
Citation: Cheng-Peng Li, Cheng Zhonglin, Mobeen Munir, Kalsoom Yasmin, Jia-bao Liu. M-polynomials and topological indices of linear chains of benzene, napthalene and anthracene[J]. Mathematical Biosciences and Engineering, 2020, 17(3): 2384-2398. doi: 10.3934/mbe.2020127
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Chemical graph theory is an emerging subfield of Mathematical Chemistry which helps in providing us tools such as polynomials and functions [1] to characterize properties of substances [2]. Wiener index has been largely used in [3]. A general modelling of some vertex-based indices of benzenoid systems has been presented in [4] and hexagonal systems in [5]. These tools carry potential information relating the structural properties of a molecular substance. Mathematicians are actively developing structural polynomials and functions that can take structural parameters such as number of atoms or molecules in a certain unit or number of bonds etc. as inputs to these functions and the out put information will be related to the properties of these molecular substances [6]. The main problem comes in the development of a very general polynomial that can generate these key functions after successive operations of differentiation and integration. The Hosoya polynomial is one such ingredient in the context of distance-based topological indices and key functions obtained from it are Weiner index, hyper Weiner index, and Harary index [6]. The M-polynomial is quite similar to the Hosoya polynomial except the fact that it produces degree-based topological indices.
A similar breakthrough was obtained recently by Deutsch and Klavzar [7] in 2015 in the form of M-polynomial which is extensively used nowadays to obtain many degree-based indices of different structures. The Authors established closed forms of degree-based indices of some famous structures like nanostar dendrimers in [8], titania nanotubes in [9], V-phenylenic nanotubes and nanotori in [10], boron nanotubes in [11], polyhex nanoubes in [12] and benzenoid systems in [13]. These indices have been closely linked with properties of chemical substances [14]. Wiener indices of trees have been computed in [15] which have a lots of applications. Benzenoid hydrocarbons play a vital role in our environment, food and chemical industries. In this article we are concerned about some linear chains of hydrocarbon in which benzene is an integral element. All considered graphs are simple and connected. We fix G for a connected simple graph with edge set E(G) and vertex set V(G), du is the degree of vertex u, δ=min{du:u∈V(G)} and Δ=max{du:u∈V(G)}. The M- Polynomial of G is defined as
M(G,x,y)=∑δ≤j≤i≤Δmijxiyj, |
where mij is the number of edges uvϵE(G) such that i≤j [7]. For the sake of mere computation, we prefer to notate M(x,y)=f(x,y). In 1975 Milan Randic introduced the Randic index R−1/2(G) and he defined it as
R−1/2(G)=∑uvϵE(G)(1/√dudv). |
the generalized Randic index is defined as
Rα(G)=∑uvϵE(G)(1/dudv)α |
, [16]. Randic used this index to study molecular attributes in [17]. Bollobas et al. discussed graphs with maximal weight using Randic index in [18]. New look of this index is presented in [19]. Authors discussed some molecular graphs with Randic index in [20] and with maximal Randic index in [21]. The Inverse Randic index [22], is defined as
RRα(G)=∑uvϵE(G)(dudv)α. |
It is clear that R−1/2(G) is a special case of Rα(G) where α=−1/2. This index has vast application in diverse areas [23] and [24]. Some recent results about Randic index can be traced from [25]. Gutman and Trinajstic defined two other indices as
M1(G)=∑uvϵE(G)dudv, |
M2(G)=∑uvϵE(G)dudv, |
and the modified second Zagreb index is
Mm2(G)=∑uvϵE(G)1/dudv. |
For details about these indices we refer to [26] and [27]. Some properties of Zagreb index have been outlined in [28] The Symetric Division index is also an important index given as
SSD(G)=∑uvϵE(G){(min(du,dv))/(max(du,dv))+(max(du,dv))/(min(du,dv))} |
Harmonic Index is
H(G)=∑uvϵE(G)2/du+dv, |
the inverse sum index is
I(G)=∑uvϵE(G)dudv/(dudv), |
and the augmented Zagreb index is
A(G)=∑uvϵE(G){dudv/(du+dv−2)}3. |
For further details of these indices, we refer to [29] and [30] where Zagreb indices and some of its variants have been provided. We use the following notations for the operations
Dx=x∂f(x,y)∂x, |
Dy=y∂f(x,y)∂y, |
δx=∫x0f(t,y)tdt, |
δy=∫y0f(t,y)tdt, |
Jf(x,y)=f(x,x), |
and
Qα(f(x,y)=xαf(x,y). |
Benzenoid graphs play important part in industry of hydrocarbons. Saturation numbers of benzenoid graphs have been computed in [31]. Linear chains of these benzene contribute in formation of many other important hydrocarbons. In 1981 Graovac et al. studied about benzenoid system with zero Energy gap [32]. In 2001 Gutman discussed Hosoya polynomial of benzenooid graphs [33]. In 2004 Vukicevic et al. gave the results about the Wiener indices of Benzenoid graph [34]. In 2006 Gutman et al. computed the formula for calculating resonance energy of benzenoid hydrocarbons [35]. In 2009 vesel studied about 4-tiling of benzenoid graphs [36]. In 2011 Das et al. gave the spectral properties of some matrix of benzenoid systems [37].
