This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIE.2020.3003634, IEEE Transactions on Industrial Electronics IEEE TRANSACTIONS ON INDUSTRIAL ELECTRONICS
Design of a New Stress Wave Communication Method for Underwater Communication Sihong He, Ning Wang, Member, IEEE, Siu-Chun Ho, Junxiao Zhu, Member, IEEE, and Gangbing Song, Member, IEEE
Abstract—Underwater communication is crucial for sub- U. S. Navy, allowing the ELF waves to penetrate seawater at sea engineering. Currently, although a variety of available depths of less than 300 meters for data transmission with the technologies are available for underwater communication, submarines, was considered as the only successfully deployed almost all of them are highly dependent on the conditions of the subsea environment. Hence, underwater communi- underwater radio frequency technology[4]. cation is still a challenging issue. This paper develops a FSO utilizes optical carrier waves to deliver packaged data new stress wave communication method that can be imple- in free space. FSO can reach up to 40 Gbps [5]. However, mented along steel pipes for underwater data transmission. In this work, we analyze stress wave propagation along in marine environments, FSO communication is vulnerable pipelines, and the corresponding channel response shows to absorption, scattering and dispersion, and communication the features of dispersion and frequency selectivity. Thus, distance is highly dependent on the state (e.g. turbidity) of a suitable carrier frequency is then selected and binary the subsea environment [6]. So far, in most proposed under- shift keying (BPSK) is applied to encode information into water optical communications, the scale of communication the carrier stress wave. The proposed single-input-single- output (SISO) communication system was implemented on distance ranges from meters to tens of meters [7-9]. MI a steel pipe and experiments were conducted both when is an emerging communication method for underwater or in air and seawater. Results demonstrate the validity and underground wireless communications relying on time variant stability of the proposed method. The communication data magnetic fields for data transmission. The propagation speed rate of the method can reach 1000 bps with a low bit error and data rate of MI can reach high values and can compensate rate (BER). The proposed method shows great promise for enabling underwater communication with lower loss and for the presence of propagation delay. MI communication is longer range than conventional underwater communication much less susceptible to underwater environment than other methods. technologies. However, recent mathematical modeling [10-12] Index Terms—Stress Wave Communication (SWC); Un- of MI underwater communication in complex environments derwater Communication; Binary Phase Shift Keying Mod- indicated the transmission range is still limited within 10 to ulation (BPSK); Piezoelectric Transducers; Single Input- 100 meters. AW is the most popular underwater communica- Single Output (SISO); Bit Error Rate (BER). tion technique based on acoustic waves transmission through both stationary and mobile nodes. In recent years, tremendous I. INTRODUCTION progress has been made on modulation schemes of underwater AWC [13-16]. Acoustic waves have demonstrated a longer A. Background and Motivation traveling distance than both EM waves and FSO. However, the main disadvantages of AW underwater communications U NDERWATER communication plays a critical role in include multipath propagation, limited bandwidth, and low many subsea engineering applications and researches, speed [17] due to time-varying and complex underwater such as offshore exploration, oceanographic data acquisition, environment. Recently, efforts have been made to mitigate pollution monitoring, climate monitoring, among others[1]. multipath effect of underwater AW multiple-input-multiple- Currently, there are four major communication methods for output (MIMO) communications [18-20]. underwater communication, including Radio Frequency (RF) communication, Free-space Optical (FSO) communication, Stress wave communication (SWC) method and variations Magnetic Induction (MI) communication and Acoustic Wave of the method have recently been proposed [21-23], and (AW) communication[1]. RF communications utilize electro- compared to the existing underwater communication methods, magnetic waves as the carrier wave, and transmit data within stress wave communications can reach a longer range with a the 3kHz to 300GHz bandwidth. In contrast to that EM waves relatively fast transmission speed. Stress wave communications possess the capability of penetrating through most objects and are mainly focused on two aspects: 1) through-metal-wall data traveling long distances when in air, they are susceptible to transmission and 2) logging while drilling (LWD). The most electromagnetic interferences and rapidly attenuate in aquatic common through-metal-wall data transmission system com- environments due to the high electrical conductivity and prises of one external transducer and one internal transducer permittivity of water. Particularly, seawater will cause EM coupled together through the conducting medium[24,25]. Re- waves to attenuate exponentially with respect to increasing garding stress wave communication in LWD, recent researches frequencies[2, 3]. Around twenty years ago, the extremely suggest that the estimated maximum achievable transmission low frequency (ELF) communications system set up by the speed reached 22 kbps using adaptive OFDM along the
