Dynamic Event-Triggered Interval Observer-Based Fault Detection for a Class of Nonlinear Cyber–Physical Systems with Disturbance

Abstract

This paper investigates the problem of interval estimation and fault detection for nonlinear cyber–physical systems (CPSs) subject to disturbances and random actuator/sensor faults. First, with the purpose of reducing the burden of data transmission, we introduce the dynamic event-triggered mechanism (DETM). For systems violating the non-negativity condition, a coordinate transformation method is applied to enhance the design flexibility. Then, the dynamic event-triggered interval observer (DETIO) is constructed and the effectiveness of DETIO is validated by demonstrating the ultimate uniform boundedness of the error system. The fault detection is achieved by considering faults in the CPSs and continuously monitoring residual signals. Finally, two numerical simulations under both faulty and fault-free conditions are shown to prove the effectiveness and superiority of the designed DETIO-based fault detection method.

1. Introduction

In past few decades, CPSs have been widely studied by the scientific community. CPSs are intelligent systems that deeply integrate the capabilities of computation, communication, and physical processes [1]. Owing to their unique capability to bridge the physical and cyber worlds, CPSs have already been applied in many areas, e.g., the electric power industry [2] and water systems [3]. However, as CPSs grow more complex and face unknown disturbances, the tasks of estimating states and detecting faults efficiently also pose challenges. For the state estimation problems in CPSs, one common method is the observer design technique. For example, ref. [4] investigated a switched observer for CPSs via a set cover approach. Ref. [5] focused on a sliding mode observer design for CPSs. Ref. [6] analyzed the estimation stability in the network system under attack. Furthermore, the interval observer (IO), as an effective tool for obtaining the estimated state boundaries of the system with unknown bounded disturbances and measurement noises, is also introduced to CPSs [7,8].

Meanwhile, due to the high demand for communication and data transmission in CPSs, the event-triggered mechanism (ETM) has been introduced and gained significant research interest. The fundamental principle of ETM is to decide the trigger through system states, instead of the conventional mechanism that triggers actions with fixed sampling intervals. The authors of [9] introduced a periodic technique to ETM and also applied it to both static state-feedback and dynamic output-based controllers. In [10], researchers combined the ETM and observer technique for the control of positive nonlinear multi-agent systems. To further reduce the burden while ensuring the performance of the system, the dynamic event-triggered mechanism was introduced [11,12,13]. Ref. [11] imported an interval dynamic variable which forms the DETM. Researchers in [12] investigated a dynamic periodic ETM to decrease asynchronous behavior generated from nonuniform communication delays. Ref. [13] applied a DETM to investigate the interval estimation problem for Euler–Lagrange systems under stealthy attack. Moreover, in order to precisely estimate the states with uncertain disturbance during communications, the event-triggered interval observer (ETIO) was proposed in [14]. Furthermore, ref. [15] took advantage of DETM to estimate the boundaries of the system with unknown but bounded disturbance and noise using a zonotope-based approach. Hence, ETM offers a new approach to save communication resources for solving the estimation problem.

In addition, for CPSs with actuator/sensor faults, ensuring system stability requires effective fault detection. The main fault detection approaches can be broadly classified into model-based [16,17], data-driven [18,19,20], and hybrid approaches [21]. Among these, the IO-based fault detection method has gained much attention, considering its strong robustness against uncertainties. For example, ref. [22] proposed an IO-based fault detection approach with unknown input for CPSs under attacks. Similarly, in [23], for a T-S fuzzy system, the fault detection method was established via a zonotope-based IO. Ref. [24] designed a sliding mode IO to detect faults and eliminate uncertainties with the existence of the measurement noise in high-speed railway traction motors. However, as far as the authors are aware, research on fault detection based on interval estimation, which integrates DETM in CPSs, remains limited.

As a result, a DETIO design is developed in this paper for fault detection problems of a class of nonlinear CPSs. The DETIO fault detection design relies on its stability, which is mainly derived from a combination of the Lyapunov stability theory and the positive system theory. Moreover, in this paper, we discuss the utilization of the coordinate transformation method under the case where the error system is not non-negative. The contributions presented in this paper can be briefly described as follows:

(1)

The DETM that possesses a dynamic interval variable, which depends on the system states, is introduced to save communication resources in CPSs; compared to the static ETM, it can save more network resources while guaranteeing the stability of the systems.

(2)

A DETIO is designed for CPSs under actuator/sensor faults. The mentioned DETIO approach can accurately obtain the bounded estimation of the states without wasting additional data transmission resources.

(3)

The designed DETIO is applied to fault detection in CPSs. By bounding the state estimates with the DETM, this fault detection method reduces computational load and ensures the robustness of the system.

The remainder of this paper is summarized as follows. Section 2 focuses on the preliminaries and problem statements. Section 3 gives the DETIO frame design. Section 4 gives some numerical examples to simulate the circumstances of fault-free and under faults, respectively. Finally, we present the conclusion in Section 5.

Notations: Given a matrix $z=\left[\begin{array}{c}{z}_{ij}\end{array}\right]\in {\mathbb{R}}^{m\times n}$, $z\ge 0$ if $z_{ij}\ge 0$. For a matrix $E\in {\mathbb{R}}^{m\times m}$ and $E^T=E$, $E\prec 0(E\succ 0)$ indicates that E is a negative (positive) definite matrix. Moreover, given a matrix $A\in {\mathbb{R}}^{m\times n}$, we define that $A^{+}=max\{A,0\}$ and $A^{-}=A^{+}-A$.

2. Preliminaries and Problem Statement

The nonlinear CPS model in this paper is considered as follows:

$$\left\{\begin{array}{c}\begin{array}{cc}\hfill & x(k+1)=Ax\left(k\right)+Bu\left(k\right)+F\left(x\right(k\left)\right)+D\delta \left(k\right)+Ef\left(k\right),\hfill \\ \hfill & y\left(k\right)=Cx\left(k\right),\hfill \end{array}\end{array}\right.$$

(1)

where $x\in {\mathbb{R}}^n$, $y\in {\mathbb{R}}^n$ and $u\in {\mathbb{R}}^n$ represent the state, output, and control input of the system, respectively. $\delta \in {\mathbb{R}}^n$ is an unknown disturbance, $f\in {\mathbb{R}}^n$ denotes the actuator fault. The matrices A, B, D, C, and E, along with the nonlinear function $F\left(x\right)$, with appropriate dimensions are known. To save network resources in a CPS, the DETM is introduced to detect faults. In this study, we propose the following DETM for the system (1):

$$t_0=0,t_{k+1}=inf\left\{t>t_k|\Gamma \left(k\right)+\alpha [\eta y^T\left(k\right)y\left(k\right)-e_y^T\left(k\right)e_y\left(k\right)\le 0]\right\},$$

(2)

where $\alpha \ge 0$, $0<\eta <0.5$. And the non-negative function $\Gamma \left(k\right)$ satisfies the following equation:

$$\Gamma (k+1)=-\lambda \Gamma \left(k\right)+\eta y^T\left(k\right)y\left(k\right)-e_y^T\left(k\right)e_y\left(k\right),$$

(3)

where $\Gamma \left(0\right)={\Gamma }_0\ge 0$ and $\lambda$ is a positive scalar.

