Method and apparatus for interpolating between data samples

Abstract: A method and apparatus for interpolating between data samples (V S ) that preserves the frequency spectrum of a sampled analog signal (V O ) is provided. Data samples (V S ) are interpolated to produce interpolated values (V IV ) that contain frequency domain information that accurately replicates an original frequency spectrum (24) of the analog signal (V O ) is disclosed. A signal processor (10) reads data samples (V S ) which occur at sampling times (t S ) and resample times (t R ) at which the V S values are interpolated. A set of t S times are found near each t R time. A digital FIR filter having a frequency function (H(fT)) and a continuous impulse response function h ( t / T) is embodied in software form within a program that controls the signal processor (10) where T is the width of the filter impulse response. The signal processor (10) convolves an offset continuous impulse response function with the V S values. A plurality of convolved values (V C ) are summed at each t R time to produce an interpolated value (V IV ) at each t R time. The frequency response function (H(fT)) of the digital FIR filter reduces aliasing errors introduced by spectral images (25a and 25b) of the original frequency spectrum (24) and reduces amplitude errors caused by the filter's pass band ripple (38). The V IV values contain frequency domain information that accurately replicates the original frequency spectrum (24).

Description: Technical Field The invention relates generally to preserving the frequency information of a sampled analog signal and, more particularly, to a method and apparatus for interpolating between data samples such that the interpolated values contain the same frequency domain information contained in the sampled analog signal. Background of the Invention Analog signals contain frequency domain information and time domain information that may be of interest to persons analyzing the signals. For various reasons, analog signals are often sampled by a time-based sampling process prior to analyzing the signal. Data samples produced by the sampling process contain both time domain information and frequency domain information about the analog signal. The time domain information, such as amplitude, for example, can be analyzed by measuring the amplitude of the data samples with an appropriate measuring device, such as a voltmeter, for example. Likewise, the frequency domain information can be analyzed by an appropriate apparatus, such as a digital spectrum analyzer, for example. In order to find time and frequency domain information for points between data samples, an interpolation technique must be used. The prior art offers numerous time-based methods of interpolation that provide varying degrees of accuracy between the interpolated values and the analog signal. Like the original data samples, time domain information contained in an interpolated value, such as amplitude, can then be measured by an appropriate device, such as a voltmeter. Likewise, if frequency domain information is sought for points between data samples, the data samples must be interpolated to find these values. Unfortunately, a time-based sampling process that produces data samples of an analog signal also produces spectral images of the analog signal's frequency spectrum. As a result, the data samples contain frequency domain information that includes the analog signal frequency spectrum information plus image information. The image information corrupts the frequency spectrum information so that the frequency domain information contained in the data samples does not accurately replicate the frequency spectrum of the analog signal. Prior art interpolation techniques further corrupt the frequency information contained in the data samples. As a result, the frequency information contained in the interpolated values does not accurately represent the frequency information contained in the analog signal. In Schafer et al, "A Digital Signal Processing Approach to Interpolation," Proceedings of the IEEE, Vol. 61, No. 6, pages 692-702 (June 1973), the authors describe a prior art interpolation system for resampling an input signal at a uniformly spaced resample times. The process involves convolving the input samples with a filter impulse response at the resample times and summing. Since the input and output sample rates are related by a constant, the value of the filter impulse response need only be known at a predetermined number of uniformly spaced points. This system does not allow interpolating at arbitrary resampling times, and it ignores the effect of the interpolation in the frequency domain. EP 099, 600 discloses a related system which provides an output signal sampled at an irrational multiple of the input signal sample rate. Again, this reference does not allow interpolating at arbitrary respamling times and ignores the effect of the interpolating operation on the frequency domain. As can be appreciated from the foregoing discussion, there is a need to provide a method and apparatus for interpolating between data samples such that the interpolated values contain the same frequency information contained in the sampled analog signal, i.e., such that the frequency spectrum of the sampled analog signal is preserved. The present invention is directed to a method and apparatus for interpolating between data samples using a digital filter in a novel manner that achieves this result, i.e., produces interpolated values that preserve the frequency spectrum of an analog signal. Summary of the Invention In accordance with this invention, a method and apparatus for producing interpolated values that contain accurate information about the original frequency spectrum of a sampled analog signal is provided, as defined in claims 1 and 5, respectively. As will be appreciated from the foregoing summary, the present invention provides a method and apparatus for preserving the frequency spectrum of a sampled analog signal by interpolating data samples using a digital filter such that the interpolated values contain frequency domain information that can be used to accurately replicate the frequency spectrum of the analog signal. Brief Description of the Drawings The foregoing, and other features and advantages of this invention, will become more readily appreciated as the same becomes further understood by reference to the following detailed description when taken in conjunction with the accompanying drawings, wherein: FIGURE 1 is a simplified block diagram of a preferred embodiment of an interpolating apparatus formed in accordance with the invention; FIGURE 2 is a simplified flowchart illustrating the functional steps of a program for controlling the apparatus illustrated in FIGURE 1; FIGURE 3 is a simplified block diagram depicting an alternative embodiment of the apparatus illustrated in FIGURE 1. FIGURES 4a, 4b and 4c are more detailed flowcharts of the functional steps illustrated in FIGURE 2; FIGURE 5 illustrates the relationship between frequency