Method | τ2 |
[19] | 0.60 |
[7] | 1.40 |
Theorem 3.1 | 2.38 |
In general, as compared to conventional combustion engines, the homogeneous charge compression ignition (HCCI) engine offers better fuel efficiency, NOx, and particulate matter emissions. The HCCI engine, on the other hand, is not connected to the spark plugs or the fuel injection system. This implies that the auto-ignition time and following combustion phase of the HCCI engine are not controlled directly. The HCCI engine will be confined to a short working range due to the cold start, high-pressure rate, combustion noise, and even knocking combustion. Biofuel innovation, such as ethanol-powered HCCI engines, has a lot of promise in today's car industry. As a result, efforts must be made to improve the distinctive characteristics of the engine by turning the engine settings to different ethanol mixtures. This study examines the aspects of ethanol-fueled HCCI engines utilizing homogenous charge preparation procedures. In addition, comparing HCCI engines to other advanced combustion engines revealed their increased importance and prospective consequences. Furthermore, the challenges of transitioning from conventional to HCCI engines are examined, along with potential answers for future upgrade approaches and control tactics.
Citation: Thang Nguyen Minh, Hieu Pham Minh, Vinh Nguyen Duy. A review of internal combustion engines powered by renewable energy based on ethanol fuel and HCCI technology[J]. AIMS Energy, 2022, 10(5): 1005-1025. doi: 10.3934/energy.2022046
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In general, as compared to conventional combustion engines, the homogeneous charge compression ignition (HCCI) engine offers better fuel efficiency, NOx, and particulate matter emissions. The HCCI engine, on the other hand, is not connected to the spark plugs or the fuel injection system. This implies that the auto-ignition time and following combustion phase of the HCCI engine are not controlled directly. The HCCI engine will be confined to a short working range due to the cold start, high-pressure rate, combustion noise, and even knocking combustion. Biofuel innovation, such as ethanol-powered HCCI engines, has a lot of promise in today's car industry. As a result, efforts must be made to improve the distinctive characteristics of the engine by turning the engine settings to different ethanol mixtures. This study examines the aspects of ethanol-fueled HCCI engines utilizing homogenous charge preparation procedures. In addition, comparing HCCI engines to other advanced combustion engines revealed their increased importance and prospective consequences. Furthermore, the challenges of transitioning from conventional to HCCI engines are examined, along with potential answers for future upgrade approaches and control tactics.
Networked control systems(NCSs) are a class of systems where the signals of feedback loops are closed via communication network. These systems are found in many applications such as automobiles and airplanes, large scale disributed industrial systems and telecommunication systems due to easier installation and maintenance, simpler upgrading and more reliability over the point-to-point connected systems [3]. Therefore, much attention has been paid to NCSs in the last decades [5,21]. In the networked control system, the information is exchanged with packets through a network where the data packets encounter delays. Considering the effects of network-induced delays in nonlinear NCS, we model its closed-loop system as a fuzzy system with bounded delays.
For a nonlinear control system, Takagi-Sugeno fuzzy model has been playing an important role. It can represent a nonlinear system effectively and is known to be a great tool to analyze and synthesize nonlinear control systems [11,12,13]. The papers [4,6,7,9,10,16,19,20] and [22] considered control design problems for nonlinear networked control systems. The paper [6] partially introduced a multiple Lyapunov-Krasovskii matrix method for fuzzy systems with time-delay but it is not a general multiple Lyapunov matrix method. The papers [4,9,20] and [22] discussed various fuzzy networked control systems but all employed a common Lyapunov-Krasovskii function method. The papers [7,10] and [19] employed a common Lyapunov-Krasovskii function method with descriptor system approach, which is still more conservative than a multiple Lyapunov-Krasovskii matrix method. The papers [6,16] and [19] used a free matrix method to reduce the conservatism but increase computational load by introducing a number of free matrices. Furthermore, the paper [17] introduced a new multiple Lyapunov matrix method but only considered the stability of a networked control system. The papers [17] and [18] considered the stability and stabilization problems based on multiple Lyapunov-Krasovskii matrix method.
In this paper, we consider the H∞ disturbance attenuation of nonlinear networked control systems based on Takagi-Sugeno fuzzy models. First, we assume a new class of fuzzy feedback controller and consider the H∞ disturbance attenuation of the closed-loop system with such a feedback controller. In order to obtain less conservative H∞ disturbance attenuation conditions, we introduce a new type of multiple Lyapunov-Krasovskii function, which reduces the conservatism in stability conditions. A multiple Lyapunov-Krasovskii function is a natural extension of a common Lyapunov-Krasovskii function. However, a conventional multiple Lyapunov function contains the membership function and hence a resulting condition depends on the derivatives of the membership function. However, the derivative of the membership function may not always be known a priori nor differentiable. The paper [8] introduced a new class of multiple Lyapunov function, which contains an integral of the membership function of fuzzy systems. This approach requires no information on the derivatives of the membership function and is shown to reduce the conservatism in H∞ disturbance attenuation conditions. In addition, triple and quadruple integrals of Lyapunov-Krasovskii functions are employed, which enormously reduce the conservatism. Based on such a multiple Lyapunov-Krasovskii function, a control design method of nonlinear networked control systems are proposed. Finally, a numerical example is shown to illustrative our control design method and to show the effectiveness of our approach.
Consider the Takagi-Sugeno fuzzy model, described by the following IF-THEN rules:
IFξ1isMi1and⋯andξpisMip,THEN˙x(t)=Aix(t)+Biu(t)+Diw(t),z(t)=Cix(t) |
where x(t)∈ℜn is the state, u(t)∈ℜm is the control input. and z(t)∈ℜq is the controlled output. The matrices Ai, Bi,Ci and Di are constant matrices of appropriate dimensions. r is the number of IF-THEN rules. Mij are fuzzy sets and ξ1,⋯,ξp are premise variables. We set ξ=[ξ1⋯ξp]T. The premise variable ξ(t) is assumed to be measurable.
Then, the state equation and the controlled output equation are described by
˙x(t)=r∑i=1λi(ξ){Aix(t)+Biu(t)+Diw(t)}Δ=Aλx(t)+Bλu(t)+Dλw(t) | (2.1) |
z(t)=r∑i=1λi(ξ)Cix(t)Δ=Cλx(t) | (2.2) |
where
λi(ξ)=βi(ξ)r∑i=1βi(ξ),βi(ξ)=p∏j=1Mij(ξj) |
and Mij(⋅) is the grade of the membership function of Mij. We assme
λi(ξ(t))≥0,i=1,⋯,r,r∑i=1λi(ξ(t))=1 | (2.3) |
for any ξ(t).
In the considered networked control system, the controller and the actuator are event-driven and sampler is clock-driven. The actual input of the system (2.1) is realized via a zero-order hold device. The sampling period is assumed to be a positive constant T and the information of the zero-order hold may be updated between sampling instants. The updating instants of the zero-order hold are denoted by tk, and τa and τb are the time-delays from the sampler to the controller and from the controller to the zero-order hold at the updating instant tk, respectively. So, the successfully transmitted data in the networked control system at the instant tk experience round trip delay τ=τa+τb which does not need to be restricted inside one sampling period. Regarding the role of the zero-order hold, for a state sample data tk−τ, the corresponding control signal would act on the plant from tk unto tk+1. Therefore, the rules of the fuzzy control input for tk≤t≤tk+1, is written as follows:
IFξ1isMi1and⋯andξpisMip,THENu(t)=Kix(t−τ(t)),i=1,⋯,r. |
where Ki,i=1,⋯,r are constant matrices, and τ(t) may be an unknown time varying delay but its lower bound τ1 and upper bound τ2 are assumed to be known. The upper bound η of the delay rate is also assumed to be known:
τ1≤τ(t)≤τ2, 0<˙τ(t)≤η. |
Then, an overall controller is given by
u(t)=r∑i=1μi(ξ(t−τ(t)))Kix(t−τ(t))Δ=Kτμx(t−τ(t)) | (2.4) |
where
μi(ξ(t))=1h∫tt−hλi(ξ(s))ds, |
and h>0 is some scalar. The closed-loop system (2.1) with (2.4) is given by
˙x(t)=r∑i=1r∑l=1λi(ξ(t))μl(ξ(t−τ(t))){Aix(t)+BiKlx(t−τ(t))+Diw(t)}=Aλx(t)+BλKτμx(t−τ(t)+Dλw(t). | (2.5) |
We note that μi(ξ(t))≥0, i=1,⋯,r and
r∑i=1μi(ξ(t))=1h∫tt−hr∑i=1λi(ξ(s))ds=1, |
which imply that μi(ξ(t)) and λi(ξ(t)) share the same properties as seen in (2.3).
We define the cost function
J=∫∞0(zT(t)z(t)−γ2wT(t)w(t))dt | (2.6) |
where γ is a prescribed scalar. Our problem is to find a condition such that the closed-loop system (2.2) and (2.5) is asymptotically stable with w(t)=0 and it satisfies J<0 in (2.6). In this case, the system is said to achieve the H∞ disturbance attenuation with γ.