Assumption 1.

Suppose that there are constant vectors ${\delta }_k^{+}$ and ${\delta }_k^{-}$; then, the disturbance ${\delta }_k$ holds:

$${\delta }_k^{-}\le {\delta }_k\le {\delta }_k^{+}.$$

(4)

Assumption 2.

Given a function $f(x,y)$, if, for any $(x,y_1),(x,y_2)$, we have a Lipschitz constant c that satisfies the following inequality:

$$\parallel f(x,y_1)-f(x,y_2)\parallel \le c\parallel y_1-y_2\parallel .$$

(5)

Then, the function $f(x,y)$ is Lipschitz continuous in y with constant c.

Lemma 1

([25]). For a given Lipschitz function $F\left(x\right)$ that is globally differentiable, the following equation holds:

$$F\left(x\right)=g_1\left(x\right)-g_2\left(x\right).$$

(6)

where $g_1\left(x\right)$ and $g_2\left(x\right)$ are two globally differentiable and increasing Lipschitz functions.

Lemma 2

([25]). Consider the function $F\left(x\right)$ in Lemma 1. The Lipschitz function $\overline{F}(x_m,x_n)$ exists and is globally differentiable, such that

$$F\left(x\right)=\overline{F}(x,x),$$

$${\displaystyle \frac{\partial \overline{F}}{\partial x_m}\ge 0,\frac{\partial \overline{F}}{\partial x_n}\le 0.}$$

From Lemmas 1 and 2, the lower and upper boundaries subject to the nonlinear function $G(x,x)$ can be derived as

$$\overline{F}(x^{-},x^{+})\le F(x,x)\le \overline{F}(x^{+},x^{-}).$$

(7)

Lemma 3

([26]). For a vector $v\in {\mathbb{R}}^{n\times 1}$, given a constant matrix $M\in {\mathbb{R}}^{n\times n}$ and the vector v satisfying $v^{-}\le v\le v^{+}$,

$$M^{+}{v}^{-}-M^{-}{v}^{+}\le Mv\le M^{+}{v}^{+}-M^{-}{v}^{-}.$$

(8)

Lemma 4

([25]). For the functions $F\left(x\right)$, $\overline{F}(x^{-},x^{+})$ and $\overline{F}(x^{+},x^{-})$ mentioned above, there exist known constant matrices $F_a,F_b,F_c,$ and $F_d$ such that

$$\left\{\begin{array}{c}\begin{array}{c}\overline{F}(x^{+},x^{-})-F(x,x)\le F_a\overline{e}+F_b\underline{e},\hfill \\ F(x,x)-\overline{F}(x^{-},x^{+})\le F_c\overline{e}+F_d\underline{e},\hfill \end{array}\end{array}\right.$$

(9)

where $\overline{e}=x^{+}-x$ and $\overline{e}=x-x^{-}$.

Lemma 5

([27]). Given the following systems

$$\left\{\begin{array}{c}\begin{array}{c}{x}_{k+1}=K{x}_k+F\left(x_k\right),\hfill \\ x_0\ge 0,\hfill \end{array}\end{array}\right.$$

(10)

where the constant matrix K is non-negative and the function $F\left(x_k\right)\ge 0$, we can obtain $x_k\ge 0$ for all $k\ge 0$.

Lemma 6

([28]). If there are two arbitrary matrices G, $V\in {\mathbb{R}}^{n\times n}$ and a constant β, we have

$$G^{T}V+V^{T}G\le {\displaystyle \frac{1}{\beta }}{G}^{T}PG+\beta V^T{P}^{-1}V,$$

(11)

where the matrix $P\succ 0$ and $\beta >0$.

Remark 1.

For the above DETM in (2) and (3), let $\alpha \ge 0$, $\eta >0$, and ${\Gamma }_0\ge 0$. Then, for $\forall k>0$, the dynamic interval variable $\Gamma \left(k\right)$ holds:

$$\Gamma \left(k\right)\ge 0.$$

(12)

Moreover, for cases where $\alpha =0$, the DETM will degrade to the static event-triggered mechanism.

3. Main Results

3.1. Design of the Fault Detection DETIO

According to the discussion above, for system (1), we propose the following fault detection DETIO:

$$\left\{\begin{array}{c}\begin{array}{cc}\hfill x^{+}(k+1)=& A{x}^{+}\left(k\right)+Bu\left(k\right)+\overline{F}(x^{+}\left(k\right),x^{-}\left(k\right))+{\mu }^{+}\left(k\right)\hfill \\ \hfill & +\overline{h}\left(k\right)+L(y_{{\tau }_p}\left(k\right)-C{x}^{+}\left(k\right)),\hfill \end{array}\\ x^{-}(k+1)=A{x}^{-}\left(k\right)+Bu\left(k\right)+\overline{F}(x^{-}\left(k\right),x^{+}\left(k\right))+{\mu }^{-}\left(k\right)\\ +\underline{h}\left(k\right)+L(y_{{\tau }_p}\left(k\right)-C{x}^{-}\left(k\right)),\end{array}\right.$$

(13)

$$\left\{\begin{array}{c}\begin{array}{c}\hfill r^{+}\left(k\right)=y\left(k\right)-C{x}^{-}\left(k\right),\\ \hfill r^{-}\left(k\right)=y\left(k\right)-C{x}^{+}\left(k\right),\end{array}\end{array}\right.$$

(14)

where $x^{+}\left(k\right)$ and $x^{-}\left(k\right)$ are estimates of $x\left(k\right)$, ${\mu }^{+}\left(k\right)=D^{+}{\delta }^{+}\left(k\right)-D^{-}{\delta }^{-}\left(k\right)$ and ${\mu }^{-}\left(k\right)=D^{+}{\delta }^{-}\left(k\right)-D^{-}{\delta }^{+}\left(k\right)$, $\overline{h}\left(k\right)=L^{-}{e}_y^{+}\left(k\right)-L^{+}{e}_y^{-}\left(k\right)$, and $\underline{h}\left(k\right)=L^{-}{e}_y^{-}\left(k\right)-L^{+}{e}_y^{+}\left(k\right)$. $r^{+}$ and $r^{-}$ are the interval residual vectors used to detect the fault. The gain L of the interval observer will be discussed in the next part.

Theorem 1.