In the present article we focus on the combinatorial and topological aspects of Linear chains of Benzene, Nepthalene and Anthracene graphs. In particular we establish closed results for M-polynomials of these systems and then using successive operations of calculus, we derive formulas for topological indices of these systems.
In this section we will compute M Polynomial of linear chains of benzene, napthalene and anthracene graphs and also some topological indices related to these graphs. We start with the linear chains of benzene.
.
Theorem 2.1.1 The M-Polynomial of linear chain of benzene graph is
M(Bn,x,y)=6x2y2+4(n−1)x3y2+(n−1)x3y3. |
Proof. Let Bn be the linear chain of benzene graph. Then from Figure 1 we have
|V(Bn)|=4n+2 |
|E(Bn)|=5n+1 |
The edge set E(Bn has following three partitions
|E2,2|={e=uvϵE(Bn)|du=2dv=2},|E3,2|={e=uvϵE(Bn)|du=3dv=2},|E3,3|={e=uvϵE(Bn)|du=3dv=3}, |
and
|E2,2|=6,|E3,2|=4(n−1),|E3,3|=n−1. |
Thus, M polynomial of Bn is
M(Bn,x,y)=∑i≥jmij(Bn)xiyj=∑2≥2m22(Bn)x2y2+∑3≥2m32(Bn)x3y2+∑3≥3m33(Bn)x3y3=∑2≥2m22(Bn)x2y2+∑3≥2m32(Bn)x3y2+∑3≥3m33(Bn)x3y3=|E2,2|x2y2+|E3,2|x3y2+|E3,3|x3y3=6x2y2+4(n−1)x3y2+(n−1)x3y3. |
Now using the operations discussed in introduction we have the following results,
proposition 2.1.2 Let Bn be linear chain of benzene graph then
1. M1(Bn)=26n−2
2. M2(Bn)=33n−9
3. Mm2(Bn)=7n/9+13/8
4. Rα(Bn)=(3α.2α+2+32α)n+(22α+1.3−3α.2α+2−32α)
5. RRα(Bn)=(1/3α.2α−1+1/32α)n+(3/22α−1−1/3α.2α−2−1/32α)
6. SSD(Bn)=32n/3+2
7. H(Bn)=29n/15+16/15
8. I(Bn)=63n/10−3/10
9. A(Bn)=2777n/64+295/64
Proof. Let
M(Bn,x,y)=6x2y2+4(n−1)x3y2+(n−1)x3y3. |
Then,