Let us first assume that all the controller gain matrices Ki, i=1,⋯,r are given. Importance on the disturbance attenuation conditions lies on how to choose an appropriate Lyapunov-Krasovskii function. Here, we introduce a new Lyapunov-Krasovskii function. To begin with, let us consider a polytopic matrix:
Zμ=r∑i=1μi(ξ(t))Zi |
and similar notations will be used for other matrices. It is easy to see that the time-derivative of Zμ is calculated as
˙Zμ=r∑i=1˙μi(ξ(t))Zi=1hr∑i=1(λi(ξ(t))−λi(ξ(t−τ)))ZiΔ=1h(Zλ−Zτλ). | (3.1) |
For later use, we give some notation and lemmas:
ζ(t)=[xT(t)xT(t−τ(t))xT(t−τ1)xT(t−τ2)∫tt−τ1xT(s)ds∫t−τ1t−τ(t)xT(s)ds∫t−τ(t)t−τ2xT(s)ds∫0−τ1∫tt+βxT(s)dsdβ∫−τ1−τ(t)∫tt+βxT(s)ds∫−τ(t)−τ2∫tt+βxT(s)dsw(t)]TΔ=[ζT1(t)ζT2(t)⋯ζT11(t)]T. |
Lemma 3.1. (Jensen's Inequality) For τ∈ℜ, x(t)∈ℜn, and P>0∈ℜn×n, the following inequalities hold:
−τ∫tt−τxT(s)Px(s)ds≤∫tt−τxT(s)dsP∫tt−τx(s)ds,−τ22∫0−τ∫tt+βxT(s)Px(s)dsdβ≤∫0−τ∫tt+βxT(s)dsdβP∫0−τ∫tt+βx(s)dsdβ,−τ36∫0−τ∫0β∫tt+θxT(s)Px(s)dsdβdθ≤∫0−τ∫0β∫tt+θxT(s)dsdβdθP∫0−τ∫0β∫tt+θx(s)dsdβdθ. |
Lemma 3.2. [1] For τ1, τ2, α, ε∈ℜ, x(t)∈ℜn, and P>0∈ℜn×n, the following inequalities hold:
−(τ2−τ1)∫t−τ1t−τ2xT(s)Px(s)ds≤−ζT6(t)Pζ6(t)−ζT7(t)Pζ7(t)−(1−α)ζT6(t)Pζ6(t)−αζT7(t)Pζ7(t),−(τ22−τ21)2∫t−τ1t−τ2∫tt+βxT(s)Px(s)dsdβ≤−ζT9(t)Pζ9(t)−ζT10(t)Pζ10(t)−(1−ε)ζT9(t)Pζ9(t)−εζT10(t)Pζ10(t). |
Now, we are ready to give our first result.
Theorem 3.1. Given control gain matrices Kl, l=1,⋯,r and scalar h>0. The closed-loop system (2.5) achieves the H∞ disturbance attenuation with γ if there exist matrices Zj>0, P1>0, P2>0, P3>0, P4>0, Rj1>0, R2>0, R3j>0, R4>0, X1j>0, X2>0, X3j>0, X4>0, U1>0, U2>0, Wj, j=1,⋯,r, and scalars δi>0, i=1,2 such that
[12θijl+θ1j+δ1ICTi∗−I]<0, i,j,l=1,⋯,r, | (3.2) |
[12θijl+θ2j+δ1ICTi∗−I]<0, i,j,l=1,⋯,r, | (3.3) |
[12θijl+θ3j−δ2ICTi∗−I]<0, i,j,l=1,⋯,r, | (3.4) |
[12θijl+θ4j−δ2ICTi∗−I]<0, i,j,l=1,⋯,r, | (3.5) |
δ1−δ2>0 | (3.6) |
[1τ1Zi+X2−X2−X2Q1i+X2]≥0, i=1,⋯,r, | (3.7) |
[1τ2−τ1Zi+X4−X4−X4Q2i+X4]≥0, i=1,⋯,r | (3.8) |
where τ12=τ2−τ1, τ(2)12=τ22−τ21
θ1j=−eT7X3je7−(e2−e4)TX4(e2−e4),θ2j=−eT6X3je6−(e2−e3)TX4(e2−e3),θ3j=−eT10R3je10−(τ12e1−e7)TR4(τ12e1−e7),θ4j=−eT9R3je9−(τ12e1−e6)TR4(τ12e1−e6),θijl=πijl−eT5X1e5−(e1−e3)TX2(e1−e3)−eT6X3e6−eT7X3e7−(e2−e3)TX4(e2−e3)−(e2−e4)TX4(e2−e4)−eT8R1je8−(τ1e1−e5)TR2(τ1e1−e5)−eT9R3je9−eT10R3je10−(τ12e1−e6)TR4(τ12e1−e6)−(τ12e1−e7)TR4(τ12e1−e7)−(τ122e1−e8)TU1(τ122e1−e8)−(τ(2)122e1−e9−e10)TU2(τ(2)122e1−e9−e10) |
πijl=[Λ11ijΛ12ijl00P100τ1P3τ12P4τ12P4∗Λ22ijl00000000∗∗−Q1j+Q2j0−P1P2P2000∗∗∗−Q2j0−P2−P2000∗∗∗∗000−P300∗∗∗∗∗000−P4−P4∗∗∗∗∗∗00−P4−P4∗∗∗∗∗∗∗000∗∗∗∗∗∗∗∗00∗∗∗∗∗∗∗∗∗0∗∗∗∗∗∗∗∗∗∗ZjDi+ATiΩDiKTlBTiΩDi00000000DTiΩDi−γ2I], |
Λ11ij=ATiZj+ZjAi+Q1j+Wj+1h(Zi−Zl)+τ21X1j+τ212X3j+τ414R1j+(τ(2)12)24R3j+ATiΩAi,Λ12ijl=ZjBiKl+ATiΩBiKl,Λ22ijl=−(1−η)Wj+KTlBTiΩBiKl,Ω=τ21X2+τ212X4+τ414R2+(τ(2)12)24R4+τ6136U1+(τ32−τ31)236U2,Φil=[ATiKTlBTi00000000 DTi],ˉCi=[Ci000000000 0], |
and ei, i=1,⋯,11 denote an 11-dimensional fundamental vector whose i-th element is 1 and 0 elsewhere.
Proof: Consider the following Lyapunov-Krasovskii function:
V(xt)=V1(xt)+V2(xt)+V3(xt)+V4(xt)+V5(xt) | (3.9) |
where xt=x(t+θ), −τ2≤θ≤0,
V1(xt)=xT(t)Zμx(t)+∫tt−τ1xT(s)dsP1∫tt−τ1xT(s)ds+∫t−τ1t−τ2xT(s)dsP2∫t−τ1t−τ2x(s)ds+∫0−τ1∫tt+θxT(s)dsdθP3∫0−τ1∫tt+θx(s)dsdθ+∫−τ1−τ2∫tt+θxT(s)dsdθP4∫−τ1−τ2∫tt+θx(s)dsdθ,V2(xt)=∫tt−τ1xT(s)Q1μx(s)ds+∫t−τ1t−τ2xT(s)Q2μx(s)ds+∫tt−τ(t)xT(s)Wμx(s)ds,V3(xt)=τ1∫0−τ1∫tt+θxT(s)X1μx(s)dsdθ+τ1∫0−τ1∫tt+θ˙xT(s)X2˙x(s)dsdθ+(τ2−τ1)∫−τ1−τ2∫tt+θxT(s)X3μx(s)dsdθ+(τ2−τ1)∫−τ1−τ2∫tt+θ˙xT(s)X4˙x(s)dsdθ,V4(xt)=τ212∫0−τ1∫0β∫tt+θxT(s)R1μx(s)dsdθdβ+τ212∫0−τ1∫0β∫tt+θ˙xT(s)R2˙x(s)dsdθdβ+τ22−τ212∫−τ1−τ2∫0β∫tt+θxT(s)R3μx(s)dsdθdβ+τ22−τ212∫−τ1−τ2∫0β∫tt+θ˙xT(s)R4˙x(s)dsdθdβ,V5(xt)=τ316∫0−τ1∫0β∫0λ∫tt+θ˙xT(s)U1˙x(s)dsdλdβdθ+τ32−τ316∫−τ1−τ2∫0β∫0λ∫tt+θ˙xT(s)U2˙x(s)dsdλdβdθ |
where
Xjμ=r∑i=1μi(ξ)Xji>0, j=1,3 |
and similar notations are used. Now, we take the derivative of V(xt) with respect to t along the solution of the system (2.5).