If $A-LC$ satisfies the non-negativity condition and $x^{-}\left(0\right)\le x\left(0\right)\le x^{+}\left(0\right)$. For all $k\in \mathbb{N}$, the following inequality holds:

$$x^{-}\left(k\right)\le x\left(k\right)\le x^{+}\left(k\right).$$

(15)

Proof. 

Define $e^{+}\left(k\right)=x^{+}\left(k\right)-x\left(k\right)$ and $e^{-}\left(k\right)=x\left(k\right)-x^{-}\left(k\right)$; then, we can deduce that

$$\left\{\begin{array}{c}\begin{array}{cc}\hfill e^{+}(k+1)=& (A-LC)e^{+}\left(k\right)-F\left(x\left(k\right)\right)+\overline{F}(x^{+}\left(k\right),x^{-}\left(k\right))\hfill \\ & +e_{\delta }^{+}\left(k\right)+L{e}_y\left(k\right)+\overline{h}\left(k\right)-Ef\left(k\right),\hfill \\ \hfill e^{-}(k+1)=& (A-LC)e^{-}\left(k\right)-\overline{F}(x^{-}\left(k\right),x^{+}\left(k\right))+F\left(x\left(k\right)\right)\hfill \\ & +e_{\delta }^{-}\left(k\right)-\underline{h}\left(k\right)-L{e}_y\left(k\right)+Ef\left(k\right),\hfill \end{array}\end{array}\right.$$

(16)

where $e_{\delta }^{+}\left(k\right)={\mu }^{+}\left(k\right)-D\delta \left(k\right)$ and $e_{\delta }^{-}\left(k\right)=D\delta \left(k\right)-{\mu }^{-}\left(k\right)$. By Lemma 3, we can obtain that $e_{\delta }^{-}\left(k\right)\ge 0$, $e_{\delta }^{+}\left(k\right)\ge 0$. Similarly,

$$\left\{\begin{array}{c}L{e}_y\left(k\right)+\overline{h}\left(k\right)=L{e}_y\left(k\right)-(L^{+}{e}_y^{-}\left(k\right)-L^{-}{e}_y^{+}\left(k\right))\ge 0,\\ -\underline{h}\left(k\right)-L{e}_y\left(k\right)=(L^{+}{e}_y^{+}\left(k\right)-L^{-}{e}_y^{-}\left(k\right))-L{e}_y\left(k\right)\ge 0.\end{array}\right.$$

(17)

If $A-LC$ satisfies the non-negative condition, and the initial conditions (15) hold, then the positivity of the error system (16) can be proven according to Lemma 5. Therefore, we can also deduce that $x^{-}\left(k\right)\le x\left(k\right)\le x^{+}\left(k\right),\forall k\ge 0$, which completes the proof.   □

3.2. Coordinate Transformation-Based Fault Detection DETIO Design

Given a situation that $A-LC$ is not a non-negative matrix, we can adopt the coordinate transformation technique to build the DETIO for CPSs. Denote $w\left(k\right)=Hx\left(k\right)$, $\overline{A}=HA{H}^{-1}$, $\overline{B}=HB$, $\overline{C}=C{H}^{-1}$, $\overline{D}=HD$, $\overline{E}=HE$, and we can rewrite the system (3) as follows:

$$\left\{\begin{array}{c}\begin{array}{c}w(k+1)=\overline{A}w\left(k\right)+\overline{B}u\left(k\right)+HF\left(H^{-1}w\left(k\right)\right)+\overline{D}\delta \left(k\right)+\overline{E}f\left(k\right),\hfill \\ y\left(k\right)=\overline{C}w\left(k\right).\hfill \end{array}\end{array}\right.$$

(18)

To obtain the estimated boundaries of $F\left(x\right)$, it is denoted that

$$\left\{\begin{array}{c}\begin{array}{c}\phi (w^{+}\left(k\right),w^{-}\left(k\right))=\overline{F}(H_r^{+}{w}^{+}\left(k\right)-H_r^{-}{w}^{-}\left(k\right),H_r^{+}{w}^{-}\left(k\right)-H_r^{-}{w}^{+}\left(k\right)),\hfill \\ \phi (w^{-}\left(k\right),w^{+}\left(k\right))=\overline{F}(H_r^{+}{w}^{-}\left(k\right)-H_r^{-}{w}^{+}\left(k\right),H_r^{+}{w}^{+}\left(k\right)-H_r^{-}{w}^{-}\left(k\right)),\hfill \end{array}\end{array}\right.$$

(19)

where $H_r=H^{-1}$, $w^{-}\left(k\right)$, and $w^{+}\left(k\right)$ represent the lower and upper estimations of $w\left(k\right)$, respectively. According to Lemmas 3 and 4, the following inequalities are deduced as

$$\begin{array}{cc}\hfill {\overline{F}}_w(w^{-},w^{+})& =H^{+}\phi (w^{-},w^{+})-H^{-}\phi (w^{+},w^{-})\le H\overline{F}\left(H^{-1}w\right)\hfill \\ \hfill & \le H^{+}\phi (w^{+},w^{-})-H^{-}\phi (w^{-},w^{+})={\overline{F}}_w(w^{+},w^{-}).\hfill \end{array}$$

(20)

Then, the fault detection DETIO framework is constructed as follows:

$$\left\{\begin{array}{c}\begin{array}{cc}\hfill w^{+}(k+1)=& \overline{A}{w}^{+}\left(k\right)+\overline{B}u\left(k\right)+{\overline{F}}_w(w^{+}\left(k\right),w^{-}\left(k\right))+d^{+}\left(k\right)\hfill \\ \hfill & +\overline{\eta }\left(k\right)+L(y_{{\tau }_p}\left(k\right)-\overline{C}{w}^{+}\left(k\right)),\hfill \\ \hfill w^{-}(k+1)=& \overline{A}{w}^{-}\left(k\right)+\overline{B}u\left(k\right)+{\overline{F}}_w(w^{-}\left(k\right),w^{+}\left(k\right))+d^{-}\left(k\right)\hfill \\ \hfill & +\underline{\eta }\left(k\right)+L(y_{{\tau }_p}\left(k\right)-\overline{C}{w}^{-}\left(k\right)),\hfill \end{array}\end{array}\right.$$

(21)

$$\left\{\begin{array}{c}\begin{array}{c}\hfill {\overline{r}}^{+}\left(k\right)=y\left(k\right)-\overline{C}{w}^{-}\left(k\right),\\ \hfill {\overline{r}}^{-}\left(k\right)=y\left(k\right)-\overline{C}{w}^{+}\left(k\right),\end{array}\end{array}\right.$$

