Digital tone detection method

Abstract: Fast methods of tone detection and tone generation disclosed are particularly suitable for implementation in a digital signal processor. Chebyshev polynomials are employed to generate periodic waveforms and to detect such waveforms. In an alternative aspect of the invention, trigonometric formulae are employed to generate periodic waveforms which are representable as the sum of sine and cosine functions. Unlike analog techniques, the digital techniques do not entail long delays in the generation or detection of tones because a fast iterative recalculation is employed at each step. Accumulated error is avoided by restarting the procedure once a predetermined value is exceeded. Independent choice of a quality factor and a confidence level is provided by the digital tone detection technique.

Description: The present invention relates to digital detection of periodic signals and, more particularly, to a method using Chebyshev polynomials and trigonometric formulae to approximate periodic waveforms. BACKGROUND OF THE INVENTION Digital tone detection is useful in telecommunications, such as in dual-tone multi-frequency (DTMF) used in "two tone" or "multi-tone" signaling. Known in the art are sineous, Taylor series and discrete Fourier transform methods of waveform generation. These methods are computationally complex and require a large storage memory. For tone detection, analog filtering of tones followed by analog energy detection is employed. Conventional tone detection apparatus typically employs an analog tone filter which receives an input signal. The tone filter is typically a high-"Q" (quality-factor) providing extremely sharp rise and fall characteristics around the resonant frequency. Such analog circuitry is complex and costly to manufacture. More importantly, its response is sensitive to changes in temperature, voltage, component values and the like which result in variations in gain and band-pass characteristics. The tone detection apparatus employs an energy detector following the tone filter responsive to the filtered signal which requires that a "confidence level" be selected. The energy detector produces a signal which is monitored by a decision device which determines whether the detected energy exceeds a "threshold" level and produces a binary-valued output therefrom indicating whether the received signal has the appropriate frequency at a satisfactory energy level. The time required to detect a tone by such apparatus is determined by the Q factor and confidence level selected. This time can be substantial if a high level of quality and confidence is required. A method using Chebyshev polynomials and trigonometric formulae to approximate periodic waveforms is known in the art, for example, from the patent application FR-A-2 429 468, wherein terms of a Chebyshev sequence are used recursively to digitally generate a sequence of samples constituting the waveform according to the equation S (m+1) = 2 S m S₁ - S (m-1) . This method, however, entails the risk that errors are accumulated. To cope with this problem, the French patent application employs a correction method in that amplitude values A i ² are continuously compared with two values While this correction method is feasible, it is nevertheless cumbersome in its hardware implementation. From the patent application GB-A-2 100 537 an adaptive technique is known for automatic frequency determination and measurement. A filter is adapted to a signal component of an input signal using a variable generated by an adapter. The variable has a prescribed relationship to the frequency of the signal component. The variable is used to weight a combination of signal values derived from past signal history to form a prediction of a future signal. An adder combines the new signal value with the prediction to form an error signal which is used by the filter and the adapter. When the filter converges, a frequency indicator using the variable provides an output signal indicative of the frequency of the signal component. It is an object of the present invention to provide a method for detection of tone signals by digital means which is simpler in its hardware implementation than conventional tone detection apparatus. This object is achieved with a digital tone detection method according to the characteristic features of claim 1. Further advantageous features of implementation may be taken from the subclaims. The novel features of the invention together with further objects and advantages will be better understood from the following summary and detailed description of the invention when considered in connection with the accompanying drawings. SUMMARY OF THE INVENTION Terms of a Chebychev sequence are used recursively to digitally generate a sequence of normalized tone signals. Because roundoff and truncation errors will propagate and accumulate, errors will tend to grow if no corrective action is taken. The method of the invention provides that when a term in the sequence exceeds a predetermined value, the generation of tone signals is restarted. The method of the invention is particularly suited to digital computation because it involves only one left shift, one multiplication and one subtraction to generate each term in the sequence of tone signals. Accordingly, little or no delay is experienced in the tone detection according to the invention. In an alternative embodiment of the invention, terms of a trignometric formulae are employed iteratively to generate both cosine and sine wave tone signals. The method calls for restarting of the generation of tones whenever a term exceeds a predetermined value. The alternative method is equally well suited to digital computation. In the method of digital tone detection the term-by-term difference between a sequence of measured tone signals and the signal predicted by the corresponding term of the Chebyshev sequence is determined. If the absolute value of this difference is less than a predetermined threshold value then it is concluded that the measured tone signals have the frequency of the Chebyshev sequence. The digital tone detection method of the instant invention can be controlled to provide a high "Q" or a low "Q" filter. Independently, a selectable confidence level can be provided for the detection. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a flowchart describing the method of digital generation of tones. Fig. 2 is a signal-flow diagram for the digital generation of tones. Fig. 3 is a flowchart describing an alternative method of digital generation of tones. Fig. 4 is a signal-flow diagram for the alternative digital generation of tones. DETAILED DESCRIPTION OF A PREFERRED EMBODIMENT Any single tone signal can be appropriately scaled to be represented as a cosine or sine waveform using methods well-known to those of ordinary skill in the art. A cosine waveform having a frequency f can be sampled at periodic sampling intervals of T time units to produce the sequence {COS(2πfTm) m=0, 1, 2, 3,...}. Terms of the Chebyshev polynomial are given by the formula C m (x) = cos (m arccos(x)) m=0,1,2,... . A general recursive relationship exists between the terms C m-1 , C m and C m+1 : C m+1 (x) = 2C m (x)C₁(x) - C m-1 (x). By expressing the terms C m-1 , C m and C m+1 in equation (2) in terms of the cosine functions of equation (1), and using T=arccos(x) yields cos(m+1)2πfT = 2cos(m2πfT)·cos 2πfT - cos 2πfT(m-1). Equation (3) thus allows a sequence of normalized tone signals to be recursively generated for values of m=1,2,..., by starting with cos(0·2πfT)=1 and cos (1·2πfT) = cos 2πfT. The recursive generation of tone signals can thus be effected by repeated recalculation of Equation (3). For a tone of frequency f and amplitude A, samples can be generated every T seconds resulting in the signal waveform S = Acos(m(2πfT)) As will be appreciated by those skilled in the art, such recalculations are readily performed by a digital processor, in which the term cos(m(2πfT)) can be iteratively calculated by equation (3). Roundoff and truncation errors will be progagated by such a procedure, however. The errors tend to accumulate and would produce a waveform of ever-increasing error if not corrected. By reinitializing the computation periodically, this accumulation problem can be avoided. A flowchart of the method of the instant invention is provided as Fig. 1. A block 10 is initially entered which performs the initialization steps indicated by Equations (4). A block 12 is next entered which performs the iterative calculation of the next sample term according to Equation (3). Next a decision block 14 is entered which tests whether the term calculated in block 12 exceeds 0.999. If not a "No" exit is taken from decision block 14 back to block 12 and the next sample term is calculated in block 12. If the test performed in block 14 indicates that the term exceeded 0.999 a "YES" exit is taken from block 14 which causes block 10 to be entered. Accordingly, any accumulated error is removed as the sequence of terms is reinitialized and restarted once again. In accordance with this method then, the calculations to generate one sample at block 12 requires one left shift, one multiplication and one subtraction. As described hereinabove, the particular frequency and amplitude desired in the resulting waveform, S, is given by Equation (5). The value used in block 12 of 0.999 is selected to be near the maximum value that the cosine function can take (1.0) and yet be readily reached within a few iterations of the loop including the "No" exit. Now with reference to Fig. 2, a signal-flow diagram of an implementation of the method of the instant invention is provided. An initialization block 20 generates the first two terms of the sequence of a tone signal according to Equation (4). These signals are received at a first input of a one time-unit delay block 22 and a first input of a one time-unit delay block 24. Delay block 22 generates a signal received by an adder node 26 at a subtractice input thereto. Adder 26 also receives at an additive input a signal generated by a multiplier node 28. Multiplier 28 receives at a first input the signal generated by second delay block 24 and at a second input the fixed signal 2cosT. The signal generated by delay 24 is also conducted to a second input of delay 22 and the signal generated by adder 26 is conducted to a second input of delay 24. The signal generated by delay 24 is also conducted to the initialization block 20 and is the output signal corresponding to equation (3). Circuitry internal to block 20 implements the test performed in flowchart decision block 12 (Fig. 1) and resets the signals generated so that the first two terms of the sequence of tone signals are conducted to delays 22 and 24. Delay blocks 22 and 24 receive control signals (not shown) from initialization block 20 which cause the signals at their first inputs to be selected during the first time period after initialization and signals at their second inputs to be selected at all other time periods. An alternative method of generation is required when both cosine and sine waveforms need be generated. Such is the case when a Quadrature Amplitude Modulation (QAM) scheme is used to transmit digital data over analog telecommunication lines. In this case, the trigonometric identities can be employed in an iterative manner to generate both cosine and sine wave samples of frequency f at intervals of T seconds. With reference to Fig. 3, a flowchart is provided employing the Equations (6) to generate samples of periodic waveforms. A block 50 is initially executed which calls for initialization of the cos 2πfT and sin 2πfT terms. Such initialization