First, using Lemma 3.1, we see that
∫tt+θ˙xT(s)X2˙x(s)ds≥−1θ∫tt+θ˙xT(s)dsX2∫tt+θ˙x(s)ds=−1θ[x(t)−x(t+θ)]TX2[x(t)−x(t+θ)] |
and
∫0−τ1∫tt+θ˙xT(s)X2˙x(s)dsdθ≥−∫0−τ11θ[x(t)−x(t+θ)]TX2[x(t)−x(t+θ)]dθ=∫τ101θ[x(t)−x(t−s)]TX2[x(t)−x(t−s)]ds≥1τ1∫τ10[x(t)−x(t−s)]TX2[x(t)−x(t−s)]ds=1τ1∫tt−τ1[x(t)−x(α)]TX2[x(t)−x(α)]dα |
Similarly, we have
∫−τ1−τ2∫tt+θ˙xT(s)X4˙x(s)dsdθ≥1τ2−τ1∫t−τ1t−τ2[x(t)−x(α)]TX4[x(t)−x(α)]dα |
Hence, we get
xT(t)Zμx(t)+∫tt−τ1xT(s)Q1μx(s)ds+∫t−τ1t−τ2xT(s)Q2μx(s)ds+τ1∫0−τ1∫tt+θ˙xT(s)X2˙x(s)dsdθ+(τ2−τ1)∫−τ1−τ2∫tt+θ˙xT(s)X4˙x(s)dsdθ≥∫tt−τ1[x(t)x(α)]T[1τ1Zμ+X2−X2−X2Q1μ+X2][x(t)x(α)]dα+∫t−τ1t−τ2[x(t)x(α)]T[1τ2−τ1Zμ+X4−X4−X4Q2μ+X4][x(t)x(α)]dα |
It follows from the above that for V1(xt)+V2(xt)+V3(xt) to be positive, the positive definiteness of Q1i and Q2i, i=1,⋯,r can be removed if the positive definiteness of Pi,Wj,X1j,X3j, i=1,⋯,4, j=1,⋯,r is guaranteed and (3.7)-(3.8) are satisfied.
The derivatives of V1(xt) and V2(xt) in (3.9) are calculated as follows:
˙V1(xt)=2(Aλx(t)+BλKτμx(t−τ(t))+Dλw(t))TZμx(t)+1hxT(t)(Zλ−Zτλ)x(t)+2(x(t)−x(t−τ1))TP1∫tt−τ1x(s)ds+2(x(t−τ1)−x(t−τ2))TP2∫t−τ1t−τ2x(s)ds+2[τ1x(t)−∫tt−τ1xT(s)ds]TP3∫0−τ1∫tt+θx(s)dsdθ+2[(τ2−τ1)x(t)−∫t−τ1t−τ2xT(s)ds]TP4∫−τ1−τ2∫tt+θx(s)dsdθ, | (3.10) |
˙V2(xt)≤xT(t)(Q1μ+Wμ)x(t)−xT(t−τ1)Q1μx(t−τ1)+xT(t−τ1)Q2μx(t−τ1)−xT(t−τ2)Q2μx(t−τ2)−(1−η)xT(t−τ(t))Wμx(t−τ(t)). | (3.11) |
Using Lemmas 3.1 and 3.2, we have
˙V3(xt)=τ21xT(t)X1μx(t)−τ1∫tt−τ1xT(s)X1μx(s)ds+τ21˙xT(t)X2˙x(t)−τ1∫tt−τ1˙xT(s)X2˙x(s)ds+(τ2−τ1)2xT(t)X3μx(t)−(τ2−τ1)∫t−τ1t−τ2xT(s)X3μx(s)ds+(τ2−τ1)2˙xT(t)X4˙x(t)−(τ2−τ1)∫t−τ1t−τ2˙xT(s)X4˙x(s)ds,≤τ21xT(t)X1μx(t)−ζT5(t)X1μζ5(t)+τ21˙xT(t)X2˙x(t)−(ζ1(t)−ζ3(t))TX2(ζ1(t)−ζ3(t))+(τ2−τ1)2xT(t)X3μx(t)−ζT6(t)X3μζ6(t)−ζT7(t)X3μζ7(t)−(1−α)ζT6(t)X3μζ6(t)−αζT7(t)X3μζ7(t)+(τ2−τ1)2˙xT(t)X4˙x(t)−(ζ2(t)−ζ3(t))TX4(ζ2(t)−ζ3(t))−(ζ2(t)−ζ4(t))TX4(ζ2(t)−ζ4(t))−(1−α)(ζ2(t)−ζ3(t))TX4(ζ2(t)−ζ3(t))−α(ζ2(t)−ζ4(t))TX4(ζ2(t)−ζ4(t)), | (3.12) |
˙V4(xt)=τ414xT(t)R1μx(t)−τ212∫0−τ1∫tt+βxT(s)R1μx(s)dsdβ+τ414˙xT(t)R2˙x(t)−τ212∫0−τ1∫tt+β˙xT(s)R2˙x(s)dsdβ+(τ22−τ21)24xT(t)R3μx(t)−τ22−τ212∫−τ1−τ2∫tt+βxT(s)R3μx(s)dsdβ+(τ22−τ21)24˙xT(t)R4˙x(t)−τ22−τ212∫−τ1−τ2∫tt+β˙xT(s)R4˙x(s)dsdβ≤τ414xT(t)R1μx(t)−ζT8(t)R1μζ8(t)+τ414˙xT(t)R2˙x(t)−(τ1ζ1(t)−ζ5(t))T(t)R2(τ1ζ1(t)−ζ5(t))+(τ22−τ21)24xT(t)R3μx(t)−ζT9(t)R3μζ9(t)−ζT10(t)R3μζ10(t)−(1−ε)ζT9(t)R3μζ9(t)−εζT10(t)R3μζ10(t)+(τ22−τ21)24˙xT(t)R4˙x(t)−((τ2−τ1)ζ1(t)−ζ7(t))TR4((τ2−τ1)ζ1(t)−ζ7(t))−((τ2−τ1)ζ1(t)−ζ6(t))TR4((τ2−τ1)ζ1(t)−ζ6(t))−ε((τ2−τ1)ζ1(t)−ζ7(t))TR4((τ2−τ1)ζ1(t)−ζ7(t))−(1−ε)((τ2−τ1)ζ1(t)−ζ6(t))TR4((τ2−τ1)ζ1(t)−ζ6(t)) | (3.13) |
˙V5(xt)=τ6136˙xT(t)U1˙x(t)−τ316∫0−τ1∫0β∫tt+λ˙xT(s)U1˙x(s)dsdλdβ+(τ32−τ31)236˙xT(t)U2˙x(t)−τ32−τ316∫−τ1−τ2∫0β∫tt+λ˙xT(s)U2˙x(s)dsdλdβ≤τ6136˙xT(t)U1˙x(t)−(τ212ζ1(t)−ζ8(t))TU1(τ212ζ1(t)−ζ8(t))+(τ32−τ31)236˙xT(t)U2˙x(t)−(τ22−τ212ζ1(t)−ζ9(t)−ζ10(t))TU2(τ22−τ212ζ1(t)−ζ9(t)−ζ10(t)). | (3.14) |
It follows from (3.10)–(3.14) that
˙V(xt)+zT(t)z(t)−γ2wT(t)w(t)=ζT(t)[r∑i=1r∑j=1r∑l=1λi(ξ)μj(ξ)μl(ξ(t−τ))(αθ(1)ijl+(1−α)θ(2)ijl+εθ(3)ijl+(1−ε)θ(4)ijl]ζ(t)+xT(t)(r∑i=1λi(ξ)Ci)T(r∑i=1λi(ξ)Ci)x(t)+˙xT(t)Ω˙x(t)Δ=ζT(t)[(αθ(1)λμμ+(1−α)θ(2)λμμ+εθ(3)λμμ+(1−ε)θ(4)λμμ]ζ(t)+ζT(t)eT1CTλCλe1ζ(t)+ζT(t)(Aλe1+BλKτμe2+Dλe11)TΩ(Aλe1+BλKτμe2+Dλe11)ζ(t) | (3.15) |
where θ(k)ijl=12θijl+θkj, k=1,2 and θ(k)ijl=12θijl+θkj, k=3,4. By Schur complement formula, the upper bound of ˙V is negative if and only if
r∑i=1r∑j=1r∑l=1λi(ξ)μj(ξ)μl(ξ(t−τ))[αθ(1)ijl+(1−α)θ(2)ijl+εθ(3)ijl+(1−ε)θ(4)ijlΦTilˉCTi∗−Ω−10∗∗−I]<0. | (3.16) |
(3.16) holds if and only if the following conditions hold simultaneously provided that δ2<δ1;
αΨ(1)λμμ+(1−α)Ψ(2)λμμ<−δ1I,εΨ(3)λμμ+(1−ε)Ψ(4)λμμ<δ2I |
where
Ψ(i)λμμ=[θ(i)λμμΦλμCTλ∗−Ω−10∗∗−I], i=1,2,3,4. |
The above conditions can be rewritten as
α(Ψ(1)λμμ+δ1I)+(1−α)(Ψ(2)λμμ+δ1I)<0, | (3.17) |
ε(Ψ(3)λμμ−δ2I)+(1−ε)(Ψ(4)λμμ−δ2I)<0. | (3.18) |
Since 0≤α, ε≤1, the terms α(Ψ(1)λμμ+δ1I)+(1−α)(Ψ(2)λμμ+δ1I) is a convex combination of Ψ(1)λμμ+δ1I and Ψ(2)λμμ+δ1I. Similarly, the terms ε(Ψ(3)λμμ−δ2I)+(1−ε)(Ψ(4)λμμ−δ2I) is a convex combination of Ψ(3)λμμ−δ2I and Ψ(4)λμμ−δ2I. These combinations are negative definite if the vertices become negative. Therefore, (3.17) and (3.18) are equivalent to
Ψ(1)λμμ+δ1I<0,Ψ(2)λμμ+δ1I<0,Ψ(3)λμμ−δ2I<0,Ψ(4)λμμ−δ2I<0 |
which can be written as (3.2)–(3.5). It follows from (3.15) that this proves that the conditions (3.2)–(3.6) suffice to show
˙V(xt)+zT(t)z(t)−γ2wT(t)w(t)<0. |
Integrating t=0 to t=∞, we have
V(x(∞))−V(x(0))+J<0. |
Since V(x(∞))≥0 and V(x(0))=0, we can show that J<0 and this achieves the H∞ disturbance attenuation of the system (2.5). The stability of the system with w(t)=0 is proved in the same lines as in [18].