domain information contained in data samples and the frequency response of a suitably designed digital finite impulse response ("FIR") filter suitable for use in the apparatus illustrated in FIGURE 1; FIGURE 6, lines A-E, illustrates the interrelationship between the frequency response of a digital FIR filter and the continuous impulse response of the digital FIR filter; and, FIGURE 7, lines A-E, is a series of waveforms illustrating the convolution of the data samples with the continuous impulse response of a four-point digital FIR filter suitable for use in the apparatus illustrated in FIGURE 1. Description of the Preferred Embodiment There are situations where it is desirable to analyze, in the frequency domain, data that has been created in the time domain. Such a situation arises when an original analog signal is sampled by a time-based sampling process that produces data samples. While there are numerous interpolation techniques that will provide interpolated values in the time domain based on the data samples, in general, such techniques ignore the frequency domain information contained in the data samples. As a result, the interpolated values may not contain accurate frequency domain information. As a consequence, there has developed a need for an interpolating technique that will produce interpolated values containing accurate frequency domain information. Among other benefits, such values can be used to analyze the frequency spectrum of the original analog signal. Another example of frequency domain information that is of interest to some industries is the changes in phase angle of the shaft of a rotating machine that occur as the machine is operated. The frequency spectrum of analog signals created when such a machine is operated contains shaft phase angle information. As will become obvious from the following discussion, the present invention provides a method and apparatus for preserving the frequency spectrum of an analog signal by interpolating data samples using a digital filter in a novel manner so as to overcome the foregoing problems of the prior art. FIGURE 1 illustrates a preferred embodiment of an apparatus for interpolating data samples in accordance with the present invention. The apparatus illustrated in FIGURE 1 comprises: a signal processor 10; a sampler 12; a storage device 14; and a clock 16. The sampler 12, the storage device 14 and the clock 16, per se, do not form part of the present invention. They are included so that the invention will be more easily understood. An original fluctuating analog signal, designated V O , which has an original frequency spectrum, is applied to the sampler 12. The sampler 12 samples the V O signal and produces a digital data signal comprising data samples, designated V S , taken at known sample times, designated t S . The t S times are provided to the sampler 12 by the clock 16. The V S values and the t S times are stored in the storage device 14. As will be better understood from the following discussion, the signal processor 10 receives control information from an external source, such as time intervals between the t S times, designated Δt; resample times at which interpolation is to be performed, designated t R ; and, the number of t R times required, i.e., a data block size, designated Bls. As required, the signal processor 10 also receives the V S and t S values stored in the storage device 14. Based upon the externally generated control information and the V S and t S values, the signal processor 10 produces a series of interpolated values, designated V IV . The V IV values contain frequency domain information as well as time domain information. As will be better understood from the following discussion, the V IV values can be used to accurately replicate both the time and frequency domain information contained in the V O signal. The signal processor 10 can take the form of a specialized signal processor, i.e., a signal processor containing a program dedicated to carrying out the invention, or a suitably programmed general purpose computer. The broad functional steps of the program that controls the signal processor 10 are illustrated in FIGURE 2 and discussed next. Initially, the signal processor 10 reads into its internal memory the V S values, t S times, t R times, Δt intervals, and the data block size, Bls. Next, the program causes the signal processor 10 to read the first t R time and find a set of V S values occurring at t S times that are located near the first t R time. As will be better understood from the discussion below, the size of the set of V S values is determined by the nature of a digital filter, specifically a digital finite impulse response (FIR) filter that, preferably, is implemented in software form in the signal processor 10. The digital FIR filter has a time domain or continuous impulse response function, designated h(x), where x is a normalized time (i.e., x = t/T, where T is defined below and t is some time of interest, such as t R , for example) and a frequency domain or frequency response function, designated H(y), where y is a normalized frequency (i.e., y = fT). The continuous impulse response function, h(x), has a finite width, T. The size of the set of V S values is determined by the impulse response width, T. For example, if the impulse response width, T, encompasses four t S times, the signal processor 10 will find the four V S values associated with the four t S times nearest the first resample time, t R . In this case, the digital FIR filter is commonly referred to as a four-point filter. After the set of V S values has been found, the program instructs the signal processor to convolve the continuous impulse response function, h(x), of the digital FIR filter with each of the V S values in the set, to produce a convolved value, designated V C , located at t R , for each of the V S values in the set. As will become better understood from the following discussion, during this convolution step, the frequency response function, H(y), of the digital FIR filter performs a filtering operation. That is, the filter reduces the effects of spectral images introduced by the sampling process. Next, the signal processor 10 sums the V C values to produce a first interpolated value, V IV , i.e., the V IV value associated with the first t R time. Once this V IV value has been computed, the program instructs the signal processor 10 to read the next t R time, and the functional steps discussed above are repeated. The functional steps illustrated in FIGURE 2 are repeated until the signal processor 10 has produced V IV values for each of the t R times received and read by the signal processor 10. As a result of the filtering operation discussed above and other aspects of the filtering operation which are discussed below, the V IV values contain accurate frequency spectrum information of the original signal (i.e., V O ). While the presently preferred embodiment of the invention comprises a signal processor 10 and a program for carrying out the invention, as discussed above and illustrated in