641. This places the dc intercept at  
precisely 1 mV. The LOG COM output (Pin 13) is the comple-  
ment of LOG OUT. It also has a 1 mV intercept, but with an  
inverted slope of –1 mA/decade. Because its pedestal is very  
large (equivalent to about 100 dB), its intercept voltage is not  
guaranteed. The intercept positioning currents include a special  
internal temperature compensation (ITC) term which can be  
disabled by connecting Pin 8 to ground.  
showing the outputs at temperatures of –55°C, +25°C and  
+125°C. While the slope and intercept are seen to be little af-  
fected by temperature, there is a lateral shift in the end points of  
the “linear” region of the transfer function, which reduces the  
effective dynamic range.  
The on chip attenuator can be used to handle input levels 20 dB  
higher, that is, from ±7.5 mV to ±2 V for dc or square wave  
inputs. It is specially designed to have a positive temperature  
coefficient and is trimmed to position the intercept at 10 mV dc  
(or –24 dBm for a sinusoidal input) over the full temperature  
range. When using the attenuator the internal bias compensa-  
tion should be disabled by grounding Pin 8. Figure 19 shows  
the output at –55°C, +25°C, +85°C and +125°C for a single,  
AD641 with the attenuator in use; the curves overlap almost  
perfectly, and the lateral shift in the transfer function does not  
occur. Therefore, the full dynamic range is available at all  
temperatures.  
The logarithmic function of the AD641 is absolutely calibrated  
to within ±0.3 dB (or ±15 µA) for 2 kHz square-wave inputs of  
±1 mV to ±100 mV, and to within ±1 dB between ±750 µV and  
±200 mV. Figure 18 is a typical plot of the dc transfer function,  
2.5  
The output of the final limiter is available in differential form at  
Pins 10 and 11. The output impedance is 75 to ground from  
either pin. For most input levels, this output will appear to have  
roughly a square waveform. The signal path may be extended  
using these outputs (see OPERATION OF CASCADED  
AD641s). The logarithmic outputs from two or more AD641s  
can be directly summed with full accuracy.  
3
+125؇C  
2
+25؇C  
–55؇C  
2.0  
1.5  
1.0  
1
0
–1  
–2  
–55؇C  
+25؇C  
+125؇C  
A pair of 1 kapplications resistors, RG1 and RG2 (Figure 17)  
are accessed via Pins 15, 16 and 17. These can be used to con-  
vert an output current to a voltage, with a slope of 1 V/decade  
(using one resistor), 2 V/decade (both resistors in series) or  
0.5 V/decade (both in parallel). Using all the resistors from two  
AD641s (for example, in a cascaded configuration) ten slope  
options from 0.25 V to 4 V/decade are available.  
0.5  
0
–0.5  
0.1  
1.0  
10.0  
INPUT VOLTAGE – mV  
100.0  
1000.0  
Figure 18. Logarithmic Output and Absolute Error vs. DC  
or Square Wave Input at TA = –55°C, +25°C, and +125°C,  
Input Direct to Pins 1 and 20  
REV. C  
–7–