Dx(f(x,y))=12x2y2+12(n−1)x3y2+3(n−1)x3y3.Dy(f(x,y))=12x2y2+8(n−1)x3y2+3(n−1)x3y3.DyDx(f(x,y))=24x2y2+24(n−1)x3y2+9(n−1)x3y3.δx(f(x,y))=3x2y2+4/3(n−1)x3y2+1/3(n−1)x3y3.δxδy(f(x,y))=3/2x2y2+2/3(n−1)x3y2+1/9(n−1)x3y3.DαxDαy(f(x,y))=22α+1.3x2y2+3α.2α+2(n−1)x3y2+32α(n−1)x3y3.δαxδαy(f(x,y))=3/22α−1x2y2+1/3α.2α−2(n−1)x3y2+1/32α(n−1)x3y3.δyDx(f(x,y))=6x2y2+6(n−1)x3y2+(n−1)x3y3.δxDy(f(x,y))=6x2y2+6(n−1)x3y2+(n−1)x3y3.δxJ(f(x,y))=3/2x4+4/5(n−1)x5+1/6(n−1)x6.δxJ(DyDx(f(x,y)))=6x4+24/5(n−1)x5+3/2(n−1)x6.δ3xQ−2J(D3xD3y(f(x,y)))=48x2+32(n−1)x3+729/64(n−1)x4 |
1. First zagreb Index :
M1(Bn)=(Dx+Dy)f(x,y)|x=y=1=26n−2, |
2. Second Zagreb Index :
M2(Bn)=(DyDx)f(x,y)|x=y=1=33n−9, |
3. Modified Second Zagreb Index :
Mm2(Bn)=(δxδy)f(x,y)|x=y=1=7n/9+13/8, |
4. Generalized Randic Index :
Rα(Bn)=DαxDαy(f(x,y))|x=y=1=(3α.2α+2+32α)n+(22α+1.3−3α.2α+2−32α), |
5. Inverse randic Index :
RRα(Bn)=δαxδαy(f(x,y))|x=y=1=(1/3α.2α−1+1/32α)n+(3/22α−1−1/3α.2α−2−1/32α), |
6.Symmetric division Index:
SSD(Bn)=(δxDx+δyDy)f(x,y)|x=y=1=32n/3+2, |
7.Harmonic Index:
H(Bn)=2δxJ(f(x,y))|x=1=29n/15+16/15, |
8.Inverse Sum Index :
I(Bn)=δxJ(DyDx(f(x,y)))|x=1=63n/10−3/10, |
9. Augmented zagreb Index :
A(Bn)=δ3xQ−2J(D3xD3y(f(x,y)))|x=1=2777n/64+295/64, |
Now we move towards the second main object of this article. Figure 2 is a linear chain of Napthalene graphs.
. Theorem 2.1.3 The M-Polynomial of linear napthalene L.Nn graph is
M(L.Nn,x,y)=6x2y2+4(2n−1)x3y2+(5n−4)x3y3. |
Proof. Let L.Nn be the linear napthalene graph. Then from Figure 2 we have
|V(L.Nn)|=10n |
|E(L.Nn)|=13n−2. |
The edge set E(L.Nn has following three partitions
|E2,2|={e=uvϵE(L.Nn)|du=2dv=2},|E3,2|={e=uvϵE(L.Nn)|du=3dv=2},|E3,3|={e=uvϵE(L.Nn)|du=3dv=3}, |
and
|E2,2|=6,|E3,2|=8n−4=4(2n−1),|E3,3|=5n−4. |
Thus, M polynomial of L.Nn is
M(Bn,x,y)=∑i≥jmij(L.Nn)xiyj=∑2≥2m22(L.Nn)x2y2+∑3≥2m32(L.Nn)x3y2+∑3≥3m33(L.Nn)x3y3=∑2≥2m22(L.Nn)x2y2+∑3≥2m32(L.Nn)x3y2+∑3≥3m33(L.Nn)x3y3=|E2,2|x2y2+|E3,2|x3y2+|E3,3|x3y3=6x2y2+4(2n−1)x3y2+(5n−4)x3y3. |