Remark 3.1. The paper [18] uses the similar method to propose a stabilizing control design for nonlinear NCSs. It has shown that its method has advantaes over the previous methods in [6] and [7]. The novelty of Theorem 3.1 lies in a new multiple Lyapunov-Krasovskii function (3.9) where Zj, Wj, Q1j, Q2j, R1j, R3j, X1j and X3j are multiple Lyapunov matrices. In addition, the integral μi(ξ(t)), i=1,⋯,r of the membership functions avoid the derivatives of the membership function in the H∞ disturbance attenuation conditions (3.2)–(3.5). The quadruple integral terms and the quadratic forms of the double integral terms ∫∫xT(s)dsdβP∫∫xT(s)dsdβ are employed in (3.9), which leads to a drastic reduction of the conservatism in the H∞ disturbance attenuation condition. In fact, recent papers [6] and [7] do not use the quadruple integrals and the quadratic forms of the double integrals. This implies that our H∞ disturbance attenuation conditions are less conservative than recent results, and is technically better than others. In fact, this advantage was shown in [18].
Remark 3.2. The conditions (3.7)–(3.8) remove the positive definiteness of Q1i and Q2i, i=1,⋯,r, and reduce the conservatism in conditions in Theorem 3.1.
Remark 3.3. The conditions (3.2)–(3.8) are not strict LMIs unless h>0 is given. By defining ˜h=1h, these conditions can be seen as bilinear matrix inequalities. Effective algorithms to solve them include the branch-and-cut algorithm, the branch-and-bound algorithm, and the Lagrangian dual global optimization algorithm in [2,14] and [15], respectively.
Next, we shall propose a control design method. It is assumed that instead of the controller (2.4), a form of the controller is given by non-PDC, described by
u(t)=r∑i=1μi(ξ(t−τ(t)))Ki(r∑i=1μi(ξ(t−τ(t)))Zi)−1x(t−τ(t))=Kτμ(Zτμ)−1x(t−τ(t)) | (4.1) |
where Ki and Zi, i=1,⋯,r are to be determined, and μi, i=1,⋯,r are given as in (2.4). Then, the closed-loop system (2.1) with (4.1) becomes
˙x(t)=Aλx(t)+BλKτμ(Zτμ)−1x(t−τ(t))+Dλw(t). | (4.2) |
Applying Theorem 3.1, we obtain the following theorem for control design.
Theorem 4.1. For some scalar h>0. A controller (4.1) makes the fuzzy system (2.1)–(2.2) achieve the H∞ disturbance attenuation with γ if there exist matrices Zj>0, ˉP1mn>0, ˉP2mn>0, ˉP3mn>0, ˉP4mn>0, ˉR1jmn>0, ˉR2mn>0, ˉR3jmn>0, ˉR4mn>0, ˉX1jmn>0, ˉX2mn>0, ˉX3jmn>0, ˉX4mn>0, ˉU1mn>0, ˉU2mn>0, ˉWjmn, Kj,j,m,n=1,⋯,r, and scalars δi>0, i=1,2 such that
[ΥpijklmnΓijl∗ˉΩjkl]<0,i,j,k,l,m,n=1,⋯,r, p=1,⋯,4, | (4.3) |
δ1−δ2>0 | (4.4) |
[1τ1ˉZi+ˉX2mn−ˉX2mn−ˉX2mnˉQ1imn+ˉX2mn]≥0 i,m,n=1,⋯,r, | (4.5) |
[1τ2−τ1ˉZi+ˉX4mn−ˉX4mn−ˉX4mnˉQ2imn+ˉX4mn]≥0 i,m,n=1,⋯,r | (4.6) |
where
Υ1ijklmn=12ˉθijklmn+ˉθ1jmn+δ1I,Υ2ijklmn=12ˉθijklmn+ˉθ2jmn+δ1I,Υ3ijklmn=12ˉθijklmn+ˉθ3jmn−δ2I,Υ4ijklmn=12ˉθijklmn+ˉθ4jmn−δ2I,ˉθ1jmn=−eT7ˉX3jmne7−(e2−e4)TˉX4mn(e2−e4),ˉθ2jmn=−eT6ˉX3jmne6−(e2−e3)TˉX4mn(e2−e3),ˉθ3jmn=−eT10ˉR3jmne10−(τ12e1−e7)TˉR4mn(τ12e1−e7),ˉθ4jmn=−eT9ˉR3jmne9−(τ12e1−e6)TˉR4mn(τ12e1−e6),ˉθijlkmn=ˉπijlkmn−eT5ˉX1mne5−(e1−e3)TˉX2mn(e1−e3)−eT6ˉX3jmne6−eT7ˉX3jmne7−(e2−e3)TˉX4mn(e2−e3)−(e2−e4)TˉX4mn(e2−e4)−eT8ˉR1jmne8−(τ1e1−e5)TˉR2mn(τ1e1−e5)−eT9ˉR3jmne9−eT10ˉR3jmne10−(τ12e1−e6)TˉR4mn(τ12e1−e6)−(τ12e1−e7)TˉR4mn(τ12e1−e7)−(τ122e1−e8)TˉU1mn(τ122e1−e8)−(τ(2)122e1−e9−e10)TˉU2mn(τ(2)122e1−e9−e10) |
ˉΞkl=−ˉX2kl−τ21ˉR2kl−2τ212ˉR4kl−τ414ˉU1kl−(τ(2)12)24ˉU2kl,ˉπijklmn=[ˉΛijklBiKl00P1mn0τ1ˉP3mnτ12ˉP4mn∗−(1−η)Wjmn000000∗∗−ˉQ1jmn+ˉQ2jmn0−P1mnˉP2mnˉP2mn0∗∗∗−ˉQ2jmn0−ˉP2mn−ˉP2mn0∗∗∗∗000−ˉP3mn∗∗∗∗∗000∗∗∗∗∗∗00∗∗∗∗∗∗∗0∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗∗τ12ˉP4mn0Di000000000000−ˉP4mn−ˉP4mn0−ˉP4mn−ˉP4mn0000000∗00∗∗−γ2I], |
ˉΛijkl=AiZj+ZjATi+ˉQ1jkl+ˉWjkl−1h(ˉZi−ˉZl)+τ21ˉX1jkl+τ212ˉX3jkl+τ414ˉR1jkl+(τ(2)12)24ˉR3jkl,ΓTijl=[AiZjBiKl00000000 DiZjCiZj000000000 0],ˉΩjkl=[2(−2Zj+τ21ˉX2kl+τ212ˉX4kl+τ414ˉR2kl+(τ(2)12)24ˉR4kl+τ6136ˉU1kl+(τ32−τ31)236ˉU2kl)0∗−I] |
where τ12=τ2−τ1, τ(2)12=τ22−τ21. In this case, control gains Kl and Zj, j,l=1,⋯,r can be found as solutions of the above LMIs.