0278-0046 (c) 2020 IEEE. Personal use is permitted, but republication/redistribution requires IEEE permission. See http://www.ieee.org/publications_standards/publications/rights/index.html for more information. Authorized licensed use limited to: University of Houston. Downloaded on August 01,2020 at 21:57:48 UTC from IEEE Xplore. Restrictions apply. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIE.2020.3003634, IEEE Transactions on Industrial Electronics IEEE TRANSACTIONS ON INDUSTRIAL ELECTRONICS
drilling string[26,27]. Recent implementation of stress wave to the analysis results, BPSK is the best candidate for the data communication on pipeline structures have opened the door modulation scheme due to its simplicity, low BER and high for potential application in subsea communications. Jin et al. performance. developed a time reversal based pulse position modulation 3) To achieve the underwater communication, we imple- (TR-PPM) stress wave communication method along a metal mented a single input-single output (SISO) communication pipe[28-30]. Huang et al. applied an Electro Magnetic Acous- system successfully. The experimental result shows that the tic Transducer (EMAT) and a piezoceramic sensor to develop communication data rate of our method can reach 1000 bps, a stress wave communication channel through a metal pipe and it has the low BER. and accomplished data transmission based on Amplitude Shift Keying (ASK) modulation[31]. Joseph et al. demonstrated To the best knowledge of the authors, this paper is the stress wave communication across one water-filled pipe in first reported instance of stress wave communication method the urban water distribution systems (WDSs) using amplitude with BPSK modulation along the pipeline structure for the modulation (AM) and achieved a data rate up to 100 bps[32]. underwater communication. To demonstrate the feasibility and stability of the proposed stress wave communication method, Stress wave (SW) propagation along a pipeline structure is an underwater communication experiment was implemented. not heavily affected by the surrounding underwater environ- The experimental results demonstrated the effectiveness of this ment. Moreover, SW travels at a relatively fast speed along new stress wave communication method for the underwater metal medium with low cost. Thus, it is a potentially reliable long distance communication. method to be utilized for underwater communication, especial- ly long-distance communication. However, until now, there is The rest of this paper is organized as follows. In Section only few reported works related to underwater stress wave II, the design process of the new stress wave communication communication. In 2015, Chakraborty et al. developed a chirp method is presented. Section III presents the experiment and -on-off keying (Chirp-OOK) based stress wave communication result discussion to illustrate the effectiveness and applicabil- method to help with frequency selectivity of the channel along ity of the proposed communication method. The concluding a 4.8-meter pipe and stated the achievement of underwater remarks and future works are summarized in Section IV. data transmission with a data rate of 100 bps[33]. Therefore, it is promising to explore methods of achieving underwater II. A NEW STRESS WAVE COMMUNICATION METHOD stress wave communications, which can be implemented on WITH BPSK MODULATION commonly found underwater pipelines in subsea oil and gas industry. The goal of this paper is to address unsolved essential issues for the underwater communication discussed in Section B. Research Problem and Contributions of this Study I. To develop the stress wave communication method, we begin from the fundamental analysis of the research problem. A new stress wave communication method is proposed in Through the development of the theory behind the mathe- this paper to address the reported drawbacks and unsolved matical model, the key components of the communication essential issue in the existing communication methods for long method can be determined; from there, the new communi- distance underwater communication. The contributions of the cation method can be fleshed out in full detail. new method are summarized in the following three aspects: 1) To characterize the channel features, we analyzed the A. Principle Statement stress wave propagation in multiple metal pipeline structures. 2) To identify a fitting carrier wave frequency located The detailed development of the proposed stress wave within the pass-band and select an appropriate data modulation communication method is shown in Fig. 1. The development scheme, we utilized the least square (LS) estimation method to procedure can be summarized in three steps: 1) carrier wave determine the channel response of the metal pipe. According frequency selection, 2) selection of data modulation scheme, and 3) BPSK based communication method setup . The detailed description of each step is presented as follows. Firstly, stress wave propagation in metal pipeline structures is analyzed. Meanwhile, the channel response is evaluated for the design of the data modulation scheme.