proposition 2.1.4 Let L.Nn be linear napthalene graph then,
1. M1(L.Nn)=70n−20,
2. M2(L.Nn)=93n−36,
3. Mm2(L.Nn)=17n/9+7/18,
4. Rα(L.Nn)=(5.32α+3α.2α+3)n+(22α+1.3−3α.2α+2−4.32α),
5. RRα(L.Nn)=(5/32α+1/3α.2α−2)n+(3/22α−1−1/3α.2α−2−4/32α),
6. SSD(L.Nn)=82n/3−14/3,
7. H(L.Nn)=73n/15+1/15,
8. I(L.Nn)=171n/10−24/5,
9. A(L.Nn)=7741n/64−473/16.
Proof. Let
M(L.Nn,x,y)=6x2y2+4(2n−1)x3y2+(5n−4)x3y3. |
Then,
Dx(f(x,y))=12x2y2+12(2n−1)x3y2+3(5n−4)x3y3,Dy(f(x,y))=12x2y2+8(2n−1)x3y2+3(5n−4)x3y3,DyDx(f(x,y))=24x2y2+24(2n−1)x3y2+9(5n−4)x3y3,δx(f(x,y))=3x2y2+4/3(2n−1)x3y2+1/3(5n−4)x3y3,δxδy(f(x,y))=3/2x2y2+2/3(2n−1)x3y2+1/9(5n−4)x3y3,DαxDαy(f(x,y))=22α+1.3x2y2+3α.2α+2(2n−1)x3y2+32α(5n−4)x3y3,δαxδαy(f(x,y))=3/22α−1x2y2+1/3α.2α−2(2n−1)x3y2+1/32α(5n−4)x3y3,δyDx(f(x,y))=6x2y2+6(n−1)x3y2+(5n−4)x3y3,δxDy(f(x,y))=6x2y2+8/3(2n−1)x3y2+(5n−4)x3y3,δxJ(f(x,y))=3/2x4+4/5(2n−1)x5+1/6(5n−4)x6,δxJ(DyDx(f(x,y)))=6x4+24/5(2n−1)x5+3/2(5n−4)x6,δ3xQ−2J(D3xD3y(f(x,y)))=48x2+32(2n−1)x3+729/64(5n−4)x4. |
1. First zagreb Index :
M1(L.Nn)=(Dx+Dy)f(x,y)|x=y=1=70n−20. |
2. Second Zagreb Index :
M2(L.Nn)=(DyDx)f(x,y)|x=y=1=93n−36. |
3. Modified Second Zagreb Index :
Mm2(L.Nn)=(δxδy)f(x,y)|x=y=1=17n/9+7/18. |
4. Generalized randic Index :
Rα(L.Nn)=DαxDαy(f(x,y))|x=y=1=(5.32α+3α.2α+3)n+(22α+1.3−3α.2α+2−4.32α). |
5. Inverse randic Index :
RRα(L.Nn)=δαxδαy(f(x,y))|x=y=1=(5/32α+1/3α.2α−2)n+(3/22α−1−1/3α.2α−2−4/32α). |
6.Symmetric division Index:
SSD(L.Nn)=(δxDx+δyDy)f(x,y)|x=y=1=82n/3−14/3. |
7.Harmonic Index:
H(L.Nn)=2δxJ(f(x,y))|x=1=73n/15+1/15. |
8.Inverse Sum Index :
I(L.Nn)=δxJ(DyDx(f(x,y)))|x=1=171n/10−24/5. |
9. Augmented zagreb Index :
A(L.Nn)=δ3xQ−2J(D3xD3y(f(x,y)))|x=1=7741n/64−473/16. |
Now we move towards the theoretical aspects of linear chain of anthracene graphs. Following Figure 3 gives a mathematical pattern of carbon atoms sequencing.