Proof: We consider the same Lyapunov-Krasovskii function (3.9) except for the first term of V1(xt), which is replaced by
ˉV1(xt)=xT(t)Z−1μx(t). |
The time-derivative of V11(xt) is calculated as
˙ˉV1(xt)=2xT(t)Z−1μ(Aλx(t)+BλKτμ(Zτμ)−1x(t−τ(t))+Dλw(t))+xT(t)˙Z−1μx(t)=xT(t)Z−1μ(AλZμ+ZμATλ−˙Zμ)Z−1μx(t)+2xT(t)Z−1μBλKτμ(Zτμ)−1x(t−τ(t)))+2xT(t)Z−1μDλw(t)) |
We follow the similar lines of proof of Theorem 3.1, and obtain
˙V(xt)=r∑i=1r∑j=1r∑k=1r∑l=1r∑m=1r∑n=1λi(ξ)μj(ξ)μk(ξ)μl(ξ)μm(ξ(t−τ))×μn(ξ(t−τ))ˉζT(t)(αˉθ(1)ijklmn+(1−α)ˉθ(2)ijklmn+εˉθ(3)ijklmn+(1−ε)ˉθ(4)ijklmn)ˉζ(t) |
where ˉθ(p)ijklmn=12˜θijklmn+ˉθpjmn, p=1,2, ˉθ(p)ijklmn=12˜θijklmn+ˉθpjmn, p=3,4,
˜θijklmn=ˉθijklmn+ΦTilΩΦil+[ZTμCTλCλZμ0⋯000⋯0⋮⋮⋱⋮00⋯0], |
ˉζ=[Z−1μ(Zτμ)−1⋯(Zτμ)−1I]ζ. |
We have defined the following matrices:
r∑j=1r∑k=1r∑l=1μj(ξ)μk(ξ)μl(ξ)ˉQjkl=ZμQμZμ,r∑j=1r∑m=1r∑n=1μj(ξ)μm(ξ(t−τ(t)))μn(ξ(t−τ(t)))ˉQjmn=ZτμQμZτμ |
for example. Similar notations have also been used for others matrices. Applying the Schur complement formula and the inequality −Ω−1≤−2Z+ZΩZ, we obtain (4.3)–(4.6).
Remark 4.1. In case that the delay rate η is unknown, we can still make use of Theorem 4.1 with Wj=0, j=1,⋯,r.
Remark 4.2. The conditions (4.3)–(4.6) are not strict LMIs unless h>0 is given, either. However, they can be solved in the same way as discussed in Remark 3.3.
We consider the system [19]
˙x(t)=2∑i=1λi(ξ){Aix(t)+Biu(t)+Diw(t)}, | (5.1) |
z(t)=2∑i=1λi(ξ)Cix(t) | (5.2) |
where x1(t)∈[1, −1] and
A1=[01−0.010], A2=[01−0.680], B1=[01], B2=[01], |
C1=[10.1], C2=[1.10.1], D1=[00.1],D2=[00.5], |
λ1(x1)=1−x21,λ2(x1)=x21. |
Suppose that 0.0≤τ(t)≤1.50 and η=0.3.
First, we compare our results with others to show the effectiveness of Theorem 3.1 for stabilization with w(t)=0 (Table 1).
This obviously show that our new multiple Lyapunov-Krasovskii function method is better than the existing conditions.
Next, we design an H∞ controller for the fuzzy networked system (5.1)–(5.2). Given the H∞ attenuation level γ=1, Theorem 4.1 gives the feedback control u(t) by
u(t)=Kτμ(Zτμ)−1x(t−τ(t)) | (5.3) |
where
K1=[0.0522−0.1368], K2=[0.1121−0.1643],Z1=[0.0936−0.0485−0.04850.1289], Z2=[0.0924−0.0468−0.04680.1258]. |
Theorem 4.1 is based on Theorem 3.1, which has been shown to be least conservative in the above numerical example. It implies that Theorem 4.1 is a control design method which requires less conservative design conditions than others.
Finally, the simulation result on the state trajectories of the closed-loop system with the initial conditions x(0)=[−0.5 0.5]T and the zero-mean Gaussian random variable w(t) of variance 0.1 is shown in Figure 1. The delay τ(t) is assumed to be τ(t)=1+0.5sin(0.1t). The bold and dotted lines indicate x1(t) and x2(t), respectively, and they show the system stability with disturbance attenuation.
The H∞ disturbance attenuation and control design of nonlinear networked control systems described by Takagi-Sugeno fuzzy systems have been considered. A new multiple Lyapunov-Krasovskii function was introduced to obtain new H∞ disturbance attenuation conditions for the closed-loop system. This technique leads to less conservative conditions. Control design method for nonlinear networked control systems was also proposed based on the same multiple Lyapnov-Krasovskii function and thus conditions for control design are less conservative than the existing ones.
The author declares that there is no conflicts of interest in this paper.
[1] |
Duc KN, Tien HN, Duy VN (2018) Performance enhancement and emission reduction of used motorcycles using flexible fuel technology. J Energy Inst 91: 145–152. https://doi.org/10.1016/j.esd.2017.12.005 doi: 10.1016/j.esd.2017.12.005
![]() |
[2] |
Duy VN, Duc KN, Cong DN, et al. (2019) Experimental study on improving performance and emission characteristics of used motorcycle fueled with ethanol by exhaust gas heating transfer system. Energy Sustainable Dev 51: 56–62. https://doi.org/10.1016/j.joei.2016.09.004 doi: 10.1016/j.joei.2016.09.004
![]() |
[3] |
Duc KN, Duy VN (2018) Study on performance enhancement and emission reduction of used fuel-injected motorcycles using bi-fuel gasoline-LPG. Energy Sustainable Dev 43: 60–67. https://doi.org/10.1016/j.esd.2019.05.006 doi: 10.1016/j.esd.2019.05.006
![]() |
[4] |
Yahuza I, Dandakouta H (2015) A performance review of ethanol-diesel blended fuel samples in compression-ignition engine. J Chem Eng Process Technol 6: 5. https://doi.org/10.4172/2157-7048.1000256 doi: 10.4172/2157-7048.1000256
![]() |
[5] |
Satgé De Caro P, Mouloungui Z, Vaitilingom G, et al. (2001) Interest of combining an additive with diesel-ethanol blends for use in diesel engines. Fuel 80: 565–574. https://doi.org/10.1016/S0016-2361(00)00117-4 doi: 10.1016/S0016-2361(00)00117-4
![]() |
[6] |
Yusri IM, Mamat R, Najafi G, et al. (2017) Alcohol based automotive fuels from first four alcohol family in compression and spark ignition engine: A review on engine performance and exhaust emissions. Renewable Sustainable Energy Rev 77: 169–181. https://doi.org/10.1016/j.rser.2017.03.080 doi: 10.1016/j.rser.2017.03.080
![]() |
[7] |
Edwin Geo V, Jesu Godwin D, Thiyagarajan S, et al. (2019) Effect of higher and lower order alcohol blending with gasoline on performance, emission and combustion characteristics of SI engine. Fuel 256: 115806. https://doi.org/10.1016/j.fuel.2019.115806 doi: 10.1016/j.fuel.2019.115806
![]() |
[8] |
Jin D, Choi K, Myung CL, et al. (2017) The impact of various ethanol-gasoline blends on particulates and unregulated gaseous emissions characteristics from a spark ignition direct injection (SIDI) passenger vehicle. Fuel 209: 702–712. https://doi.org/10.1016/j.fuel.2017.08.063 doi: 10.1016/j.fuel.2017.08.063
![]() |
[9] |
Krishnamoorthi M, Malayalamurthi R, He Z, et al. (2019) A review on low temperature combustion engines: Performance, combustion and emission characteristics. Renewable Sustainable Energy Rev 116: 109404. https://doi.org/10.1016/j.rser.2019.109404 doi: 10.1016/j.rser.2019.109404
![]() |
[10] |
Agarwal AK, Singh AP, Maurya RK (2017) Evolution, challenges and path forward for low temperature combustion engines. Prog Energy Combust Sci 61: 1–56. https://doi.org/10.1016/j.pecs.2017.02.001 doi: 10.1016/j.pecs.2017.02.001
![]() |
[11] |
Krishnamoorthi M, Malayalamurthi R, He Z, et al. (2019) A review on low temperature combustion engines: Performance, combustion and emission characteristics. Renewable Sustainable Energy Rev 116: 109404. https://doi.org/10.1016/j.rser.2019.109404 doi: 10.1016/j.rser.2019.109404
![]() |
[12] |
Yoshikawa T, Reitz RD (2009) Development of an improved NOx reaction mechanism for low temperature diesel combustion modeling. SAE Int J Engines 1: 1105–1117. https://doi.org/10.4271/2008-01-2413 doi: 10.4271/2008-01-2413
![]() |
[13] |
Shim E, Park H, Bae C (2020) Comparisons of advanced combustion technologies (HCCI, PCCI, and dual-fuel PCCI) on engine performance and emission characteristics in a heavy-duty diesel engine. Fuel 262: 116436. https://doi.org/10.1016/j.fuel.2019.116436 doi: 10.1016/j.fuel.2019.116436
![]() |
[14] |
Chaudhari VD, Deshmukh D (2019) Challenges in charge preparation and combustion in homogeneous charge compression ignition engines with biodiesel: A review. Energy Rep 5: 960–968. https://doi.org/10.1016/j.egyr.2019.07.008 doi: 10.1016/j.egyr.2019.07.008
![]() |
[15] |