FIGURES 1 and 2, it is to be understood that alternative embodiments exist which are also suitable for carrying out the invention. One such alternative embodiment is a hardware embodiment of the sort illustrated in FIGURE 3. In this alternative hardware embodiment, the sampler 12, the storage device 14 and the clock 16 perform the functions discussed above. The alternative apparatus comprises: a receiver 18; a data locator 20; a digital filter 21; a convolver 22; and, a summer 23. The digital filter 21 is preferably a digital FIR filter having the h(x) and H(y) functions noted above. The receiver 18 receives the V S values and t S times from the storage device 14. The data block size, Bls, the time interval between t S times, Δt, and the resample times, t R , are provided to the receiver 18 by an external source. The data locator 20 finds the set of t S times nearest the first t R time and determines the associated V S values. As noted above, the size of the V S value set is determined by the impulse response width, T, of the impulse response function, h(x), of the digital FIR filter 21. Once the V S values have been found, the convolver 22 convolves the continuous impulse response function, h(x), with the V S values to produce a V C value located at the t R time for each t S time in the set. Next, the summer 23 sums the V C values at the t R time to produce the V IV value associated with the first t R time. The apparatus illustrated in FIGURE 3 repeats the above process until V IV values have been produced for each t R time received by the receiver 18. In a manner similar to that discussed above for the signal processor 10 (FIGURE 1), the frequency response function, H(y), of the digital FIR filter 21 performs a filtering operation. As a result, the original frequency spectrum of the V O signal is accurately reproduced in the frequency domain information contained in the V IV values. Before returning to the preferred embodiment of the invention (FIGURE 1) and discussing, in more detail, the functional steps of the program illustrated in FIGURE 2, a general "background" discussion of various aspects of the present invention is presented so that the invention may be more easily understood. More specifically, the novel concepts of: using the continuous impulse response function, h(x), of a digital FIR filter to perform time-based interpolation of the data samples, V S ; and, using the frequency response function, H(y), of the digital FIR filter to produce V IV values that contain accurate frequency spectrum information of the original signal (i.e., V O ). As is well known in the signal sampling art, digitally sampling an analog signal produces spectral images of the analog signal's frequency spectrum. As a result, the data samples produced by a digital sampling process contain frequency domain information relative to both the frequency spectrum of the analog signal and images of the frequency spectrum. When the data samples containing such information are interpolated, a portion of the image information is contributed to the analog signal frequency spectrum information contained in the interpolated values. This contribution of image information results in aliasing errors that distort the frequency spectrum information contained in the interpolated values. As a result, the frequency spectrum information contained in the interpolated values cannot be used to accurately determine the frequency spectrum of the analog signal. As will become better understood from the following discussion, the digital FIR filter used in the present invention reduces the contribution of the spectral image information in the interpolated values. As a result of this and other filtering operations performed by the filter, which are discussed below, the frequency domain information contained in the interpolated values can be used to accurately determine the frequency spectrum of the analog signal. FIGURE 5 illustrates the relationship between a digital FIR filter suitable for use with the present invention and the frequency spectrum of an analog signal and its spectral images. An original fluctuating analog signal, such as V O , for example, may be described as having a frequency spectrum 24 with the general shape depicted in FIGURE 5. So as to simplify the following discussion, the frequency spectrum 24 is centered about a zero frequency point. As noted above, spectral images are produced during sampling of the V O signal. As was also noted above, frequency domain information relative to the frequency spectrum 24 and the spectral images is contained in the resulting data samples, V S . As is well known in the sampling art, by sampling the V O signal at a sampling rate, designated f s , using an oversampling factor, designated m, where m > 1, the spectral images are centered at integer multiples of f s (i.e., ±1f s , ±2f s , ±3f s , etc.). A representative pair of spectral images 25a and 25b are depicted in FIGURE 5 as dashed curves and are centered at ±1f s . As is also well known in the sampling art, the bandwidths of the frequency spectrum 24 and the spectral images 25a and 25b are the same and are a function of the sampling rate, f s , and the oversampling factor, m. Specifically, the bandwidths are equal to the sampling rate divided by the oversampling factor (i.e., f s /m). Thus, as illustrated in FIGURE 5, the frequency spectrum 24 has a bandwidth that lies between ±f s /2m. Likewise, the bandwidth of the representative spectral image 25a lies between + f s ( 2m-1 / 2m) and + f s ( 2m+1 / 2m), and the bandwidth of the other representative spectral image 25b lies between -f s ( 2m-1 / 2m) and -f s ( 2m+1 / 2m). As noted above, and as will be better understood from the following discussion, a filter, such as a suitably designed digital FIR filter, can reduce the contributions of the spectral images 25a and 25b to the frequency spectrum 24 when the interpolation of the V S data samples is performed. In addition to the original frequency spectrum and images 25a and 25b, FIGURE 5 also illustrates an exemplary frequency response 29 for a suitably designed digital FIR filter having the general frequency response function, H(y), discussed above. The frequency response 29 has a shape that is defined by: a main lobe 40; and a series of side lobes 36a and 36b. As is well known in the filtering art, the main lobe 40 comprises a pass band 30 and a pair of transition bands 32a and 32b located on either side of the pass band 30. Transitions between the pass band 30 and the transition bands 32a and 32b are defined by points 62a and 62b, respectively. The series of side lobes 36a and 36b form a pair of stop bands 34a and 34b, located adjacent to transition bands 32a and 32b, respectively. Transitions between the stop band 34a and the transition band 32a, and between the stop band 34b and the transition band 32b are defined by points 60a and 60b, respectively. The pass band 30, transition bands 32a and 32b, and stop bands 34a and 34b are indicated by brackets in FIGURE 5. For ease of illustration, the frequency response 