# Dynamic Range Analysis of the Phase Generated Carrier Demodulation Technique

Authors: M. J. Plotnikov; A. V. Kulikov; V. E. Strigalev; I. K. Meshkovsky
Journal: Advances in Optical Technologies
 (2014)

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## Abstract

The dependence of the dynamic range of the phase generated carrier (PGC) technique on low-pass filters passbands is investigated using a simulation model. A nonlinear character of this dependence, which could lead to dynamic range limitations or measurement uncertainty, is presented for the first time. A detailed theoretical analysis is provided to verify the simulation results and these results are consistent with performed calculations. The method for the calculation of low-pass filters passbands according to the required dynamic range upper limit is proposed.


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## Body

## 1. Introduction

Fiber optic interferometric sensors have been intensively developed for the past few decades. Fiber-optic interferometers are used as a sensitive element in fiber optic gyroscopes, hydrophones, and so forth [1]. As a result, many special data acquisition methods, digital signal processing algorithms, and demodulation techniques have been invented to recover measured phase signals. One of the most popular demodulation techniques is phase generated carrier (PGC) demodulation technique [2].This technique has been used in many applications such as hydroacoustics [3–5], vibration [6], and pipeline leakage detection [7], and its main properties have been thoroughly studied [8–10].However, implementation methods of demodulation techniques have changed with the advent of high performance field programmable gate arrays (FPGAs). FPGAs allow realizing complex real-time digital signal processing algorithms, and therefore they are ideally suitable for the multichannel PGC technique implementation to demodulate signals from fiber-optic sensor arrays [11]. Unfortunately, the usage of FPGAs for such purposes has got some problems caused by sampling frequency restrictions and finite passbands of digital schemes.This paper is devoted to the detailed analysis of the PGC technique taking into account its practical implementation problems and digital design restrictions. The dependence of the dynamic range of the PGC technique on low-pass filters passbands is investigated for the first time and the nonlinear character of this dependence is shown and explained.


## 2. Simulation

The PGC demodulation scheme is presented in Figure1 [11]. Its functional model was implemented using MATLAB to investigate dependences of output signals on various parameters. Filter Design and Analysis Tool (FDATool) was used for generating necessary finite impulse response digital filters.Figure 1
PGC demodulation scheme.Several parameters were constants in this model:(i)
the duration of simulated signals was 1 second;(ii)
the carrier frequency was set to 10 kHz;(iii)
the sampling frequency of the model was 100 kHz.Low-pass filters passbands were set to 500 Hz hence the input signal at the frequency 500 Hz passed through these filters without attenuation.Results of performed simulations are shown in Figure2.Figure 2
Simulation results of the PGC demodulation scheme: dependencies of the output signal on the measured phase signal amplitude (D) and the carrier modulation depth (C).During this simulation the amplitude of the measured phase signal (at the frequency 500 Hz) and the carrier modulation depth were changing from 0 to 6.28 rad.According to obtained results (see Figure2), the output signal from the PGC demodulation scheme depends nonlinearly on both the measured phase signal amplitude (D) and the carrier modulation depth (C). To get a detailed explanation of these results, both dependencies were analyzed separately.