Rajak U, Nashine P, Verma TN, et al. (2019) Performance, combustion and emission analysis of microalgae Spirulina in a common rail direct injection diesel engine. Fuel 255: 115855. https://doi.org/10.1016/j.fuel.2019.115855 doi: 10.1016/j.fuel.2019.115855
![]() |
[16] |
Saiteja P, Ashok B (2021) A critical insight review on homogeneous charge compression ignition engine characteristics powered by biofuels. Fuel 285: 119202. https://doi.org/10.1016/j.fuel.2020.119202 doi: 10.1016/j.fuel.2020.119202
![]() |
[17] |
Uyumaz A (2015) An experimental investigation into combustion and performance characteristics of an HCCI gasoline engine fueled with n-heptane, isopropanol and n-butanol fuel blends at different inlet air temperatures. Energy Convers Manage 98: 199–207. https://doi.org/10.1016/j.enconman.2015.03.043 doi: 10.1016/j.enconman.2015.03.043
![]() |
[18] |
Valero-Marco J, Lehrheuer B, López JJ, et al. (2018) Potential of water direct injection in a CAI/HCCI gasoline engine to extend the operating range towards higher loads. Fuel 231: 317–327. https://doi.org/10.15282/ijame.14.2.2017.17.0346 doi: 10.15282/ijame.14.2.2017.17.0346
![]() |
[19] |
Hunicz J (2014) An experimental study of negative valve overlap injection effects and their impact on combustion in a gasoline HCCI engine. Fuel 117: 236–250. https://doi.org/10.1016/j.fuel.2018.05.093 doi: 10.1016/j.fuel.2018.05.093
![]() |
[20] |
Yao M, Zheng Z, Liu H (2009) Progress and recent trends in homogeneous charge compression ignition (HCCI) engines. Prog Energy Combust Sci 35: 398–437. https://doi.org/10.1016/j.fuel.2013.09.079 doi: 10.1016/j.fuel.2013.09.079
![]() |
[21] |
Aljaberi HA, Aziz Hairuddin A, Aziz NA (2017) The use of different types of piston in an HCCI engine: A review. Int J Automot Mech Eng 14: 4348–4367. https://doi.org/10.15282/ijame.14.2.2017.17.0346 doi: 10.15282/ijame.14.2.2017.17.0346
![]() |
[22] |
Battin-Leclerc F (2008) Detailed chemical kinetic models for the low-temperature combustion of hydrocarbons with application to gasoline and diesel fuel surrogates. Prog Energy Combust Sci 34: 440–498. https://doi.org/10.1016/j.pecs.2007.10.002 doi: 10.1016/j.pecs.2007.10.002
![]() |
[23] |
Luong MB, Hernández Pérez FE, Im HG (2020) Prediction of ignition modes of NTC-fuel/air mixtures with temperature and concentration fluctuations. Combust Flame 213: 382–393. https://doi.org/10.1016/j.combustflame.2019.12.002 doi: 10.1016/j.combustflame.2019.12.002
![]() |
[24] |
Harada A, Shimazaki N, Sasaki S, et al. (1998) The effects of mixture formation on premixed lean diesel combustion engine. SAE Tech Pap. https://doi.org/10.4271/980533 doi: 10.4271/980533
![]() |
[25] |
Killingsworth NJ, Aceves SM, Flowers DL, et al. (2006) A simple HCCI engine model for control. Proc IEEE Int Conf Control Appl 2424–2429. https://doi.org/10.1109/CACSD-CCA-ISIC.2006.4777020 doi: 10.1109/CACSD-CCA-ISIC.2006.4777020
![]() |
[26] |
Mack JH, Aceves SM, Dibble RW (2009) Demonstrating direct use of wet ethanol in a homogeneous charge compression ignition (HCCI) engine. Energy 34: 782–787. https://doi.org/10.1016/j.energy.2009.02.010 doi: 10.1016/j.energy.2009.02.010
![]() |
[27] |
Shudo T, Kitahara S, Ogawa H (2006) Influence of carbon dioxide on combustion in an HCCI engine with the ignition-control by hydrogen. SAE Tech Pap. https://doi.org/10.4271/2006-01-3248 doi: 10.4271/2006-01-3248
![]() |
[28] |
Anh T Le, Duy VN, Thi HK, et al. (2018) Experimental investigation on establishing the HCCI process fueled by n-heptane in a direct injection diesel engine at different compression ratios. Sustainability 10: 3878. https://doi.org/10.3390/su10113878 doi: 10.3390/su10113878
![]() |
[29] |
Peucheret S, Wyszyński ML, Lehrle RS, et al. (2005) Use of catalytic reforming to aid natural gas HCCI combustion in engines: Experimental and modelling results of open-loop fuel reforming. Int J Hydrogen Energy 30: 1583–1594. https://doi.org/10.1016/j.ijhydene.2005.02.001 doi: 10.1016/j.ijhydene.2005.02.001
![]() |
[30] |
Hosseini V, Checkel MD (2006) Using reformer gas to enhance HCCI combustion of CNG in A CFR Engine. SAE Tech Pap. https://doi.org/10.4271/2006-01-3247 doi: 10.4271/2006-01-3247
![]() |
[31] |
Hyvönen J, Wilhelmsson C, Johansson B (2006) The effect of displacement on air-diluted multi-cylinder HCCI engine performance. SAE Tech Pap 2006. https://doi.org/10.4271/2006-01-0205 doi: 10.4271/2006-01-0205
![]() |
[32] |
Gnanam G, Sobiesiak A, Reader G, et al. (2006) An HCCI engine fuelled with iso-octane and ethanol. SAE Tech Pap. https://doi.org/10.4271/2006-01-3246 doi: 10.4271/2006-01-3246
![]() |
[33] |
Gray AW, Ryan TW (1997) Homogeneous charge compression ignition (HCCI) of diesel fuel. SAE Tech Pap. https://doi.org/10.4271/971676 doi: 10.4271/971676
![]() |
[34] |
Agarwal AK, Singh AP, Lukose J, et al. (2013) Characterization of exhaust particulates from diesel fueled homogenous charge compression ignition combustion engine. J Aerosol Sci 58: 71–85. https://doi.org/10.1016/j.jaerosci.2012.12.005 doi: 10.1016/j.jaerosci.2012.12.005
![]() |
[35] |
Kaiser EW, Matti Maricq M, Xu N, et al. (2005) Detailed hydrocarbon species and particulate emissions from a HCCI engine as a function of air-fuel ratio. SAE Tech Pap. https://doi.org/10.4271/2005-01-3749 doi: 10.4271/2005-01-3749
![]() |
[36] |
Price P, Stone R, Misztal J, et al. (2007) Particulate emissions from a gasoline homogeneous charge compression ignition engine. SAE Tech Pap 2007: 776–790. https://doi.org/10.4271/2007-01-0209 doi: 10.4271/2007-01-0209
![]() |
[37] |
Åmand LE, Leckner B (1991) Influence of fuel on the emission of nitrogen oxides (NO and N2O) from an 8-MW fluidized bed boiler. Combust Flame 84: 181–196. https://doi.org/10.1016/0010-2180(91)90047-F doi: 10.1016/0010-2180(91)90047-F
![]() |
[38] |
Ishii H, Koike N, Suzuki H, et al. (1997) Exhaust purification of diesel engines by homogeneous charge with compression ignition Part 2: Analysis of combustion phenomena and NOx formation by numerical simulation with experiment. SAE Tech Pap. https://doi.org/10.4271/970315 doi: 10.4271/970315
![]() |
[39] |
Swami Nathan S, Mallikarjuna JM, Ramesh A (2010) An experimental study of the biogas-diesel HCCI mode of engine operation. Energy Convers Manage 51: 1347–1353. https://doi.org/10.1016/j.enconman.2009.09.008 doi: 10.1016/j.enconman.2009.09.008
![]() |
[40] |
Hairuddin AA, Yusaf T, Wandel AP (2014) A review of hydrogen and natural gas addition in diesel HCCI engines. Renewable Sustainable Energy Rev 32: 739–761. https://doi.org/10.1016/j.rser.2014.01.018 doi: 10.1016/j.rser.2014.01.018
![]() |
[41] |
Olsson JO, Tunestål P, Johansson B, et al. (2002) Compression ratio influence on maximum load of a natural gas fueled HCCI engine. SAE Tech Pap 2002. https://doi.org/10.4271/2002-01-0111 doi: 10.4271/2002-01-0111
![]() |
[42] |
Yap D, Peucheret SM, Megaritis A, et al. (2006) Natural gas HCCI engine operation with exhaust gas fuel reforming. Int J Hydrogen Energy 31: 587–595. https://doi.org/10.1016/j.ijhydene.2005.06.002 doi: 10.1016/j.ijhydene.2005.06.002
![]() |
[43] |
Saravanan N, Nagarajan G (2008) An experimental investigation on a diesel engine with hydrogen fuel injection in intake manifold. SAE Tech Pap. https://doi.org/10.4271/2008-01-1784 doi: 10.4271/2008-01-1784
![]() |
[44] |
Yusaf TF, Buttsworth DR, Saleh KH, et al. (2010) CNG-diesel engine performance and exhaust emission analysis with the aid of artificial neural network. Appl Energy 87: 1661–1669. https://doi.org/10.1016/j.apenergy.2009.10.009 doi: 10.1016/j.apenergy.2009.10.009