(22)

where

$$\left\{\begin{array}{c}\begin{array}{cc}\hfill d^{+}\left(k\right)=& {\overline{D}}^{+}{\delta }^{+}\left(k\right)-{\overline{D}}^{-}{\delta }^{-}\left(k\right)\hfill \\ \hfill d^{-}\left(k\right)=& {\overline{D}}^{+}{\delta }^{-}\left(k\right)-{\overline{D}}^{-}{\delta }^{+}\left(k\right)\hfill \end{array}\end{array}\right.and\left\{\begin{array}{c}\begin{array}{c}\hfill \overline{\eta }\left(k\right)=L^{-}{e}_y^{+}\left(k\right)-L^{+}{e}_y^{-}\left(k\right)\\ \hfill \underline{\eta }\left(k\right)=L^{-}{e}_y^{-}\left(k\right)-L^{+}{e}_y^{+}\left(k\right)\end{array}\end{array}\right..$$

(23)

Since the transformation matrix H is nonsingular, using the initial condition, it can be obtained that

$$w^{-}\left(0\right)\le w\left(0\right)\le w^{+}\left(0\right),$$

(24)

where

$$\left\{\begin{array}{c}\begin{array}{c}{w}^{+}\left(0\right)=H^{+}{x}^{-}\left(0\right)-H^{-}{x}^{+}\left(0\right),\hfill \\ w^{-}\left(0\right)=H^{+}{x}^{+}\left(0\right)-H^{-}{x}^{-}\left(0\right).\hfill \end{array}\end{array}\right.$$

(25)

Defining ${ϵ}^{+}\left(k\right)=w^{+}\left(k\right)-w\left(k\right)$ and ${ϵ}^{-}\left(k\right)=w\left(k\right)-w^{-}\left(k\right)$. Then, the dynamic errors can be deduced as

$$\left\{\begin{array}{c}\begin{array}{cc}\hfill {ϵ}^{+}(k+1)=& (\overline{A}-L\overline{C}){ϵ}^{+}\left(k\right)+{\overline{F}}_w(w{\left(k\right)}^{+},w{\left(k\right)}^{-})-H\overline{F}\left(H^{-1}w\left(k\right)\right)\hfill \\ \hfill & +e_{\Delta }^{+}\left(k\right)+L{e}_y\left(k\right)+\overline{\eta }\left(k\right)-\overline{E}f\left(k\right),\hfill \end{array}\\ {ϵ}^{-}(k+1)=(\overline{A}-L\overline{C}){ϵ}^{-}\left(k\right)+H\overline{F}\left(H^{-1}w\left(k\right)\right)-{\overline{F}}_w(w{\left(k\right)}^{-},w{\left(k\right)}^{+})\hfill \\ +e_{\Delta }^{-}\left(k\right)-L{e}_y\left(k\right)-\underline{\eta }\left(k\right)+\overline{E}f\left(k\right),\end{array}\right.$$

(26)

where $e_{\Delta }^{+}\left(k\right)=d^{+}\left(k\right)-\overline{D}\delta \left(k\right)$ and $e_{\Delta }^{-}\left(k\right)=\overline{D}\delta \left(k\right)-d^{-}\left(k\right)$.

Remark 2.

For CPSs that do not satisfy the non-negative condition, through the coordinate transformation method, we can still construct a matrix H, causing $A-LC$ to be non-negative after transformation. This approach enhances the flexibility and reduces the constraints of designing a DETIO for CPSs.

Theorem 2.

Given a non-negative matrix $\overline{A}-L\overline{C}$, under the cases where the initial condition after the coordinate transformation holds, we have

$$w^{-}\left(k\right)\le w\left(k\right)\le w^{+}\left(k\right).$$

(27)

Proof. 

If $\overline{A}-L\overline{C}$ is a non-negative matrix, by Lemma 5, the dynamic error system (26) can be deduced to be positive. From Lemma 2 and (24), since the matrix H is nonsingular, we can obtain the following inequalities:

$$w^{-}\left(k\right)\le w\left(k\right)\le w^{+}\left(k\right),k\ge 0.$$

(28)

Thus, the proof of Theorem 2 is finished.    □

Subsequently, by denoting ${\xi }_k={\left[{{ϵ}^{+}\left(k\right)}^T{{ϵ}^{-}\left(k\right)}^T\right]}^T$, and according to (18) and (26), we have

$$\begin{array}{cc}\hfill {\xi }_{k+1}=& M{\xi }_k+\check{F}+\check{\omega }+\check{\epsilon }+\check{E}\hfill \end{array}$$

(29)

where

$$M=\left[\begin{array}{cc}\overline{A}-L\overline{C}& 0\\ 0& \overline{A}-L\overline{C}\end{array}\right],$$

$$\check{F}=\left[\begin{array}{c}{\overline{F}}_w(w^{+}\left(k\right),w^{-}\left(k\right))-H\overline{F}\left(H^{-1}w\left(k\right)\right)\\ H\overline{F}\left(H^{-1}w\left(k\right)\right)-{\overline{F}}_w(w^{-}\left(k\right),w^{+}\left(k\right))\end{array}\right],\check{\omega }=\left[\begin{array}{c}{\overline{D}}^{+}{d}^{+}-{\overline{D}}^{-}{d}^{-}-\overline{D}d\\ \overline{D}d-{\overline{D}}^{+}{d}^{-}+{\overline{D}}^{-}{d}^{+}\end{array}\right],$$

$$\check{\epsilon }=\left[\begin{array}{c}L{e}_y+L^{-}{e}_y^{+}-L^{+}{e}_y^{-}\\ -L{e}_y+L^{+}{e}_y^{+}-L^{-}{e}_y^{-}\end{array}\right],\check{E}=\left[\begin{array}{c}-\overline{E}f\\ \overline{E}f\end{array}\right].$$

Theorem 3.

Given positive constants λ and ${\gamma }_i(i=1,2,\dots ,10)$, and under Assumptions 1 and 2, if there exists a positive-definite and symmetric matrix P that satisfies the following inequalities:

$$\begin{array}{c}\hfill \Pi =\left[\begin{array}{ccc}{\Pi }_1& 0& 0\\ *& {\Pi }_2& 0\\ *& *& {\Pi }_3\end{array}\right]\prec 0,\end{array}$$

(30)

where

$$\begin{array}{cc}\hfill & {\Pi }_1=(1+{\gamma }_1+{\gamma }_2+{\gamma }_3)M^{T}PM+(1+{\displaystyle \frac{1}{{\gamma }_1}}+{\gamma }_4+{\gamma }_5){\widehat{F}}^{T}P\widehat{F}-(1-\lambda )P,\hfill \\ \hfill & {\Pi }_2=-I,\hfill \\ \hfill & {\Pi }_3=\eta {\overline{C}}^T\overline{C}-\rho I,\hfill \end{array}$$

$$\widehat{F}=\left[\begin{array}{cc}{F}_a& F_b\\ F_c& F_d\end{array}\right],$$

then the system (26) is uniformly ultimately bounded (UUB).

