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AD650JN 参数 Datasheet PDF下载

AD650JN图片预览
型号: AD650JN
PDF下载: 下载PDF文件 查看货源
内容描述: 电压 - 频率和频率 - 电压转换器 [Voltage-to-Frequency and Frequency-to-Voltage Converter]
分类和应用: 转换器
文件页数/大小: 12 页 / 285 K
品牌: ADI [ ADI ]
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AD650  
1 µF to 10 µF tantalum capacitor should be connected directly  
to the supply side of the pull-up resistor and to the digital  
ground—Pin 10. The pull-up resistor should be connected  
directly to the frequency output—Pin 8. The lead lengths on the  
bypass capacitor and the pull up resistor should be as short as  
possible. The capacitor will supply (or absorb) the current tran-  
sients, and large ac signals will flow in a physically small loop  
through the capacitor, pull up resistor, and frequency output  
transistor. It is important that the loop be physically small for  
two reasons: first, there is less self-inductance if the wires are  
short, and second, the loop will not radiate RFI efficiently.  
The digital ground (Pin 10) should be separately connected to  
the power supply ground. Note that the leads to the digital  
power supply are only carrying dc current and cannot radiate  
RFI. There may also be a dc ground drop due to the difference  
in currents returned on the analog and digital grounds. This will  
not cause any problem. In fact, the AD650 will tolerate as much  
as 0.25 volt dc potential difference between the analog and digital  
grounds. These features greatly ease power distribution and  
ground management in large systems. Proper technique for  
grounding requires separate digital and analog ground returns to  
the power supply. Also, the signal ground must be referred  
directly to analog ground (Pin 11) at the package. All of the sig-  
nal grounds should be tied directly to Pin 11, especially the  
one-shot capacitor. More information on proper grounding and  
reduction of interference can be found in Reference 1.  
Figure 7. 1 MHz V/F Connection Diagram  
DECOUPLING AND GROUNDING  
It is good engineering practice to use bypass capacitors on the  
supply-voltage pins and to insert small-valued resistors (10 to  
100 ) in the supply lines to provide a measure of decoupling  
between the various circuits in a system. Ceramic capacitors of  
0.1 µF to 1.0 µF should be applied between the supply-voltage  
pins and analog signal ground for proper bypassing on the AD650.  
In addition, a larger board level decoupling capacitor of 1 µF to  
10 µF should be located relatively close to the AD650 on each  
power supply line. Such precautions are imperative in high reso-  
lution data acquisition applications where one expects to exploit  
the full linearity and dynamic range of the AD650. Although  
some types of circuits may operate satisfactorily with power sup-  
ply decoupling at only one location on each circuit board, such  
practice is strongly discouraged in high accuracy analog design.  
TEMPERATURE COEFFICIENTS  
The drift specifications of the AD650 do not include temperature  
effects of any of the supporting resistors or capacitors. The drift  
of the input resistors R1 and R3 and the timing capacitor COS  
directly affect the overall temperature stability. In the application  
of Figure 2, a 10 ppm/°C input resistor used with a 100 ppm/°C  
capacitor may result in a maximum overall circuit gain drift of:  
Separate digital and analog grounds are provided on the AD650.  
The emitter of the open collector frequency output transistor is  
the only node returned to the digital ground. All other signals  
are referred to analog ground. The purpose of the two separate  
grounds is to allow isolation between the high precision analog  
signals and the digital section of the circuitry. As much as sev-  
eral hundred millivolts of noise can be tolerated on the digital  
ground without affecting the accuracy of the VFC. Such ground  
noise is inevitable when switching the large currents associated  
with the frequency output signal.  
150 ppm/°C (AD650A) + 100 ppm/°C (COS) + 10 ppm/°C (RIN) 260 ppm/°C  
In bipolar configuration, the drift of the 1.24 kresistor used to  
activate the internal bipolar offset current source will directly  
affect the value of this current. This resistor should be matched  
to the resistor connected to the op amp noninverting input (Pin  
2), see Figure 4. That is, the temperature coefficients of these  
two resistors should be equal. If this is the case, then the effects  
of the temperature coefficients of the resistors cancel each other,  
and the drift of the offset voltage developed at the op amp non-  
inverting input will be determined solely by the AD650. Under  
these conditions the TC of the bipolar offset voltage is typically  
–200 ppm/°C and is a maximum of –300 ppm/°C. The offset  
voltage always decreases in magnitude as temperature is increased.  
At 1 MHz full scale, it is necessary to use a pull-up resistor of  
about 500 in order to get the rise time fast enough to provide  
well defined output pulses. This means that from a 5 volt logic  
supply, for example, the open collector output will draw 10 mA.  
This much current being switched will surely cause ringing on  
long ground runs due to the self inductance of the wires. For  
instance, #20 gauge wire has an inductance of about 20 nH per  
inch; a current of 10 mA being switched in 50 ns at the end of  
12 inches of 20 gauge wire will produce a voltage spike of 50 mV.  
The separate digital ground of the AD650 will easily handle  
these types of switching transients.  
Other circuit components do not directly influence the accuracy  
of the VFC over temperature changes as long as their actual val-  
ues are not so different from the nominal value as to preclude  
operation. This includes the integration capacitor, CINT. A  
change in the capacitance value of CINT simply results in a dif-  
ferent rate of voltage change across the capacitor. During the  
Integration Phase (refer to Figure 2), the rate of voltage change  
across CINT has the opposite effect that it does during the Reset  
Phase. The result is that the conversion accuracy is unchanged  
A problem will remain from interference caused by radiation of  
electro-magnetic energy from these fast transients. Typically, a  
voltage spike is produced by inductive switching transients;  
these spikes can capacitively couple into other sections of the  
circuit. Another problem is ringing of ground lines and power  
supply lines due to the distributed capacitance and inductance  
of the wires. Such ringing can also couple interference into sen-  
sitive analog circuits. The best solution to these problems is  
proper bypassing of the logic supply at the AD650 package. A  
1“Noise Reduction Techniques in Electronic Systems,” by H. W. OTT,  
(John Wiley, 1976).  
REV. C  
–7–  
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