29 is centered at the zero frequency point. As is well known in the filtering art, the shape of the frequency response 29 is determined, in part, by the oversampling factor, m. More specifically, the relationship between the transition points: 60a and 62a; and, 60b and 62b is fixed and is equal to: 2m - 1; where m > 1. For example, an oversampling factor of two (i.e., m = 2) causes points 60a and 60b to occur at three times the frequency of points 62a and 62b. That is, the stop bands 34a and 34b begin at three times the cutoff frequencies of the pass band 30. In the above example (i.e., m = 2), the pass band 30 lies between ±f s /4 and the stop bands begin at ±3f s /4S Since the bandwidth of the original signal frequency spectrum 24 is equal to f s /m, in the above example (i.e., m = 2), the bandwidth is equal to f s /2 and lies between ± fs/4. As a result, the original signal frequency spectrum 24 lies within the pass band 30 of the digital FIR filter and the images 25a and 25b lie within the stop bands 34a and 34b. If the digital FIR filter were a perfect filter, the stop bands 34a and 34b would be perfectly attenuating, and the frequency information passed by the digital FIR filter would simply be the frequency spectrum 24. However, because real filters are not perfect, the stop bands 34a and 34b have imperfect attenuation capabilities. The series of side lobes 36a and 36b depict the imperfect attenuation of the stop bands 34a and 34b. The peak imperfect attenuation level is illustrated in FIGURE 5 by the horizontal dashed lines 44a and 44b. Because the stop bands 34a and 34b are not perfectly attenuating, portions of the spectral images 25a and 25b that lie within the stop bands 34a and 34b and are below the attenuation levels 44a and 44b are passed by the digital FIR filter. These portions of the images 25a and 25b passed by the digital FIR filter produce aliasing errors in the frequency information passed by the filter. Thus, the passed frequency information cannot be used to accurately replicate the original signal frequency spectrum 24. As will be better understood from the following discussion, the general shape of the frequency response 29 can be altered through appropriate design of the digital FIR filter. For example, the amplitudes of the series of side lobes 36a and 36b can be reduced, thereby increasing the attenuation levels 44a and 44b of the stop bands 34a and 34b. By increasing the stop band attenuation, a smaller portion of the spectral images 25a and 25b will be passed by the filter and the aliasing errors associated with the original signal frequency spectrum 24 passed by the digital FIR filter will be reduced. As a result, original signal frequency spectrum information contained in the interpolated values, V IV , will contain less image information, so that the frequency domain information contained in the V IV values can be used to more accurately replicate the original signal frequency spectrum. Another source of errors that can distort the original signal frequency spectrum 24 passed by the digital FIR filter is the shape of the pass band 30. In an ideal filter, the pass band 30 would be perfectly flat with respect to frequency. However, in practice, filters are not ideal and the pass band 30 is not perfectly flat. The digital FIR filter illustrated in FIGURE 5 has a pass band ripple 38 that may introduce amplitude errors into the frequency spectrum 24 that is passed by the filter. As will be better understood from the following discussion, the pass band flatness can be improved through appropriate filter design by reducing the pass band ripple 38. Reducing the pass band ripple 38 reduces the amplitude errors introduced into the frequency spectrum 24 by the ripple. Thus, in accordance with the invention, it is desirable to design a digital FIR filter that has a suitably flat pass band 30 and suitably attenuating stop bands 34a and 34b. An exemplary method for designing such a digital FIR filter suitable for use in the present invention is discussed next. In the preferred embodiment of the invention, as was noted above, the digital FIR filter is actually implemented in software form within the signal processor 10. As is well known in the filtering art, the frequency response function, H(y), of such a digital FIR filter depicted by the exemplary frequency response 29 in FIGURE 5, can be represented by one or more mathematical equations characterized by poles and zeros in the complex-frequency plane (hereinafter referred to as the frequency plane). As will be better understood from the following discussion, relocating one or more pairs of zeros within the frequency plane is one method of modifying the frequency shape 29. More specifically, the amplitudes of the side lobes 36a and 36b may be adjusted (i.e., reduced) by moving zeros along the real axis in the frequency plane, and the amplitude of the pass band ripple 38 may be adjusted (i.e., reduced) by moving zeros along the imaginary axis of the frequency plane. As is well known in the filtering art, the frequency response function, H(y), of a filter, such as a digital FIR filter, is related to the continuous impulse response function, h(x), of the filter. Specifically, the h(x) function is the inverse Fourier transform of the H(y) function. Thus, just as with the H(y) function, the h(x) function can be represented by one or more mathematical equations that are the inverse Fourier transform of the equations representing the H(y) function. As a result, changes made to the H(y) function which alter the frequency response 29 will cause corresponding changes in the continuous impulse response function, h(x). As will be presented in the following discussion, each pair of zeros that is moved about the frequency plane adds a cosine term to the equations representing the impulse response function, h(x). Adding cosine terms to the h(x) function changes the shape of the digital FIR filter's impulse response. However, as will be explained more fully below, as long as the number of zeros remains the same within a suitable frequency band, the width of the continuous impulse response, T, remains unchanged. FIGURE 6 illustratively depicts this relationship between the H(y) and h(x) functions of the digital FIR filter. FIGURE 6, line A illustrates a rectangular continuous impulse response 50. Such a rectangular impulse response 50 is representative of the h(x) function for a perfect FIR filter. The rectangular impulse response 50 has unity height (i.e., h = 1) and width, T. The corresponding H(y) function for a filter having the rectangular impulse response 50 is the Fourier transform of the impulse response 50 and can be defined by an equation of the general form: H(y) = sin πy πy . The frequency response 29 represented by Equation (1) is illustrated in FIGURE 6 on line B. The zero crossings of the frequency response 29 are the zeros of Equation (1). By normalizing the frequency scale in FIGURE 6 by T, the zeros occur at multiples of 1/T (i.e., y = ±1, ±2, etc.). The frequency response illustrated in FIGURE 6, line