TABLE I: VELOCITIES OF STRESS WAVE IN DIFFERENT METAL MATERIALS
Wave Mode Steel Copper Iron Aluminium
Longitudinal, CL 5000 (m/s) 3650 (m/s) 3900 (m/s) 5000 (m/s)
Transversal, CT 3200 (m/s) 2250 (m/s) 2450 (m/s) 3050 (m/s) Fig. 1: Flow chart to explain the proposed method.
0278-0046 (c) 2020 IEEE. Personal use is permitted, but republication/redistribution requires IEEE permission. See http://www.ieee.org/publications_standards/publications/rights/index.html for more information. Authorized licensed use limited to: University of Houston. Downloaded on August 01,2020 at 21:57:48 UTC from IEEE Xplore. Restrictions apply. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIE.2020.3003634, IEEE Transactions on Industrial Electronics IEEE TRANSACTIONS ON INDUSTRIAL ELECTRONICS
Secondly, according to the results of response analysis, the where θ0 is an arbitrary constant. As the functions should binary phase shift keying (BPSK) scheme has been selected be periodic in the circumferential direction for stress wave for the data modulation in favor of its low bit error rate propagating in the axial direction, m =0or m ∈ Z. (BER) and simplicity among the different phase shift keying The general solution to the waves propagating in the axial (PSK) schemes. Thus, BPSK can be easily integrated into the direction of this hollow cylinder is given by Eq.(2), Eq.(3), proposed communication method. Eq.(4), and Eq.(5). The Bessel functions of second kind Finally, based on the BPSK modulation scheme, a new should be retained in this case, because the presence of both stress wave communication method has been designed and incoming (toward the center) and outgoing (away from the tested. center) stress waves is necessary to satisfy the traction-free boundary conditions on both the inner and outer surfaces. For Torsion motion, T (m, r), uθ should be the only nonzero B. Theoretical Background for Proposed Method displacement component. Furthermore, it is independent of θ. These conditions are met by setting An = Bn = m =0, n ∈ According to the working process of the proposed method π {1, 2} θ0 = as shown in Fig. 1, the corresponding theoretical background , and 2 in the integral solution. As Longitudinal, mathematical models are presented as follows. L(m, r), stress waves refer to the axially symmetrical motion 1) Evaluation of Stress Wave Propagation in Pipeline in the cylinder. The presence of displacement components Structures: Stress wave propagation in pipelines can be cat- characterize the longitudinal stress wave in the radial and θ egorized into three types of modes, namely the longitudinal axial directions, and none in the -direction. Vanishing of the mode (L), Transversal mode (T) (or shear wave) and flexural determinant can yield the corresponding dispersion equations. mode (F) (a type of surface wave) [34-36]. Among them, 2) Channel Response: Channel response is important in longitudinal mode and Transversal mode are symmetric, while communication for scheme design and data recovery. In our flexural mode is anti-symmetric. In Table I, the velocities research, least square (LS) estimation method [39] is utilized. of stress wave in multiple metal materials are listed [37]. LS estimation uses the input and measured output data to build To select a suitable carrier wave channel, a mathematical a model. The model coefficients are obtained by minimizing model is needed [38]. As shown in Fig.2, a pipeline structure