![]() |
[45] |
Tsolakis A, Megaritis A, Yap D (2008) Application of exhaust gas fuel reforming in diesel and homogeneous charge compression ignition (HCCI) engines fuelled with biofuels. Energy 33: 462–470. https://doi.org/10.1016/j.energy.2007.09.011 doi: 10.1016/j.energy.2007.09.011
![]() |
[46] |
Lee MY, Lee GS, Kim CJ, et al. (2018) Macroscopic and microscopic spray characteristics of diesel and gasoline in a constant volume chamber. Energies 11. https://doi.org/10.3390/en11082056 doi: 10.3390/en11082056
![]() |
[47] |
Zhu H, Bohac SV., Huang Z, et al. (2013) Defeat of the soot/NOx trade-off using biodiesel-ethanol in a moderate exhaust gas recirculation premixed low-temperature combustion mode. J Eng Gas Turbines Power 135. https://doi.org/10.1115/1.4024380 doi: 10.1115/1.4024380
![]() |
[48] |
Lu X, Han D, Huang Z (2011) Fuel design and management for the control of advanced compression-ignition combustion modes. Prog Energy Combust Sci 37: 741–783. https://doi.org/10.1016/j.pecs.2011.03.003 doi: 10.1016/j.pecs.2011.03.003
![]() |
[49] |
LEE TYK (2012) Combustion and emission characteristics of wood pyrolysis oil-butanol blended fuels in a Di diesel engine. Int J Automot Technol 13: 293–300. https://doi.org/10.1007/s12239 doi: 10.1007/s12239
![]() |
[50] |
Singh AP, Agarwal AK (2012) An experimental investigation of combustion, emissions and performance of a diesel fuelled HCCI engine. SAE Tech Pap. https://doi.org/10.4271/2012-28-0005 doi: 10.4271/2012-28-0005
![]() |
[51] |
Turkcan A, Altinkurt MD, Coskun G, et al. (2018) Numerical and experimental investigations of the effects of the second injection timing and alcohol-gasoline fuel blends on combustion and emissions of an HCCI-DI engine. Fuel 219: 50–61. https://doi.org/10.1016/j.fuel.2018.01.061 doi: 10.1016/j.fuel.2018.01.061
![]() |
[52] |
Saxena S, Bedoya ID (2013) Fundamental phenomena affecting low temperature combustion and HCCI engines, high load limits and strategies for extending these limits. Prog Energy Combust Sci 39: 457–488. https://doi.org/10.1016/j.pecs.2013.05.002 doi: 10.1016/j.pecs.2013.05.002
![]() |
[53] |
Olsson JO, Tunestål P, Haraldsson G, et al. (2001) A turbo charged dual fuel HCCI engine. SAE Tech Pap. https://doi.org/10.4271/2001-01-1896 doi: 10.4271/2001-01-1896
![]() |
[54] |
Dec JE (2009) Advanced compression-ignition engines—Understanding the in-cylinder processes. Proc Combust Inst 32 Ⅱ: 2727–2742. https://doi.org/10.1016/j.proci.2008.08.008 doi: 10.1016/j.proci.2008.08.008
![]() |
[55] |
Aronsson U, Andersson Ö, Egnell R, et al. (2009) Influence of spray-target and squish height on sources of CO and UHC in a HSDI diesel engine during PPCI low-temperature combustion. SAE Tech Pap 4970. https://doi.org/10.4271/2009-01-2810 doi: 10.4271/2009-01-2810
![]() |
[56] |
Reitz RD, Duraisamy G (2015) Review of high efficiency and clean reactivity controlled compression ignition (RCCI) combustion in internal combustion engines. Prog Energy Combust Sci 46: 12–71. https://doi.org/10.1016/j.pecs.2014.05.003 doi: 10.1016/j.pecs.2014.05.003
![]() |
[57] |
Gowthaman S, Sathiyagnanam AP (2018) Analysis the optimum inlet air temperature for controlling homogeneous charge compression ignition (HCCI) engine. Alexandria Eng J 57: 2209–2214. https://doi.org/10.1016/j.aej.2017.08.011 doi: 10.1016/j.aej.2017.08.011
![]() |
[58] |
Tse TJ, Wiens DJ, Reaney MJT (2021) Production of bioethanol—A review of factors affecting ethanol yield. Fermentation 7: 1–18. https://doi.org/10.3390/fermentation7040268. doi: 10.3390/fermentation7040268
![]() |
[59] |
Jambo SA, Abdulla R, Mohd Azhar SH, et al. (2016) A review on third generation bioethanol feedstock. Renewable Sustainable Energy Rev 65: 756–769. https://doi.org/10.1016/j.rser.2016.07.064 doi: 10.1016/j.rser.2016.07.064
![]() |
[60] |
Koçar G, Civaş N (2013) An overview of biofuels from energy crops: Current status and future prospects. Renewable Sustainable Energy Rev 28: 900–916. https://doi.org/10.1016/j.rser.2013.08.022 doi: 10.1016/j.rser.2013.08.022
![]() |
[61] |
Malça J, Freire F (2006) Renewability and life-cycle energy efficiency of bioethanol and bio-ethyl tertiary butyl ether (bioETBE): Assessing the implications of allocation. Energy 31: 3362–3380. https://doi.org/10.1016/j.energy.2006.03.013 doi: 10.1016/j.energy.2006.03.013
![]() |
[62] |
Juodeikiene G, Cernauskas D, Vidmantiene D, et al. (2014) Combined fermentation for increasing efficiency of bioethanol production from Fusarium sp. contaminated barley biomass. Catal Today 223: 108–114. https://doi.org/10.1016/j.cattod.2013.09.028 doi: 10.1016/j.cattod.2013.09.028
![]() |
[63] |
Mardi MK, Abdolalipouradl M, Khalilarya S (2015) The effect of exhaust gas recirculation on performance and emissions of a SI engine fuelled with ethanol-gasoline blends. Int J Eng Trans A Basics 28: 133–138. https://doi.org/10.5829/idosi.ije.2015.28.01a.17 doi: 10.5829/idosi.ije.2015.28.01a.17
![]() |
[64] |
Zervas E, Montagne X, Lahaye J (2002) Emission of alcohols and carbonyl compounds from a spark ignition engine. Environ Sci Technol 36: 2414–2421. https://doi.org/10.1021/es010265t doi: 10.1021/es010265t
![]() |
[65] |
Abdel-Rahman AA, Osman MM (1997) Experimental investigation on varying the compression ratio of SI engine working under different ethanol-gasoline fuel blends. Int J Energy Res 21: 31–40. https://doi.org/10.1002/(SICI)1099-114X(199701)21:1<31::AID-ER235>3.0.CO;2-5 doi: 10.1002/(SICI)1099-114X(199701)21:1<31::AID-ER235>3.0.CO;2-5
![]() |
[66] |
Hsieh WD, Chen RH, Wu TL, Lin TH (2002) Engine performance and pollutant emission of an SI engine using ethanol–gasoline blended fuels. Atmos. Environ. 36: 403-410. https://doi.org/10.1016/S1352-2310(01)00508-8 doi: 10.1016/S1352-2310(01)00508-8
![]() |
[67] |
Chao HR, Lin TC, Chao MR, et al. (2000) Effect of methanol-containing additive on the emission of carbonyl compounds from a heavy-duty diesel engine. J Hazard Mater 73: 39–54. https://doi.org/10.1016/S0304-3894(99)00162-4 doi: 10.1016/S0304-3894(99)00162-4
![]() |
[68] |
Wu CW, Chen RH, Pu JY, et al. (2004) The influence of air-fuel ratio on engine performance and pollutant emission of an SI engine using ethanol-gasoline-blended fuels. Atmos Environ 38: 7093–7100. https://doi.org/10.1016/j.atmosenv.2004.01.058 doi: 10.1016/j.atmosenv.2004.01.058
![]() |
[69] |
Xing-Cai L, Jian-Guang Y, Wu-Gao Z, et al. (2004) Effect of cetane number improver on heat release rate and emissions of high speed diesel engine fueled with ethanol-diesel blend fuel. Fuel 83: 2013–2020. https://doi.org/10.1016/j.fuel.2004.05.003 doi: 10.1016/j.fuel.2004.05.003
![]() |
[70] |
Schifter I, Diaz L, Rodriguez R, et al. (2011) Combustion and emissions behavior for ethanol-gasoline blends in a single cylinder engine. Fuel 90: 3586–3592. https://doi.org/10.1016/j.fuel.2011.01.034 doi: 10.1016/j.fuel.2011.01.034
![]() |
[71] |
Hernandez JJ, Sanz-Argent J, Benajes J, et al. (2008) Selection of a diesel fuel surrogate for the prediction of auto-ignition under HCCI engine conditions. Fuel 87: 655–665. https://doi.org/10.1016/j.fuel.2007.05.019 doi: 10.1016/j.fuel.2007.05.019
![]() |
[72] |
Lü XC, Chen W, Huang Z (2005) A fundamental study on the control of the HCCI combustion and emissions by fuel design concept combined with controllable EGR. Part 1. the basic characteristics of HCCI combustion. Fuel 84: 1074–1083. https://doi.org/10.1016/j.fuel.2004.12.014 doi: 10.1016/j.fuel.2004.12.014