Proof. 

Choose the candidate Lyapunov function for the systems given by (3) and (18) as follows:

$$W\left(k\right)=V\left(k\right)+\Gamma \left(k\right),$$

(31)

where $V\left(k\right)={\xi }_k^{T}P{\xi }_k$, and then it can be obtained that

$$\begin{array}{cc}\hfill W(k+1)=& {[M{\xi }_k+\check{F}+\check{\omega }+\check{\epsilon }+\check{E}]}^{T}P[M{\xi }_k+\check{F}+\check{\omega }+\check{\epsilon }+\check{E}]+{\Gamma }_{k+1}\hfill \\ \hfill =& {\left(M{\xi }_k\right)}^{T}P\left(M{\xi }_k\right)+{\left(M{\xi }_k\right)}^{T}P\check{F}+{\left(M{\xi }_k\right)}^{T}P\check{\omega }+{\left(M{\xi }_k\right)}^{T}P\check{\epsilon }+{\left(M{\xi }_k\right)}^{T}P\check{E}\hfill \\ \hfill & +{\left(\check{F}\right)}^{T}PM{\xi }_k+{\left(\check{\omega }\right)}^{T}PM{\xi }_k+{\left(\check{\epsilon }\right)}^{T}PM{\xi }_k+{\left(\check{E}\right)}^{T}PM\hfill \\ \hfill & +{\left(\check{F}\right)}^{T}P\check{\omega }+{\left(\check{\omega }\right)}^{T}P\check{F}+{\left(\check{F}\right)}^{T}P\check{\epsilon }+{\left(\check{\epsilon }\right)}^{T}P\check{F}+{\left(\check{F}\right)}^{T}P\check{E}+{\left(\check{E}\right)}^{T}P\check{F}\hfill \\ \hfill & +{\left(\check{\omega }\right)}^{T}P\check{\epsilon }+{\left(\check{\epsilon }\right)}^{T}P\check{\omega }+{\left(\check{\omega }\right)}^{T}P\check{E}+{\left(\check{E}\right)}^{T}P\check{\stackrel{ˇ}{\omega }}+{\left(\check{\epsilon }\right)}^{T}P\check{E}+{\left(\check{E}\right)}^{T}P\check{\epsilon }\hfill \\ \hfill & +{\left(\check{F}\right)}^{T}P\check{F}+{\left(\check{\omega }\right)}^{T}P\check{\omega }+{\left(\check{\epsilon }\right)}^{T}P\check{\epsilon }+{\left(\check{E}\right)}^{T}P\check{E}\hfill \\ \hfill & -\lambda \Gamma \left(k\right)+\eta y^T\left(k\right)y\left(k\right)-e_y^T\left(k\right)e_y\left(k\right).\hfill \end{array}$$

Then, the following are denoted:

$$\begin{array}{cccc}\hfill M_1\left(k\right)& ={\left(M{\xi }_k\right)}^{T}P\check{F},\hfill & \hfill & M_2\left(k\right)={\left(M{\xi }_k\right)}^{T}P\check{\omega },\hfill \\ \hfill M_3\left(k\right)& ={\left(M{\xi }_k\right)}^{T}P\check{\epsilon },\hfill & \hfill & M_4\left(k\right)={\left(M{\xi }_k\right)}^{T}P\check{E},\hfill \\ \hfill M_5\left(k\right)& ={\check{F}}^{T}P\check{\omega },\hfill & \hfill & M_6\left(k\right)={\check{F}}^{T}P\check{\epsilon },\hfill \\ \hfill M_7\left(k\right)& ={\check{F}}^{T}P\check{E},\hfill & \hfill & M_8\left(k\right)={\check{\omega }}^{T}P\check{\epsilon },\hfill \\ \hfill M_9\left(k\right)& ={\check{\omega }}^{T}P\check{\epsilon },\hfill & \hfill & M_{10}\left(k\right)={\check{\epsilon }}^{T}P\check{E}.\hfill \end{array}$$

(32)

From Lemma 6, we can deduce that

$$\begin{array}{cc}\hfill & M_1\left(k\right)+M_1^T\left(k\right)\le {\gamma }_1{\left(M{\xi }_k\right)}^{T}PM{\xi }_k+{\displaystyle \frac{1}{{\gamma }_1}}{\left(\check{F}\right)}^{T}P\check{F},\hfill \\ \hfill & M_2\left(k\right)+M_2^T\left(k\right)\le {\gamma }_2{\left(M{\xi }_k\right)}^{T}PM{\xi }_k+{\displaystyle \frac{1}{{\gamma }_2}}{\left(\check{\omega }\right)}^{T}P\check{\omega },\hfill \\ \hfill & M_3\left(k\right)+M_3^T\left(k\right)\le {\gamma }_3{\left(M{\xi }_k\right)}^{T}PM{\xi }_k+{\displaystyle \frac{1}{{\gamma }_3}}{\left(\check{\epsilon }\right)}^{T}P\check{\epsilon },\hfill \\ \hfill & M_4\left(k\right)+M_4^T\left(k\right)\le {\gamma }_4{\left(M{\xi }_k\right)}^{T}PM{\xi }_k+{\displaystyle \frac{1}{{\gamma }_4}}{\left(\check{E}\right)}^{T}P\check{E},\hfill \\ \hfill & M_5\left(k\right)+M_5^T\left(k\right)\le {\gamma }_5{\left(\check{F}\right)}^{T}P\check{F}+{\displaystyle \frac{1}{{\gamma }_5}}{\left(\check{\omega }\right)}^{T}P\check{\omega },\hfill \\ \hfill & M_6\left(k\right)+M_6^T\left(k\right)\le {\gamma }_6{\left(\check{F}\right)}^{T}P\check{F}+{\displaystyle \frac{1}{{\gamma }_6}}{\left(\check{\epsilon }\right)}^{T}P\check{\epsilon },\hfill \\ \hfill & M_7\left(k\right)+M_7^T\left(k\right)\le {\gamma }_7{\left(\check{F}\right)}^{T}P\check{F}+{\displaystyle \frac{1}{{\gamma }_7}}{\left(\check{E}\right)}^{T}P\check{E},\hfill \\ \hfill & M_8\left(k\right)+M_8^T\left(k\right)\le {\gamma }_8{\left(\check{\omega }\right)}^{T}P\check{\omega }+{\displaystyle \frac{1}{{\gamma }_8}}{\left(\check{\epsilon }\right)}^{T}P\check{\epsilon },\hfill \\ \hfill & M_9\left(k\right)+M_9^T\left(k\right)\le {\gamma }_9{\left(\check{\omega }\right)}^{T}P\check{\omega }+{\displaystyle \frac{1}{{\gamma }_9}}{\left(\check{E}\right)}^{T}P\check{E},\hfill \\ \hfill & M_{10}\left(k\right)+M_{10}^T\left(k\right)\le {\gamma }_{10}{\left(\check{\epsilon }\right)}^{T}P\check{\epsilon }+{\displaystyle \frac{1}{{\gamma }_{10}}}{\left(\check{E}\right)}^{T}P\check{E}.\hfill \end{array}$$