B, can be depicted in a more conventional form by changing the ordinate from a linear to a logarithmic magnitude scale. This causes the negative excursions of the frequency response to become positive excursions while remaining in the same relative position along the frequency axis. The resulting waveform of the frequency response is illustrated in FIGURE 6 on line C and has the same general shape as the frequency response 29 illustrated in FIGURE 5 and discussed above. Accordingly, the frequency response waveform illustrated in FIGURE 6, line C has a main lobe 40 and a series of side lobes 36a and 36b. For reasons of clarity, the pass band 30, transition bands 32a and 32b, and stop bands 34a and 34b are not illustrated in FIGURE 6, however, they have the same characteristics as discussed above and illustrated in FIGURE 5. FIGURE 6, line D, is a graphical illustration of how relocating zeros along the real axis in the frequency plane can reduce the amplitudes of the side lobes 36a and 36b. For example, by relocating two pairs of zeros that occur at the normalized frequency values of ±1 and ±2 (i.e., y = ±1, ±2), the width of the main lobe 40 is increased. Moving one pair of zeros along the real axis causes a new pair of side lobes 46a and 46b to be inserted where the zero pair has been relocated, such as at y = ±3.5, for example. The reinserted side lobes 46a and 46b reduce the amplitudes of side lobes 42a and 42b, which are adjacent to the main lobe 40. In the above example, the adjacent side lobes 42a and 42b have the highest peak value and therefore determine the attenuation levels 44a and 44b. By moving one pair of zeros from y = ±1, for example, to y = ±3.5, the stop band attenuation levels 44a and 44b are increased to levels 44a' and 44b' and are defined by the reduced amplitudes of the adjacent side lobes 42a and 42b. A second pair of zeros, originally located at y = ±2 in the above example, can be relocated to a point along the imaginary axis such as y = ± i1.3, for example. The imaginary axis in FIGURE 6, line D is normal to the page and is not shown for reasons of clarity. As noted above, by appropriately positioning the second pair of zeros along the imaginary axis, the pass band ripple 38 (not shown) of the frequency response can be reduced. Thus, by appropriately relocating pairs of zeros associated with the frequency response, the pass band ripple 38 and stop band attenuation levels 44a and 44b can be improved. As noted above, when zeros are relocated in the frequency plane, cosine terms are added to the continuous impulse response function, h(x), which change the shape of the h(x) function. In the example illustrated in FIGURE 6, the added cosine terms cause the rectangular impulse response 50 to change to a nonrectangular impulse response 52, whose shape is illustrated in FIGURE 6 on line E. The width, T, of the nonrectangular impulse response 52 remains unchanged because, as was noted above, the total number of zeros in the above example was not changed. So as to better understand the present invention, a brief discussion of the relationship between the movement of zero pairs in the frequency plane and the addition of cosine terms to the time domain function is presented next. As noted above, Equation (1) represents the frequency response of a perfect filter having the rectangular impulse response 50 illustrated in FIGURE 6, line A. As is well known in the filtering art, a perfect filter, i.e., a rectangular response 50 is not achievable. A more realistic filter has a nonrectangular impulse response (such as the nonrectangular impulse response 52 illustrated in FIGURE 6, line E, for example). Such a nonrectangular impulse response 52 can be represented by introducing a series of cosine terms into Equation (1). The corresponding frequency function, H(y), for such a nonrectangular impulse response 52 can be defined by an equation of the general form: where: n is the number of cosine terms in the time domain; ℓ is an integer; and, a ℓ is coefficient of the ℓ th cosine term. Equation (2) represents a series of waveforms, each having the general frequency shape defined by Equation (1), centered at different frequencies (i.e., y - ℓ) and having different amplitudes (i.e., a ℓ ). This is further illustrated by writing Equation (2) in a slightly different form as illustrated by the following equation: The corresponding time domain or continuous impulse response function, h(x), is defined as the inverse Fourier transform of Equation (2), and can be represented by an equation having the general form: where: R(x) is a rectangle having unit width and height. A ℓ is a coefficient of a cosine term defined as: A ℓ = 2(-1) ℓ a ℓ for ℓ ≠0; and, A ℓ = a ℓ for ℓ = 0; and, x = t / T where T is the width of the h(x) function. Thus, as illustrated by Equation (4), a nonrectangular impulse response 52 can be defined by a constant and a series of cosine terms. As stated above, such a nonrectangular impulse response 52 has the corresponding frequency shape defined by Equation (3). For reasons to be discussed below, Equation (3) can be reduced to a rational fraction having the general form: H(y) = y π sin πy B 0 [(y 2 -α 2 1 )(y 2 -α 2 2 )...(y 2 -α 2 n )] y 2 x (y 2 -1)...(y 2 -n 2 ) where: B 0 is a constant; and, α ℓ (where ℓ is an integer between 1 and n) is related to A ℓ in Equation (4). The α ℓ terms are the roots (i.e., zeros) of the numerator in Equation (5). As can be seen by comparing Equations (4) and (5), the number of cosine terms in the time domain (Equation (4)) is related to the number of new zeros in the frequency domain (Equation 5)). Moving a zero in the frequency plane is accomplished by adding an appropriate α ℓ term to Equation (5) that cancels one zero term and replaces the cancelled zero term with a new zero term, thus relocating the cancelled zero to a new location without changing the number of zero terms. Adding α ℓ terms to Equation (5) so as to relocate a zero causes a cosine term to be added to Equation (4) because, as noted above, the α ℓ terms are related to the A ℓ terms (i.e., the cosine coefficients). Thus, by moving zeros of the H(y) function in the frequency plane so as to improve the stop band attenuation 44a and 44b and improve the flatness of the pass band 30, causes cosine terms to be added to the impulse response in the time domain. As will be readily understood from the foregoing discussion by a person of reasonable skill in this art, the frequency response of a digital FIR filter can be designed so as to optimize the stop band attenuation 44a' and 44b' and pass band ripple 38 of the filter by moving zeros in the frequency plane. As will be better understood from the following discussion, and in accordance with the preferred embodiment of the present invention, the continuous impulse response function, h(x), can be convolved with the data sample values, V S , to (eventually) produce the interpolated values, V IV , at the appropriate resample times, t R . In general, during a convolution operation, the h(x) function is centered at an