![]() |
[73] |
Lü X, Hou Y, Zu L, et al. (2006) Experimental study on the auto-ignition and combustion characteristics in the homogeneous charge compression ignition (HCCI) combustion operation with ethanol/n-heptane blend fuels by port injection. Fuel 85: 2622–2631. https://doi.org/10.1016/j.fuel.2006.05.003 doi: 10.1016/j.fuel.2006.05.003
![]() |
[74] |
Yao M, Chen Z, Zheng Z, et al. (2006) Study on the controlling strategies of homogeneous charge compression ignition combustion with fuel of dimethyl ether and methanol. Fuel 85: 2046–2056. https://doi.org/10.1016/j.fuel.2006.03.016 doi: 10.1016/j.fuel.2006.03.016
![]() |
[75] |
Ma JJ, Lü XJ, Ji LB, et al. (2008) An experimental study of HCCI-DI combustion and emissions in a diesel engine with dual fuel. Int J Therm Sci 47: 1235–1242. https://doi.org/10.1016/j.ijthermalsci.2007.10.007 doi: 10.1016/j.ijthermalsci.2007.10.007
![]() |
[76] |
Shi L, Cui Y, Deng K, et al. (2006) Study of low emission homogeneous charge compression ignition (HCCI) engine using combined internal and external exhaust gas recirculation (EGR). Energy 31: 2665–2676. https://doi.org/10.1016/j.energy.2005.12.005 doi: 10.1016/j.energy.2005.12.005
![]() |
[77] |
Dubreuil A, Foucher F, Mounaïm-Rousselle C, et al. (2007) HCCI combustion: Effect of NO in EGR. Proc Combust Inst 31 Ⅱ: 2879–2886. https://doi.org/10.1016/j.proci.2006.07.168 doi: 10.1016/j.proci.2006.07.168
![]() |
[78] |
Miller Jothi NK, Nagarajan G, Renganarayanan S (2008) LPG fueled diesel engine using diethyl ether with exhaust gas recirculation. Int J Therm Sci 47: 450–457. https://doi.org/10.1016/j.ijthermalsci.2006.06.012 doi: 10.1016/j.ijthermalsci.2006.06.012
![]() |
[79] |
Kim DS, Lee CS (2006) Improved emission characteristics of HCCI engine by various premixed fuels and cooled EGR. Fuel 85: 695–704. https://doi.org/10.1016/j.fuel.2005.08.041 doi: 10.1016/j.fuel.2005.08.041
![]() |
[80] |
Chang J, Fillpi Z, Assanis D, et al. (2005) Characterizing the thermal sensitivity of a gasoline homogeneous charge compression ignition engine with measurements of instantaneous wall temperature and heat flux. Int J Engine Res 6: 289–309. https://doi.org/10.1243/146808705X30558 doi: 10.1243/146808705X30558
![]() |
[81] |
Yao M, Zheng Z, Liu H (2009) Progress and recent trends in homogeneous charge compression ignition (HCCI) engines. Prog Energy Combust Sci 35: 398–437. https://doi.org/10.1016/j.pecs.2009.05.001 doi: 10.1016/j.pecs.2009.05.001
![]() |
[82] |
Peng Y, Tan M, Guo L, et al. (2007) Study the ethanol SI/HCCI combustion mode transition by using the fast thermal management system. Chinese Sci Bull 52: 2731–2736. https://doi.org/10.1007/s11434-007-0361-3 doi: 10.1007/s11434-007-0361-3
![]() |
[83] |
Canakci M (2008) An experimental study for the effects of boost pressure on the performance and exhaust emissions of a DI-HCCI gasoline engine. Fuel 87: 1503–1514. https://doi.org/10.1016/j.fuel.2007.08.002 doi: 10.1016/j.fuel.2007.08.002
![]() |
[84] | Ramana PV, Ce HIT (2016) Recent developments in HCCI engine technology with alternative fuels. 1–11. Avaiable from: https://www.researchgate.net/publication/311510663. |
[85] |
Aziz NA, Rahman NA, Innayatullah O (2013) Control of homogeneous charge compression ignition (HCCI) engine through stochastic variables. World Appl Sci J 27: 359–366. https://doi.org/10.5829/idosi.wasj.2013.27.03.1199 doi: 10.5829/idosi.wasj.2013.27.03.1199
![]() |
[86] |
Christensen M, Johansson B (1999) Homogeneous charge compression ignition with water injection. SAE Tech Pap. https://doi.org/10.4271/1999-01-0182 doi: 10.4271/1999-01-0182
![]() |
[87] |
Ng CKW, Thomson MJ (2007) Modelling of the effect of fuel reforming and EGR on the acceptable operating range of an ethanol HCCI engine. Int J Veh Des 44: 107–123. https://doi.org/10.1504/IJVD.2007.013221 doi: 10.1504/IJVD.2007.013221
![]() |
[88] |
Yap D, Megaritis A, Wyszynski ML (2004) An investigation into bioethanol homogeneous charge compression ignition (HCCI) engine operation with residual gas trapping. Energy Fuels 18: 1315–1323. https://doi.org/10.1021/ef0400215 doi: 10.1021/ef0400215
![]() |
[89] |
Yap D, Karlovsky J, Megaritis A, et al. (2005) An investigation into propane homogeneous charge compression ignition (HCCI) engine operation with residual gas trapping. Fuel 84: 2372–2379. https://doi.org/10.1016/j.fuel.2005.05.008 doi: 10.1016/j.fuel.2005.05.008
![]() |
[90] |
Zhang Y, He BQ, Xie H, et al. (2006) The combustion and emission characteristics of ethanol on a port fuel injection HCCI engine. SAE Tech Pap 2006. https://doi.org/10.4271/2006-01-0631 doi: 10.4271/2006-01-0631
![]() |
[91] |
MacK JH, Dibble RW, Buchholz BA, et al. (2005) The effect of the di-tertiary butyl peroxide (DTBP) additive on HCCI combustion of fuel blends of ethanol and diethyl ether. SAE Tech Pap. https://doi.org/10.4271/2005-01-2135 doi: 10.4271/2005-01-2135
![]() |
[92] |
Manente V, Tunestål P, Johansson B (2008) Influence of the wall temperature and combustion chamber geometry on the performance and emissions of a mini HCCI engine fueled with diethyl ether. SAE Tech Pap, 776–790. https://doi.org/10.4271/2008-01-0008 doi: 10.4271/2008-01-0008
![]() |
[93] |
Mack JH, Flowers DL, Buchholz BA, et al. (2005) Investigation of HCCI combustion of diethyl ether and ethanol mixtures using carbon 14 tracing and numerical simulations. Proc Combust Inst 30 II: 2693–2700. https://doi.org/10.1016/j.proci.2004.08.136 doi: 10.1016/j.proci.2004.08.136
![]() |
[94] |
Xie H, Wei Z, He B, et al. (2006) Comparison of HCCI combustion respectively fueled with gasoline, ethanol and methanol through the trapped residual gas strategy. SAE Tech Pap 2006. https://doi.org/10.4271/2006-01-0635 doi: 10.4271/2006-01-0635
![]() |
[95] |
Martinez-Frias J, Aceves SM, Flowers DL (2007) Improving ethanol life cycle energy efficiency by direct utilization of wet ethanol in HCCI engines. J Energy Resour Technol Trans ASME 129: 332–337. https://doi.org/10.1115/1.2794768 doi: 10.1115/1.2794768
![]() |
[96] |
Mack JH, Aceves SM, Dibble RW (2009) Demonstrating direct use of wet ethanol in a homogeneous charge compression ignition (HCCI) engine. Energy 34: 782–787. https://doi.org/10.1016/j.energy.2009.02.010 doi: 10.1016/j.energy.2009.02.010
![]() |
[97] |
Martinez-Frias J, Aceves SM, Flowers DL (2007) Improving ethanol life cycle energy efficiency by direct utilization of wet ethanol in HCCI engines. J Energy Resour Technol Trans ASME 129: 332–337. https://doi.org/10.1115/1.2794768 doi: 10.1115/1.2794768
![]() |
[98] |
Megaritis A, Yap D, Wyszynski ML (2007) Effect of water blending on bioethanol HCCI combustion with forced induction and residual gas trapping. Energy 32: 2396–2400. https://doi.org/10.1016/j.energy.2007.05.010 doi: 10.1016/j.energy.2007.05.010
![]() |
[99] |
Brewster S, Railton D, Maisey M, et al. (2007) The effect of E100 water content on high load performance of a spray guide direct injection boosted engine. SAE Tech Pap. https://doi.org/10.4271/2007-01-2648 doi: 10.4271/2007-01-2648
![]() |
[100] |
Olberding J, Beyerlein DCS, Steciak J, et al. (2005) Dynamometer testing of an ethanol-water fueled transit van. SAE Tech Pap. https://doi.org/10.4271/2005-01-3706 doi: 10.4271/2005-01-3706
![]() |
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