(33)

Thus, we can derive that

$$\begin{array}{cc}\hfill \Delta W_k& =W(k+1)-W\left(k\right)\hfill \\ \hfill & \le (1+{\gamma }_1+{\gamma }_2+{\gamma }_3+{\gamma }_4){\left(M{\xi }_k\right)}^{T}PM{\xi }_k+(1+{\displaystyle \frac{1}{{\gamma }_1}}+{\gamma }_5+{\gamma }_6+{\gamma }_7){\left(\check{F}\right)}^{T}P\check{F}\hfill \\ \hfill & +(1+{\displaystyle \frac{1}{{\gamma }_2}}+{\displaystyle \frac{1}{{\gamma }_5}}+{\gamma }_8+{\gamma }_9){\left(\check{\omega }\right)}^{T}P\check{\omega }+(1+{\displaystyle \frac{1}{{\gamma }_3}}+{\displaystyle \frac{1}{{\gamma }_6}}+{\displaystyle \frac{1}{{\gamma }_8}}+{\gamma }_{10}){\left(\check{\epsilon }\right)}^{T}P\check{\epsilon }\hfill \\ \hfill & +(1+{\displaystyle \frac{1}{{\gamma }_4}}+{\displaystyle \frac{1}{{\gamma }_7}}+{\displaystyle \frac{1}{{\gamma }_9}}+{\displaystyle \frac{1}{{\gamma }_{10}}}){(\check{E})}^{T}P\check{E}-{\xi }_k^{T}P{\xi }_k-(\lambda +1)\Gamma \left(k\right)\hfill \\ \hfill & +\eta y^T\left(k\right)y\left(k\right)-e_y^T\left(k\right)e_y\left(k\right).\hfill \end{array}$$

(34)

According to Lemma 4, we obtain the following inequalities:

$${\check{F}}^{T}P\check{F}\le {\xi }_k^T{\widehat{F}}^{T}P\widehat{F}{\xi }_k.$$

(35)

Substituting (35) into (34), we can derive that

$$\begin{array}{cc}\hfill \Delta W_k& \le {\xi }_k^T[(1+{\gamma }_1+{\gamma }_2+{\gamma }_3+{\gamma }_4)M^{T}PM+(1+{\displaystyle \frac{1}{{\gamma }_1}}+{\gamma }_5+{\gamma }_6+{\gamma }_7){\widehat{F}}^{T}P\widehat{F}-P]{\xi }_k\hfill \\ \hfill & +(1+{\displaystyle \frac{1}{{\gamma }_2}}+{\displaystyle \frac{1}{{\gamma }_5}}+{\gamma }_8+{\gamma }_9){\left(\check{\omega }\right)}^{T}P\check{\omega }+(1+{\displaystyle \frac{1}{{\gamma }_3}}+{\displaystyle \frac{1}{{\gamma }_6}}+{\displaystyle \frac{1}{{\gamma }_8}}+{\gamma }_{10}){\left(\check{\epsilon }\right)}^{T}P\check{\epsilon }\hfill \\ \hfill & +(1+{\displaystyle \frac{1}{{\gamma }_4}}+{\displaystyle \frac{1}{{\gamma }_7}}+{\displaystyle \frac{1}{{\gamma }_9}}+{\displaystyle \frac{1}{{\gamma }_{10}}}){\left(\check{E}\right)}^{T}P\check{E}-(\lambda +1)\Gamma \left(k\right)\hfill \\ \hfill & +\eta w^T\left(k\right){\overline{C}}^T\overline{C}w\left(k\right)-e_y^T\left(k\right)e_y\left(k\right).\hfill \end{array}$$

(36)

Let $z\left(k\right)={\left[{\xi }^T\left(k\right)e_y^T\left(k\right)w^T\left(k\right)\right]}^T$, and define

$$\begin{array}{cc}\hfill {\Delta }_k=& +(1+{\displaystyle \frac{1}{{\gamma }_2}}+{\displaystyle \frac{1}{{\gamma }_5}}+{\gamma }_8+{\gamma }_9){\left(\check{\omega }\right)}^{T}P\check{\omega }+(1+{\displaystyle \frac{1}{{\gamma }_3}}+{\displaystyle \frac{1}{{\gamma }_6}}+{\displaystyle \frac{1}{{\gamma }_8}}+{\gamma }_{10}){\left(\check{\epsilon }\right)}^{T}P\check{\epsilon }\hfill \\ \hfill & +(1+{\displaystyle \frac{1}{{\gamma }_4}}+{\displaystyle \frac{1}{{\gamma }_7}}+{\displaystyle \frac{1}{{\gamma }_9}}+{\displaystyle \frac{1}{{\gamma }_{10}}}){\left(\check{E}\right)}^{T}P\check{E}.\hfill \end{array}$$

(37)

Then, we can obtain the inequalities as follows:

$$\begin{array}{cc}\hfill \Delta W\left(k\right)+\lambda W\left(k\right)-\rho w^T\left(k\right)w\left(k\right)\le & {\xi }_k^T[(1+{\gamma }_1+{\gamma }_2+{\gamma }_3+{\gamma }_4)M^{T}PM+(1+{\displaystyle \frac{1}{{\gamma }_1}}+{\gamma }_5\hfill \\ \hfill & +{\gamma }_6+{\gamma }_7){\widehat{F}}^{T}P\widehat{F}-(1-\lambda )P]{\xi }_k-e_y^T\left(k\right)e_y\left(k\right)\hfill \\ \hfill & +w^T\left(k\right)(\eta {\overline{C}}^T\overline{C}-\rho I)w\left(k\right)+{\Delta }_k\hfill \\ \hfill & =z^T\left(k\right)\Pi z\left(k\right)+{\Delta }_k.\hfill \end{array}$$

(38)

where

$$\begin{array}{c}\hfill \Pi =\left[\begin{array}{ccc}{\Pi }_1& 0& 0\\ *& {\Pi }_2& 0\\ *& *& {\Pi }_3\end{array}\right],\end{array}$$

$$\begin{array}{c}{\Pi }_1=(1+{\gamma }_1+{\gamma }_2+{\gamma }_3+{\gamma }_4)M^{T}PM+(1+{\displaystyle \frac{1}{{\gamma }_1}}+{\gamma }_5+{\gamma }_6+{\gamma }_7){\widehat{F}}^{T}P\widehat{F}-(1-\lambda )P,\hfill \\ {\Pi }_2=-I,\hfill \\ {\Pi }_3=\eta {\overline{C}}^T\overline{C}-\rho I.\hfill \end{array}$$

   □

According to Assumption 1, we can derive that $\check{\omega }$ and $\check{\epsilon }$ are actually bounded, and then the error system (26) is UUB.