appropriate sample time, t S , so that a t R time is encompassed by the finite impulse response width, T. The h(x) function is multiplied by the V S value corresponding to the centered t S time, thereby producing a weighted h(x) function. A convolved value, designated V C , is the particular value of the weighted h(x) function corresponding to the t R time encompassed by the impulse response width, T. As will be better understood from the following discussion, a plurality of V C values for each t R time are computed when a plurality of weighted h(x) functions overlap the t R time. The plurality of V C values are summed at each t R time to produce the interpolated value, V IV . The convolution steps briefly discussed above are illustrated in FIGURE 7 and discussed in greater detail next by way of an example. In the example which follows, a four-point digital FIR filter is used. As noted above, a four-point filter has a h(x) function whose width, T, encompasses four data samples, (i.e., 4Δt ≤ T < 5Δt). FIGURE 7, line A, illustrates an exemplary series of V S values produced by a time-based sampling process. The V S values occur at t S times that, preferably, are spaced apart by equal time intervals, designated Δt. In the above example, each t S time is assigned an integer value, designated N, starting, for example, with the first t S time (i.e., N = 1) and increasing sequentially to the last t S time (i.e., N = Nth value). This is illustrated in FIGURE 7, line A as the integers 1 to N above the series of t S times. A t R time, preferably, is located between two adjacent t S points--t 8 and t 9 or designated integers 8 and 9, for example. In this example, the four t S times located nearest to t R , designated integer values of seven through ten (i.e., N = 7-10), are located at sample times, designated t 7 through t 10 , and have V S values, designated V 7 through V 10 , respectively. The convolution operation is illustrated in FIGURE 7 on lines B-E. The h(x) function is represented by the nonrectangular impulse response shape 52. First, the impulse response 52 is centered at t 7 and is multiplied by the V 7 value to produce a convolution value, designated V C1 , located at t R . Next, the impulse response 52 is centered at t 8 and multiplied by V 8 to produce a convolution value, designated V C2 , located at t R . Similarly, the impulse response 52 is separately located at t 9 and t 10 and multiplied by V 9 and V 10 to produce convolution values, designated V C3 and V C4 , respectively. Next, the V C1 -V C4 values are summed to produce the V IV value at the t R time. The convolution process is repeated for subsequent t R times until a V IV value has been computed for each t R time. The convolution operation illustrated in the above example can be expressed in terms of a general convolution equation having the following form: where: k is an integer; and, q is equal to the number of t S times encompassed by the impulse response width, T, (i.e., q = 4 for the four-point digital FIR filter in the above example). The impulse response function, h(x), is expressed in terms of the t R time offset by an integer multiple of Δt (i.e., N k Δt) and therefore forms an offset impulse response function Since, as was discussed above, each t S time is assigned a sequential integer value (i.e., 1 to N), the t S times located near any t R time can be defined by the following equation: N k = N 0 + k where N 0 is the integer multiple of Δt for the t S time closest to t R , and k is the integer defined in Equation (6). N 0 can be calculated from the following equation: N 0 = INT ( t R Δt + 0.5) where N 0 is rounded off to the nearest integer. An offset between t R and N 0 , designated t', is computed from the following equation: t' = t R - N 0 Δt . Solving Equation (7) for N 0 and substituting this value into Equation (8) and rearranging the terms provides the following relationship: t R - N k Δt = t' - kΔt. Substituting the right-hand side of Equation (10) into the impulse response term in Equation (6) yields the following relationship: Equation (11) illustrates how the offset impulse response function of the digital FIR filter can be expressed in terms of the offset time, t' Substituting the right side of Equation (11) into Equation (6) produces the following equation: As illustrated in Equation (12), V IV can be computed from a general convolution equation by multiplying the V S values (i.e., V S (N k Δt)) by the offset impulse response function The products are then summed to produce the V IV value at the resampling time, t R . Generally, the value of t' is different for each t R time and, as a result, the value of must be computed for each t R time. There are several well-known techniques for computing a few of which are noted next. One technique is to store several precalculated values of the impulse response function (i.e., h(x)) and use these values to compute directly. Another technique is to store only a few precalculated values of h(x) and interpolate to find Additionally, if a large look-up table of cosine terms is available, Equation (4) could be solved directly and the result could be inserted directly into Equation (6). Obviously, several conventional techniques exist for computing the value of and, as such, these techniques do not form a part of the present invention. As can be seen from examining Equation (12), the present invention provides a representation of a continuous approximation of the V O signal. That is, for any t R time desired, Equation (12) can be solved to provide the corresponding V IV value. As noted above, in addition to time domain information, the V IV values computed from Equation (12) contain frequency domain information that can be used to accurately replicate the V O signal frequency spectrum. As set forth in the foregoing discussion and in accordance with the preferred embodiment of the present invention, a digital FIR filter is used in a novel manner to interpolate between data samples of an analog signal and produce interpolated values that contain accurate V O signal frequency spectrum information. As noted above, such a digital FIR filter is preferably implemented in software form in a program that controls a signal processor 10 suitable for carrying out the invention. The broad functional steps of such a program are illustrated in FIGURE 2 and discussed above. A more detailed flow chart of the program depicted in FIGURE 2 is illustrated in FIGURES 4a, 4b, and 4c and discussed next. The steps set forth in FIGURES 4a-4c are examples of a four-point digital FIR filter application, such as for the four-point filter discussed in the above example. Obviously, the steps depicted in FIGURES 4a-4c can be readily adapted to other digital FIR filters (such as a ten-point filter, for example). Initially, as illustrated in FIGURE 4a, the program instructs the signal processor 10 to read and store: the V S values; the t S times; the t R times; the Δt interval; and, the data block size, Bls. The program further instructs the signal processor 10 to open a temporary file, V IV (I), for storing the computed V IV values. Next, the program causes the signal processor 10 to assign sequential integer values, N, to the t S times that have been read and stored. Preferably, the signal processor 10 begins with the first t S time and proceeds sequentially to the last t S time. That is, for example, if there are ten t S times, they are consecutively numbered 1-10 from the first to the last t S time. Next, the signal processor 10 is instructed to read the first t R time. The next functional step performed by the signal processor 10 is to determine the set of t S times that are closest to the first t R time. As noted above, the size of the set is determined by the width of the impulse response, T. First, a resampling index counter, designated I, and a summation index counter, designated K, are initialized (i.e., I = 1 and K = 1). Next, the program instructs the signal processor 10 to determine the closest t S time to the first t R time, i.e., N 0 . N 0 is computed from the following equation: Next, the offset, t', between the first resample time, t R , and the nearest t S time, (i.e., N 0 · Δt) is computed from Equation (9) above. Once N 0 and t' have been computed, the program instructs the signal processor 10 to find the other t S times, in the set of t S times closest to t R . In the present example, i.e., a four-point digital FIR filter application, the signal processor 10 will locate the four t S times closest to t R . Specifically, and as illustrated in FIGURE 4b, if t' is equal to or greater than half the interval between adjacent t S times (i.e., t' ≥ Δt/2), then the four closest t S times are determined by the following equation: N K = N 0 + K - C . If t' is less than half the Δt interval (i.e., t' < Δt/2), then the four closest t S values are determined by the following equation: N K = N 0 + C - K . In Equations (14) and (15), K is the summation index counter value noted above and C is an integer whose value is one-half the number of t S times encompassed by T (i.e., where C = 2 for the four-point filter in the above example). After the first N K point has been determined from Equation (14) or (15), the program determines whether the N K point lies within the data block (i.e., 1≤N K ≤Bl s ) and, if not, adjusts the N K value so that it is within the data block. More specifically, if the integer value of the t S time lies outside the data block (i.e., N K > Bls), and is greater than or equal to one (i.e., N K ≥1), the program places the t S time within the data block by subtracting the data block size from the integer value of the t S time (i.e., N K = N K - Bls). The signal processor 10 stores this value of N K . If the integer value of the t S time is outside the data block and is less than one (i.e., N K < 1), then the program adds the data block size to the integer value of the t S time (i.e., N K = N K + Bls) and stores this value of N K . If the integer value of the t S time is within the data block (i.e., 1≤N K ≤Bl s ), the value of N K is stored. Next, the program determines if all of the t S times in the set have been found. Specifically, in the four-point filter example discussed above, if the summation index counter value is less than four (i.e., K < 4) then the counter is incremented (i.e., K = K + 1) and the above process is repeated. A summation index counter value greater than or equal to four (i.e., K ≥ 4) indicates that the four t S times in the set have been found and the program proceeds to the next functional step, which is described next and illustrated in FIGURE 4c. Once the appropriate number of t S times near the t R time have been found, the signal processor 10 convolves the continuous impulse response function (h(x)), of a suitably designed digital FIR filter with the V S values of the t S times found in the set discussed above. As noted above, a suitable digital FIR filter is preferably implemented in software form and can be characterized by one or more mathematical formulae, such as Equation (2) (i.e., the frequency response function, H(y)) and Equation (4) (i.e., the impulse response function, h(x)), for example. The program instructs the signal processor 10 to determine a particular value of the offset impulse response function, defined in Equation (11) above, where k is replaced by K in the program illustrated in FIGURE 4C. As discussed above, the value of can be determined by conventional techniques. Next, the signal processor 10 performs the convolution operation by using the value of in the general convolution equation set forth in Equation (12) where, as noted above, k = K and q = 4. The resulting V IV value is stored as a V IV (I) value. This last step in the program performs the two functional steps illustrated in FIGURE 2 and discussed above. That is, the functional steps of producing the V C values and summing them to produce a V IV value are performed by the signal processor 10 in the convolution operation step illustrated in FIGURE 4C. Once the V IV value has been computed and stored by the signal processor 10, the program increments the resampling counter, I (i.e., I = I + 1). If the resampling counter value is less than or equal to the total number of resample times read by the signal processor 10 (i.e., I ≤ Bls), then the next t R time is read and the above steps are repeated. A resampling counter value that exceeds the total number of resample times (i.e., I > Bls) indicates that the V IV values have been computed for all t R times read by the signal processor 10 and the program is exited. As can be readily appreciated from the foregoing description, the invention provides a method and apparatus for preserving the frequency spectrum of a sampled analog signal using a digital FIR filter in a novel manner for interpolating between data samples. As a result, the interpolated values contain frequency information that can be used to accurately replicate the frequency spectrum of the analog signal. While a preferred embodiment of the invention has been illustrated and described herein, it is to be understood that, within the scope of the appended claims, various changes can be made. For example, digital FIR filters other than the four-point filter discussed in the above example can also be used. In fact, even non-FIR filters (i.e., filters having continuous impulse responses of infinite width) can be utilized, however, the convolution operation becomes much more complex. The frequency response and impulse response of the digital FIR filter can also be different than as illustrated and discussed above. Likewise, an oversampling factor other than two (i.e., 1 < m = 2) could also be used. While the time interval, Δt, between adjacent data samples is preferably the same, the invention is capable of performing its intended function even when the data samples are produced by a sampling process that samples the analog signal at a variable rate. Furthermore, the program merely illustrates one possible method of carrying out the invention and it is to be understood that other equally suitable programs could be utilized.