## 3. Analysis

The demodulated result of the PGC scheme (see Figure1) for small signal amplitudes and small signal frequencies is expressed as [11, 12]
(1)Sout(t)=B2J1(C)J2(C)φ(t),(2)φ(t)=Dcos⁡ωt+φ0,
where B depends on the input optical power and the mixing efficiency of the interferometer, C is carrier modulation depth, Ji(C) with i=1,2,…, are the first-order and second-order Bessel functions with C, D is the measured phase signal amplitude, ω is the angular frequency of the measured phase signal, and φ0 is the initial phase of the interferometer.As shown in Figure2, the amplitude dependence of the output signal on the carrier modulation depth is directly proportional to the result of multiplication J1(C)J2(C). This result is consistent with (1). Furthermore, it can be seen that the optimal value of the carrier modulation depth, which provides the local extreme value of J1(C)J2(C) and corresponds to the maximum amplitude of the output signal, is C≈2.37 rad [12].According to (1), the amplitude dependence of the output signal from the PGC demodulation scheme is a linear function for small input signal amplitudes; that is, the amplitude of the output signal is directly proportional to the amplitude of measured phase signals. However, obtained results show that this dependence is nonlinear for large input signal amplitudes (see Figure 2).In order to explain obtained results, signals after low-pass filters in the PGC demodulation scheme (see Figure1) should be expressed in detail as(3)S1(t)=-BJ1(C)×(cos⁡φ0[2∑k=0∞(-1)kJ2k+1(D)cos⁡[(2k+1)ωt]]+sinφ0[J0(D)+2∑k=1∞(-1)kJ2k(D)cos⁡(2kωt)]),S2(t)=-BJ2(C)×(cos⁡φ0[J0(D)+2∑k=1∞(-1)kJ2k(D)cos⁡(2kωt)]-sinφ0[2∑k=0∞(-1)kJ2k+1(D)cos⁡[(2k+1)ωt]]).According to (3), signals S1(t) and S2(t) have got infinite spectrum, which consists of harmonics. They are proportional to Jn(D), where n≥1.But during the practical implementation of the digital PGC scheme it is impossible to provide infinite passbands of digital low-pass filters. Anyway, all passbands will be limited by the digital scheme sampling frequency. Therefore, some high-order harmonics of signalsS1(t) and S2(t) might be filtered out.To determine the output signal dependence on the amplitude of the measured phase signal, further PGC technique operations on signalsS1(t) and S2(t) should be performed according to Figure 1 for several cases: when signals S1(t) and S2(t) contain only the first harmonic of the measured phase signal, two harmonics, three harmonics, and so forth. These cases will be matched to appropriate low-pass filters passbands.To simplify these calculations, low-pass filters are supposed to be ideal and thus all filtered out harmonics will not be present in filtered signals. The initial phase of the interferometer is considered to be constant.Then, in the simplest case, when low-pass filters passbands are equal to the fundamental frequency of the measured phase signal (i.e., low-pass filters passbands include the first harmonic of the measured phase signal and the input signal at the frequency of this harmonic could pass through low-pass filters without attenuation), signals (3) can be represented as
(4)S1(t)=-2BJ1(C)J1(D)cos⁡ωtcos⁡φ0-BJ1(C)J0(D)sinφ0,(5)S2(t)=2BJ2(C)J1(D)cos⁡ωtsinφ0-BJ2(C)J0(D)cos⁡φ0.Derivatives of (4) and (5) can be expressed as
(6)∂S1(t)∂t=2BJ1(C)J1(D)ωsinωtcos⁡φ0,(7)∂S2(t)∂t=-2BJ2(C)J1(D)ωsinωtsinφ0.Then cross-multiplication between signals (4) and (7), (5), and (6) yields
(8)S1(t)∂S2(t)∂t=4B2J1(C)J2(C)J12(D)ωsinωtcos⁡ωtsinφ0cos⁡φ0+2B2J1(C)J2(C)J0(D)J1(D)ωsinωtsin2φ0,(9)S2(t)∂S1(t)∂t=4B2J1(C)J2(C)J12(D)ωsinωtcos⁡ωtsinφ0cos⁡φ0-2B2J1(C)J2(C)J0(D)J1(D)ωsinωtcos⁡2φ0.Subtracting the signal (8) from (9) gives
(10)S2(t)∂S1(t)∂t-S1(t)∂S2(t)∂t=-2B2J1(C)J2(C)J0(D)J1(D)ωsinωt.After the integration, the output signal can be expressed as(11)Sout(t)=2B2J1(C)J2(C)J0(D)J1(D)cos⁡ωt.Performing the same mathematical manipulations with signalsS1(t) and S2(t) according to the PGC demodulation scheme (see Figure 1) in cases of wider low-pass filters passbands, the final equation of the output signal amplitude dependence on the input signal amplitude at the fundamental input signal frequency can be obtained:
(12)Sout(t)=2B2J1(C)J2(C)∑k=0N-1(2k+1)Jk(D)Jk+1(D)cos⁡ωt,
where N is equal to the number of useful harmonics of the measured phase signal that are arranged in low-pass filters passbands.To verify the obtained result (12), the special simulation was performed with various low-pass filter passbands: 500 Hz, 1000 Hz, and 1500 Hz. Corresponding theoretical dependences (according to (12)) and simulation results (normalized according to the dependence on B and C) are presented in Figure 3.Figure 3
Theoretical and simulation results: output signal amplitude dependencies on the measured phase signal amplitude (D) for various low-pass filter passbands: 1—500 Hz; 2—1000 Hz; 3—1500 Hz.The plot in Figure3 represents the output signal amplitude at the fundamental input signal frequency 500 Hz. According to Figure 3, the theoretical amplitude dependence of the output signal on the measured phase signal amplitude (see (12)) matches simulation results. Therefore, the output signal amplitude of the PGC scheme depends nonlinearly on the measured phase signal amplitude (for large input signal amplitudes) due to restrictions of low-pass filters passbands. It could lead to dynamic range limitations or measurement uncertainty of input phase signals.This dependence is of significant interest in terms of the practical implementation of the digital PGC technique, because it determines the dynamic range upper limit of the demodulation scheme. The wider the low-pass filters passbands are, the higher the dynamic range is.It should be noted that the demodulated signal is generally contaminated by high-order harmonics and their amplitude dependencies on the measured phase signal amplitude are also nonlinear. However, a detailed description of their exact behavior is beyond the scope of this paper.There is one more important result of low-pass filters passbands restrictions, which should be taken into account during the PGC technique implementation. It is the dependence of the dynamic range on the input signal frequency. This dependence (normalized according to the dependence onB and C) is presented in Figure 4. It should be noted that the dependence on C is known (see (1) and (12)) and the output signal might be corrected for this dependence by taking into account the once measured value of C in a real application.Figure 4
Simulation results: the dynamic range of the PGC demodulation scheme increases with the decrease in the input signal frequency (low-pass filter passbands: 500 Hz).As shown in Figure4, the dynamic range of the PGC scheme increases with the decrease in the input signal frequency. It can be explained by increasing the amount of useful harmonics of the input signal, which are arranged in fixed low-pass filter passbands. This result is consistent with the dynamic range analysis [13].In real demodulation schemes the dynamic range upper limit is determined by the required maximum amplitude of the measured phase signal. Therefore, low-pass filters passbands should be calculated according to this maximum amplitude using (12) during the PGC technique practical implementation.


## 4. Conclusion

In the present work it was shown for the first time that the dependence of the dynamic range of the PGC technique on low-pass filters passbands is nonlinear for large input signal amplitudes because of low-pass filters passbands restrictions. The nonlinear character of this dependence could cause dynamic range limitations or measurement uncertainty of input phase signals (see (12) and Figure 3).According to obtained results, the additional calculation of low-pass filters passbands should be performed in accordance with requirements to the amplitude dependence of the output signal and the necessary dynamic range of the PGC demodulation scheme.



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*Source: 815108-2014-03-17.xml*