Based on Theorems 1 and 3, the design of a DETIO for fault detection can be implemented by Algorithm 1.

Algorithm 1 Algorithm for Fault Detection DETIO

1: Model CPSs with given disturbances and random faults. 2: Initialize DETM parameters in (3). 3: Design the fault detection DETIO framework for above CPSs. 4: Apply coordinate transformation if systems do not satisfy non-negativity condition. 5: Solve LMI problem from Theorem 3 to obtain the observer gain L. 6: Obtain the interval residual signals through (22) to detect faults.

4. Numerical Example

4.1. Example of an Unmanned Ground Vehicle

4.1.1. Simulation of Fault-Free Case

To verify the DETIO, a unique form of nonlinear CPS without faults is first considered. Given an unmanned ground vehicle (UGV) model shown in Figure 1, it can be simplified and described as the following equation:

$$\left\{\begin{array}{c}\dot{z}\left(t\right)=\left[\begin{array}{cc}0& 1\\ 0& -{\displaystyle \frac{U}{M}}\end{array}\right]z\left(t\right)+\left[\begin{array}{c}0\\ {\displaystyle \frac{1}{M}}\end{array}\right]\mu \left(t\right),\hfill \\ y\left(t\right)=\left[\begin{array}{cc}1& 0\\ 0& 0\end{array}\right]z\left(t\right).\hfill \end{array}\right.$$

(39)

where the vehicle state $z\left(t\right)=\left[\begin{array}{c}x\left(t\right)\\ v\left(t\right)\end{array}\right]$; x and v represent the current position and velocity; and U and M denote the translational friction coefficient and mechanical mass of the UGV. The input of the system is represented by $\mu \left(t\right)$, and $y\left(t\right)$ denotes the output signal. It is assumed that $U=0.8$ and $M=1$, and we consider the nonlinear terms of the system; then, through discretization, we can obtain the parametric matrices as follows:

$$A=\left[\begin{array}{c}10.096\\ 00.923\end{array}\right],B=\left[\begin{array}{c}0.005\\ 0.096\end{array}\right],$$

$$C=\left[\begin{array}{c}10\end{array}\right],D=\left[\begin{array}{c}10\\ 01\end{array}\right].$$

Let the disturbance ${\delta }_k=\left[\begin{array}{c}0.05sin\left(k\right)+0.05\\ -0.05cos\left(k\right)+0.05\end{array}\right]$ and choose the nonlinear function $F(x_1,x_2)=\left[\begin{array}{c}0.05sin\left(x_1\right)\\ 0.05cos\left(x_2\right)\end{array}\right]$. Moreover, let $E=\left[\begin{array}{c}1\\ 0\end{array}\right]$ and for $\forall k\ge 0$, $f=0$, which in this case is fault-free. Then, select the coordinate transformation matrix H as

$$H=\left[\begin{array}{cc}1& -1\\ 1& -2\end{array}\right].$$

The remaining parameters are given below:

$$\lambda =0.01,\eta =0.01,\rho =3.$$

(40)

Then, the matrix $\widehat{F}$ and weighting matrix P are obtained as

$$\widehat{F}=\left[\begin{array}{cccc}0.1& 0& 0.05& 0\\ 0& 0.1& 0& 0.05\\ 0.05& 0& 0.1& 0\\ 0& 0.05& 0& 0.1\end{array}\right],P=\left[\begin{array}{cccc}8.6103& -4.0690& 0.0901& -0.0426\\ -4.0690& 1.9229& -0.0426& 0.0201\\ 0.0901& -0.0426& 8.6103& -4.0690\\ -0.0426& 0.0201& -4.0690& 1.9229\end{array}\right].$$

Therefore, according to Theorem 3, we can obtain the gain matrix L as follows:

$$L=\left[\begin{array}{c}0.5038\\ -0.05\end{array}\right].$$

Through simulation, we can obtain the results as follows. Figure 2 and Figure 3 separately depict the state trajectories and estimation of $x_1$ and $x_2$. Figure 4 and Figure 5 verify that the error system gradually stabilizes to a positive lower bound, which proves the effectiveness of this method. Figure 6 shows the situation without faults. For the area where $0\in [r^{-},r^{+}]$, this means that the estimated values are still within the upper and lower boundaries, while for the area where $0\notin [r^{-},r^{+}]$, this indicates that the actuator is faulty. Moreover, Figure 7 manifests the intervals and triggering instants of the event, which also illustrates that the Zeno behavior does not happen. In the figures, ‘u’ denotes the upper bound of the estimation and ‘l’ represents the lower bound of the estimation.

4.1.2. Simulation with Random Faults

To validate the effectiveness of the developed results, we tested the situation where random faults exist. We used the same UGV model as above, with the actuator fault algorithm previously set as

$$f\left(k\right)=\left\{\begin{array}{ccc}{\left[\begin{array}{c}00\end{array}\right]}^T,\hfill & \hfill & 0\mathrm{s}<k\le 8\mathrm{s},\hfill \\ {\left[\begin{array}{c}2.51.2\end{array}\right]}^T,\hfill & \hfill & 8\mathrm{s}<k\le 13\mathrm{s},\hfill \\ {\left[\begin{array}{c}00\end{array}\right]}^T,\hfill & \hfill & 13\mathrm{s}<k\le 15\mathrm{s},\hfill \\ {\left[\begin{array}{c}2.01.5\end{array}\right]}^T,\hfill & \hfill & 15\mathrm{s}<k\le 20\mathrm{s}.\hfill \end{array}\right.$$

(41)

The residual results can be obtained in Figure 8 by simulation, and the following can be found:

$$\left\{\begin{array}{ccc}0\in [r^{-},r^{+}],\hfill & \hfill & 0\mathrm{s}<k<12.1\mathrm{s},\hfill \\ 0\notin [r^{-},r^{+}],\hfill & \hfill & 12.1\mathrm{s}\le k\le 13.5\mathrm{s},\hfill \\ 0\in [r^{-},r^{+}],\hfill & \hfill & 13.5\mathrm{s}<k<15.1\mathrm{s},\hfill \\ 0\notin [r^{-},r^{+}],\hfill & \hfill & 15.1\mathrm{s}\le k\le 20\mathrm{s}.\hfill \end{array}\right.$$

(42)

It is easy to see that the fault is detected in $0.1$ s, which proves the sensitivity and precision of the proposed method. Figure 9 shows the triggering intervals of the faulty cases, which also illustrates the characteristics of the proposed design for the fault detection DETIO in saving resources.