the errors between the measured output and predicted output. (r, θ, z) Φ with cylindrical coordinate system, , we assume Given the value of x, the best prediction of y (mean square A is a scalar function and is a vector function, then any error ) is the mean f(x) of y given y. thus, displacement field, u, can be expressed in the following manner y = f(x)+noise. u = Φ + ×A. (1) ( ) For time-harmonic waves propagating in the axial (the z- Here, the function f x is called a regression function. axis) direction of the cylindrical wave guide, the displacement It is to be estimated from sampling n covariables and their ( ) ··· ( ) potentials can be obtained by the following equations. responses x1,y1 , , xn,yn . Suppose f(x) is known up to a finite number p ≤ n of ϕ = φ(r)cos(mθ + θ0)exp[i(kzz − wt)], (2) parameters β =(β1, ··· ,βp) , that is, f(x)=fβ(x).We estimate β by the value β that gives the best fit to the data. ψr = ψr(r)sin(mθ + θ0)exp[i(kzz − wt)], (3) The least squares estimator, which is denoted by β , is that ψθ = ψθ(r)cos(mθ + θ0)exp[i(kzz − wt)], (4) value of b that minimizes
ψz = ψz(r)sin(mθ + θ0)exp[i(kzz − wt)]. (5) n 2 (yi − fb(xi)) , (6) i=1
over all possible b. Then, the linear regression method is used to optimize the least squares estimator. We consider fβ(x) is a linear function of β, then
fβ(x)=x1β1 + ···+ xpβp, (7)
where (x1, ··· ,xp) stand for the observed variables used in fβ(x). Fig. 2: A cylindrical waveguide with the cylindrical To write down the least squares estimator for the linear coordinate system. regression model, it is convenient to use matrix notation. Let
0278-0046 (c) 2020 IEEE. Personal use is permitted, but republication/redistribution requires IEEE permission. See http://www.ieee.org/publications_standards/publications/rights/index.html for more information. Authorized licensed use limited to: University of Houston. Downloaded on August 01,2020 at 21:57:48 UTC from IEEE Xplore. Restrictions apply. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 10.1109/TIE.2020.3003634, IEEE Transactions on Industrial Electronics IEEE TRANSACTIONS ON INDUSTRIAL ELECTRONICS
Fig. 3: Basic rule of BPSK.
y =(y1, ··· ,yn) , and X be the n × p data matrix of the n 3) BPSK Modulation and Demodulation: Generally, the observations on the p variables phase-coherent modulation and demodulation procedure of ⎡ ⎤ BPSK can be depicted as Fig.3 [40]. The mathematical model x1,1 ··· x1,p ⎢ . . ⎥ of BPSK is presented as follows. X = ⎣ . ··· . ⎦ =(X1, ··· ,Xp), . . Assume the transmitting information can be modeled as an xn,1 ··· xn,p N-bit binary sequence ai ∈{0, 1}, and i ∈{1, 2,,N}. Then, where Xj is the column vector containing the n observations the modulating signal P (t) is deduced by converting the binary on variable j, j ∈{1, ··· ,n}. Denote the squared length of sequence to a non-return-to-zero signal, 2 n 2 an n-dimensional vector V by V = V V = i=1 vi . To construct confidence intervals for the components of β , ⎛ ⎞ 2i − 1 or linear combinations of these components, one needs an N t − · Tb ⎜ 2 ⎟ estimator of the covariance matrix of β. The covariance matrix P (t)= (2ai − 1) · rect ⎝ ⎠ . (8) Tb of estimator β is i=1 (X X)−1σ2, 2 Tb where σ is the variance of the noise. Finally, a confidence where represents the bit duration interval for βj is obtained by taking the least squares estimator Let C(t) denote the carrier wave with the following prop- βj± a margin as follows erties,