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ADC701JH 参数 Datasheet PDF下载

ADC701JH图片预览
型号: ADC701JH
PDF下载: 下载PDF文件 查看货源
内容描述: [暂无描述]
分类和应用: 转换器
文件页数/大小: 15 页 / 112 K
品牌: BB [ BURR-BROWN CORPORATION ]
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FFT Parameters  
SELECTION OF TEST FREQUENCIES  
Accurate FFT analysis of 16-bit systems requires adequate  
computing hardware and software. The FFT length (number  
of points) should be relatively large—at least 4K and prefer-  
ably 16K or larger. There are several reasons for this:  
The FFT (and any similar DSP operation) treats the total  
time-domain record length as one cycle of an infinitely long  
periodic signal. Therefore, if the end of the sampled record  
does not match up smoothly with the beginning, the output  
spectrum will contain serious errors known as leakage or  
truncation error(2). This well-known problem is usually  
handled by applying a windowing function to the time-  
domain samples, suppressing the worst effects of the mis-  
match. However, the most often used windows such as  
Hanning, Hamming, raised cosine, etc., are completely inad-  
equate for 16-bit ADC testing. More sophisticated functions  
such as the four-sample Blackman-Harris window(3) will  
provide much better results, although there still will be  
obvious spreading of the spectral lines.  
1. The converter itself has 64K codes. Ideally, the test  
would guarantee that all codes are tested at least once.  
Practically speaking, however, that would require im-  
mensely long FFTs (>>64K points) or averaging of a  
large number of smaller FFTs. By using an FFT length of  
4K or greater and proper selection of the test frequencies,  
a very good statistical picture of the ADC performance  
will be obtained which shows the effect of any defects in  
the transfer function.  
2. The noise floor of the output spectrum is not low enough  
if less than 4K points are taken. Shorter FFTs have fewer  
bins to cover the output spectrum, so a larger fraction of  
the total system noise appears in each bin. Although the  
SNR of the ADC701/SCH702 system is in the range of  
–93dB, the noise level of the available generators may  
increase the total measured noise power to –80dB. Every  
doubling of the FFT length will spread the noise power  
among twice as many bins, resulting in a 3dB reduction  
of the spectral noise floor. In order to resolve spurious  
components that are at the level of –110dB, an average  
noise floor of less than –113dB would be barely ad-  
equate. This requires at least 2048 bins in the output  
half-spectrum, corresponding to a 4K-point FFT. Even  
at this level, it will be difficult or impossible to separate  
higher order harmonics in the ADC701 response from  
the average noise level, indicating that longer FFTs are  
desirable.  
The most successful approach is to eliminate the need for  
windowing by properly selecting the test signal frequency  
(or frequencies) in relation to the ADC sampling frequency(4).  
If the time sample contains exactly an integer number of  
cycles, then there is no mismatch or truncation error. An-  
other point to consider is that the sampling frequency should  
not be an exact integer multiple of the signal frequency,  
which would tend to reduce the number of different ADC  
codes that are tested and also tend to artificially concentrate  
quantization error in the harmonics of the test signal.  
Both of these criteria are met by choosing an FFT length  
which is a power of two (the most standard and fastest to  
compute) and choosing a test frequency which causes an  
exact odd integer number of cycles to appear in the time  
record. In software, this selection can be accomplished very  
easily:  
1. Determine the desired sampling frequency fS.  
3. Following the guidelines for test frequency selection  
which are outlined in the next section, it becomes clear  
that longer FFTs allow a much wider choice of test  
frequencies without concern for sophisticated data win-  
dowing or code coverage problems.  
2. Determine the desired input signal frequency fAPPROX.  
3. Determine the FFT length N, which should be a power of  
2 (e.g., 4096 or 16384).  
4. Divide fAPPROX by fS, multiply the quotient by N, and  
round the result to the nearest odd integer. This is M, the  
number of cycles in the time record.  
Besides the consideration of FFT length, it is important to  
realize that the FFT calculations must be performed with  
high-precision arithmetic. The use of 32-bit fixed or floating  
point calculations will generally be inadequate because the  
noise floor due to calculation errors alone will interfere with  
the ADC performance data. Unfortunately, this considera-  
tion precludes the use of most DSP accelerator boards and  
similar hardware. In order to preserve the full dynamic range  
of the ADC output, it is best to use standard 64- or 80-bit  
arithmetic. To avoid excessively long calculation times, the  
FFT algorithm should be written in an efficiently compiled  
language and make use of techniques such as trigonometric  
look-up tables in software and dedicated floating-point  
coprocessors in hardware. There are several commercial  
software packages available from Burr-Brown and others  
that meet these requirements.  
5. Multiply M by fS and divide by N to obtain the exact  
input signal frequency fACTUAL  
.
SIGNAL GENERATOR CONSIDERATIONS  
To suppress leakage effects, the calculated ratio of fS to  
fACTUAL must be precisely maintained during the test. This  
requirement is met easily by the use of synthesized signal  
generators whose reference oscillators can be locked to-  
gether. Other possible approaches include external phase  
locking of non-synthesized generators and direct digital  
synthesis techniques. If it is not possible to use phase-locked  
signals, then a Blackman-Harris window may be used as  
mentioned previously.  
®
13  
ADC701/SHC702  
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