values can be provided by numerical analysis methods known to those of ordinary skill in the art. Next a block 52 is entered which employs Equations (6) to iteratively calculate the next sample values of cosine and sine. In order to avoid accumulation of truncation and roundoff error, a decision block 54 is next entered which tests whether cos 2πfT exceeds 0.999. This test results in either a return to the initialization block 50 or the recalculation block 52 as was described hereinabove in connection with the Chebyschev method of Fig. 1. With reference to Fig. 4, a signal-flow diagram of am implementation of the method of the instant invention is provided. An initialization block 60 generates the first term of the sequence of tone signals. The signal is received at a first input of a one time-unit delay block 62 and a first input of a one time-unit delay block 64. Delay block 62 generates a signal received at a first input of a multiplier node 65 and a first input of a multiplier node 66. The signal generated by delay 64 is received at a first input of a multiplier node 68 and a first input of a multiplier node 70. A signal corresponding to cos 2πfT is received at a second input of multipliers 65 and 68. A signal corresponding to sin 2πfT is received at a second input of multiplers 66 and 70. An adder node 72 receives the signal generated by multiplier 65 at an additive input and the signal generated by multiplier 70 at a subtractive input. An adder node 74 receives the signal generated by multiplier 74 at an additive input and the signal generated by multiplier 68 at a subtractive input. The signal generated by adder 72 is conducted to a second input of delay 62 and to the initialization block 60. The signal generated by adder 74 is conducted to a second input of delay 64 and is the output signal corresponding to the second of equations (6). The signal generated by delay 62 is the output signal corresponding to the first of equations (6). Circuitry internal to block 60 implements the test performed in flowchart decision block 54 (Fig. 3) and resets the signal generated so that the first term of the sequence of tone signals are conducted to delays 62 and 64. Delay blocks 62 and 64 receive control signals (not shown) from initialization block 60 which cause the signals at their first inputs to be selected during the first time period following initialization and signals at their second inputs to be selected at all other time periods. The method of digitally generating waveforms described in connection with Figs. 1 and 2 can be employed to provide a method of digital tone detection. If the tone to be detected is given by the sequence of samples {1, cos 2πfT, cos 2·2πfT, cos 3·2πfT, ...} and the tone signals received are represented by the sequence of samples {x0, x1, x2, x3, ...} then, in the case of the method employing the Chebyschev sequence, an error term for each sample is given by the equation Error = Xn - [(2 cos2πfT) Xn-1 - Xn-2] Equation (9) represents the difference between the measured tone signals Xn and the signal predicted by the corresponding term of the Chebyshev sequence Cn, shown in terms of Xn-1 and Xn-2. If the absolute value of the error is less than a selected threshold value, i.e. |error| < threshold then it is determined that the sequence of received samples (8) has the frequency of the sequence (7). To control the "Q-factor" employed in conventional tone detectors the threshold value can be lowered, resulting in a "high-Q" filter, or raised, resulting in a "low-Q" filter. Similarly, to increase the confidence level employed in conventional tone detectors, a voting-logic scheme can be used. For instance, several previous samples can be used in equation (9) to generate the predicted signal, rather than merely two, X n-1 and X n-2 . Then if a predetermined percentage of these samples, such as 90%, satisfy equation (10), it is determined that the sequence of received samples (8) has the frequency of sequence (7). In this way, the two major parameters affecting the detection of tones can be chosen independently. This feature of the instant invention provides a significant advantage over the tone detectors of the prior art.

Claims: Method of digital tone detection wherein a digitally generated waveform having a predetermined comparison sequence of signal samples P(m) is employed for comparison with a sequence of received tone signals constituting a periodic waveform S(t) having a predetermined frequency f and being sampled at predetermined intervals of time T m , thereby taking samples of said signal S(2πfTm), characterized by the following combination of sequential steps: (A) calculating an error value E between said sample S(2πfTm) and a corresponding sample P(m) of said comparison sequence according to the equation E = S(2πfTm) - P(m) (B) comparing the absolute value of said error E with a predetermined threshold value; and (C) indicating detection of said periodic waveform S(t) if said comparison indicates this absolute error value E is less than said threshold value. Detection method according to claim 1, characterized in that said predetermined comparison sequence of signal samples P(m) is determined by the equations: P(0) = 1 P(1) = cos (2πfT) P(m+1) = 2P (m) · P(1) - P(m-1) . Detection method according to claim 1 or claim 2, wherein steps (A) and (B) are repeated a predetermined number of samples "n" , and step (C) further indicating detection of said periodic waveform S(t) if each said comparison at step (B) indicates the said absolute error value E is less than said threshold value, in a predetermined percentage of n comparisons.

Inventors: ASGHAR SAF, PYI HWA-SHENG, ASGHAR, SAF, PYI, HWA-SHENG
Applicants: ADVANCED MICRO DEVICES INC, ADVANCED MICRO DEVICES, INC.
Application year: 1988
Main classification: H04Q1
IPC codes: H04L27, H04Q1, G06G7, G06F7, H03B28