Claims: A method of producing interpolated values of an analog signal which has been sampled at known sample times (ts), the method comprising the steps of: (a) storing data samples (Vs) of the analog signal, said data samples containing frequency domain information about the analog signal's original frequency spectrum and frequency domain information about images of the analog signal's original frequency spectrum; (b) receiving an arbitrary selection of desired resample times (tr) at which said data samples are to be interpolated; and for each resample time (tr) : (c) choosing a set of data samples (Vs) occuring at sample times (ts) that are located nearest the resample time (tr); (d) weighting said set of data samples (Vs) by convoluting each of said data samples (Vs) with a continuous nonrectangular impulse response function h(x) of a filter having a predetermined frequency response H(y) comprising a substantially flat passband and suitably attenuating stopbands, said weighting producing a plurality of convolution values at each of said arbitrary selection of resample times (tr); and, (e) summing said plurality of convolution values at each of said resample times and producing an interpolated value at each of said resample times (tr). Method according to claim 1, wherein the size of the set of sample values (Vs) is determined by the width of the impulse response of the filter. The method according to one of the preceding claims, wherein the analog signal is sampled at a sampling frequency, fs, with an oversampling factor, m, and the predetermined frequency response includes a substantially flat passband for a band of frequencies between - fs/2m and fs/2m, and suitably attenuating stopbands for frequencies above fs (2m-1) / 2m and below -fs (2b-1) / 2m. Method according to one of claims 1 to 3, wherein a frequency function for the continuous nonrectangular impulse response has a general form as follows: An apparatus for producing interpolated values of an analog signal which has been sampled at known sampling times (ts), the apparatus comprising: (a) a receiver (18) for receiving data samples (Vs) of the analog signal, said data samples contain frequency domain information about the analog signal's original frequency spectrum and frequency domain information about images of the analog signal's original frequency spectrum, and for receiving an arbitrary selection of resample times (tr) at which said data samples (Vs) are to be interpolated; and, (b) interpolating means (20, 21, 22, 23) coupled to said receiver (18) for receiving said data samples (Vs) and said selection of resample times (tr), said interpolating means interpolating between said data samples to produce interpolated values (Viv) at said resample times (tr), wherein said interpolating means includes (b1) a filter (21) producing a continuous nonrectangular impulse response h(x) and an associated frequency response (Hy) comprising a substantially flat pass-band and suitably attenuating stopbands; (b2) a data locator (20) coupled to said receiver (18) for receiving said data samples (Vs) and said resample times (tr) and locating a set of said data samples (Vs) for each resample time (tr) that is located nearest each of said resample times (tr); (b3) convolving means (22), coupled to said data filter (21) and said data locator (20), for weighting the set of the data samples (Vs) with the continuous nonrectangular impulse response of the filter (21) for each of said resample times (tr) to produce a plurality of convolution values at the respective resample times (tr); and (b4) a summer (23) coupled to the convolving means (22) which sums the plurality of convolution values at each of the resample times to produce one of the interpolated values (Viv) at each of the resample times (tr). The apparatus according to claim 5 wherein a frequency function for the continuous nonrectangular impulse response has a general form as follows: The apparatus according to claim 5 or 6, wherein said frequency response of said filter (21) comprises: (a) a pass band for passing frequency domain information about the frequency spectrum of the analog signal and reducing contribution from pass band errors contained in said interpolated values; and, (b) stop bands for reducing contribution from images of the frequency spectrum of the analog signal contained in said interpolated values. The apparatus according to one of claims 5 to 7, wherein said filter (21) is a digital filter. The apparatus according to one of claims 5 to 8, wherein said filter (21) is a digital finite impulse response filter. The apparatus according to one of claims 5 to 9, wherein said filter (21) is implemented in software form.

Inventors: POTTER RONALD W, POTTER, RONALD W.
Applicants: HEWLETT PACKARD CO, HEWLETT-PACKARD COMPANY
Application year: 1989
Main classification: H03H17
IPC codes: H03H17, G06G7