4.2. Example of an Unmanned Aerial Vehicle

4.2.1. Simulation of a Fault-Free Case

To further verify the applicability of the fault detection DETIO, we consider an unmanned aerial vehicle (UAV) model as shown in Figure 10. Referring to [29], the UAV system can be described as follows:

$$\left\{\begin{array}{c}\left[\begin{array}{c}\dot{\alpha }\left(t\right)\\ \dot{\beta }\left(t\right)\end{array}\right]=A\left[\begin{array}{c}\alpha \left(t\right)\\ \beta \left(t\right)\end{array}\right]+Bu\left(k\right)+p\left(k\right),\hfill \\ y\left(k\right)=C\left[\begin{array}{c}\alpha \left(t\right)\\ \beta \left(t\right)\end{array}\right].\hfill \end{array}\right.$$

(43)

where $\alpha \left(t\right)$ and $\beta \left(t\right)$ represent the angle of attack and the pitch rate of the UAV. $u\left(k\right)$ is the system input and $p\left(k\right)$ is the disturbance. $y\left(k\right)$ is the output of the UAV system. The partial parametric matrices are as follows:

$$A=\left[\begin{array}{cc}0.8825& 0.0987\\ -0.8458& 0.9122\end{array}\right],B=\left[\begin{array}{c}-0.0194\\ -1.9290\end{array}\right],$$

$$C=\left[\begin{array}{c}10.2\end{array}\right],D=\left[\begin{array}{c}10\\ 01\end{array}\right],E=\left[\begin{array}{c}2\\ 0\end{array}\right].$$

The external disturbance ${\delta }_k=\left[\begin{array}{c}0.1+0.1sin\left(k\right)\\ 0.1-0.1cos\left(k\right)\end{array}\right]$ and the nonlinear function $F(x_1,x_2)=\left[\begin{array}{c}0.1sin\left(x_1\right)\\ 0.1cos\left(x_2\right)\end{array}\right]$. Moreover, the transformation matrix H is selected as

$$H=\left[\begin{array}{cc}1& 0\\ -1& -2\end{array}\right].$$

The remaining parameters remain consistent with the parameters in (40), and for $\forall k\ge 0$, $f=0$. Then, the matrix $\widehat{F}$ and the weighting matrix P are obtained as

$$\widehat{F}=\left[\begin{array}{cccc}0.1& 0& 0.05& 0\\ 0& 0.1& 0& 0.05\\ 0.05& 0& 0.1& 0\\ 0& 0.05& 0& 0.1\end{array}\right],P=\left[\begin{array}{cccc}23.3435& -0.9440& -0.1006& 0.0041\\ -0.9440& 0.0382& 0.0041& -0.0002\\ -0.1006& 0.0041& 23.3435& -0.9440\\ 0.0041& -0.0002& -0.9440& 0.0382\end{array}\right].$$

Through Theorem 3, we can obtain the gain matrix of the UAV system as follows:

$$L=\left[\begin{array}{c}0.8687\\ -0.85\end{array}\right].$$

The following are the results of the simulation. Figure 11 and Figure 12 manifest the original states and its interval estimations. Figure 13 and Figure 14 illustrate the effectiveness of this approach in the UAV model. Figure 15 shows the residual which proves that no faults are detected in this fault-free situation. And Figure 16 displays the intervals and triggering instants of the event with no occurrence of Zeno behavior.

4.2.2. Simulation with Random Faults

To verify the effectiveness and applicability of this approach, random faults are introduced into the above UAV model, and the fault algorithm is preset as follows:

$$f\left(k\right)=\left\{\begin{array}{ccc}{\left[\begin{array}{c}00\end{array}\right]}^T,\hfill & \hfill & 0\mathrm{s}<k\le 6\mathrm{s},\hfill \\ {\left[\begin{array}{c}-1.0-0.7\end{array}\right]}^T,\hfill & \hfill & 6\mathrm{s}<k\le 15\mathrm{s},\hfill \\ {\left[\begin{array}{c}00\end{array}\right]}^T,\hfill & \hfill & 15\mathrm{s}<k\le 20\mathrm{s}.\hfill \end{array}\right.$$

(44)

Through simulation, we can obtain the results shown in Figure 17, where we can find that

$$\left\{\begin{array}{ccc}0\in [r^{-},r^{+}],\hfill & \hfill & 0\mathrm{s}<k<6.6\mathrm{s},\hfill \\ 0\notin [r^{-},r^{+}],\hfill & \hfill & 6.6\mathrm{s}\le k\le 16.5\mathrm{s},\hfill \\ 0\in [r^{-},r^{+}],\hfill & \hfill & 16.5\mathrm{s}<k<20\mathrm{s}.\hfill \end{array}\right.$$

(45)

This indicates the occurrence of the faults in the system. Figure 18 exhibits the triggering intervals of the UAV example under faults, demonstrating the economical feature of saving system resources using this approach.

4.3. Quantitative Comparison with UGV Model

Consider the UGV model mentioned in Section 4.1, to further demonstrate the proposed method of this article, a comparison is conducted between our approach and the fault detection with ETIO using static ETM. Figure 19 shows the triggering instants and intervals of static ETIO fault detection under random faults in (41).

Table 1. The number of event-triggered instants of different fault detection methods.

Methods	Number of Event-Triggered Instants
DETIO Fault Detection	44 Times
Static ETIO Fault Detection	58 Times
Traditional IO Fault Detection 1	200 Times

¹ Fundamental sample time is set to 0.1 s.

displays the event-triggered counts of the proposed method, the static ETIO approach, and the traditional IO technique, respectively.

From Table 1, we can conclude that the proposed method of this paper has a better performance in resource saving and data transmission, compared to other methods without DETM.

5. Conclusions

This paper studies a DETIO-based fault detection approach that is applied to nonlinear CPSs. A DETIO framework is designed through the positive system theory and integrated DETM to minimize data transmission and conserve network resources. For systems which violate the non-negative condition, the coordinate transformation method is introduced to enhance the flexibility of designing the observer. Finally, numerical simulations of two situations are manifested to demonstrate the viability of the developed approach. Based on both a simplified UGV model and a UAV model, the interval estimation of states is obtained by fault-free cases. Then, through simulation with random faults, we prove the effectiveness and rapidity of the presented method. Furthermore, the avoidance of Zeno behavior is also illustrated by the simulation, which proves the effectiveness in conserving resources. Moreover, three different fault detection approaches based on the UGV model are compared to verify the superiority of the proposed method. In future work, we will investigate the deployment of DETM in interval observer-based fault detection of distributed CPSs.