Theorem 2.1.5 The M-Polynomial of linear anthracene L.An graph is
M(L.An,x,y)=6x2y2+4(3n−1)x3y2+2(3n−2)x3y3. |
Proof. Let L.An be the linear anthracene graph. Then from figure 3 we have
|V(L.An)|=14n, |
|E(L.An)|=18n−2, |
The edge set E(L.An has following three partitions
|E2,2|={e=uvϵE(L.An)|du=2dv=2},|E3,2|={e=uvϵE(L.An)|du=3dv=2},|E3,3|={e=uvϵE(L.An)|du=3dv=3}, |
and
|E2,2|=6,|E3,2|=4(3n−1),|E3,3|=2(3n−2). |
Thus, M polynomial of L.An is
M(Bn,x,y)=∑i≥jmij(L.An)xiyj,=∑2≥2m22(L.An)x2y2+∑3≥2m32(L.An)x3y2+∑3≥3m33(L.An)x3y3,=∑2≥2m22(L.An)x2y2+∑3≥2m32(L.An)x3y2+∑3≥3m33(L.An)x3y3,=|E2,2|x2y2+|E3,2|x3y2+|E3,3|x3y3=6x2y2+4(3n−1)x3y2+2(3n−2)x3y3, |
proposition 2.1.6 Let L.An be linear anthracene graph then,
1. M1(L.An)=96n−20,
2. M2(L.An)=126n−36,
3. Mm2(L.An)=8n/3+7/18,
4. Rα(L.An)=(32α+1.2+3α+1.2α+2)n+(22α+1.3−3α.2α+2−32α.22),
5. RRα(L.An)=(1/3α−1.2α−2+2/32α−1)n+(3/22α−1−1/3α.2α−2−4/32α),
6. SSD(L.An)=38n−14/3,
7. H(L.An)=34n/5+1/15,
8. I(L.An)=117n/5−24/5,
9. A(L.An)=825n−473/16.
Proof. Let
M(L.An,x,y)=6x2y2+4(3n−1)x3y2+2(3n−2)x3y3. |
Then,
Dx(f(x,y))=12x2y2+12(3n−1)x3y2+6(3n−2)x3y3,Dy(f(x,y))=12x2y2+8(3n−1)x3y2+6(3n−2)x3y3,DyDx(f(x,y))=24x2y2+24(3n−1)x3y2+18(3n−2)x3y3,δx(f(x,y))=3x2y2+4/3(3n−1)x3y2+2/3(3n−2)x3y3,δxδy(f(x,y))=3/2x2y2+2/3(3n−1)x3y2+2/9(3n−2)x3y3,DαxDαy(f(x,y))=22α+1.3x2y2+3α.2α+2(3n−1)x3y2+32α.2(3n−2)x3y3,δαxδαy(f(x,y))=3/22α−1x2y2+1/3α.2α−2(3n−1)x3y2+2/32α(3n−2)x3y3,δyDx(f(x,y))=6x2y2+6(3n−1)x3y2+2(3n−2)x3y3,δxDy(f(x,y))=6x2y2+8/3(3n−1)x3y2+2(3n−2)x3y3,δxJ(f(x,y))=3/2x4+4/5(3n−1)x5+1/3(3n−2)x6,δxJ(DyDx(f(x,y)))=6x4+24/5(3n−1)x5+3(3n−2)x6,δ3xQ−2J(D3xD3y(f(x,y)))=48x2+32(3n−1)x3+729/32(3n−2)x4. |
1. First zagreb Index :
M1(L.An)=(Dx+Dy)f(x,y)|x=y=1=96n−20 |
2. Second Zagreb Index :
M2(L.An)=(DyDx)f(x,y)|x=y=1=126n−36 |
3. Modified Second Zagreb Index :
.Mm2(L.An)=(δxδy)f(x,y)|x=y=1=8n/3+7/18 |
4. Generalized randic Index :
Rα(L.An)=DαxDαy(f(x,y))|x=y=1=(32α+1.2+3α+1.2α+2)n+(22α+1.3−3α.2α+2−32α.22) |
5. Inverse randic Index :
RRα(L.An)=δαxδαy(f(x,y))|x=y=1=(1/3α−1.2α−2+2/32α−1)n+(3/22α−1−1/3α.2α−2−4/32α) |
6.Symmetric division Index:
SSD(L.An)=(δxDx+δyDy)f(x,y)|x=y=1=38n−14/3 |
7.Harmonic Index:
H(L.An)=2δxJ(f(x,y))|x=1=34n/5+1/15 |
8.Inverse Sum Index :
I(L.An)=δxJ(DyDx(f(x,y)))|x=1=117n/5−‘24/5 |
9. Augmented zagreb Index :
A(L.An)=δ3xQ−2J(D3xD3y(f(x,y)))|x=1=825n−473/16. |
In this paper we derived M-polynomials and closed forms of some degree-based topological indices of linear chains of benzene, napthalene and anthracene graphs. Actual features about these results are the correlation of these indices on the basic units of these three chains. These indices could potentially play a significant role in determining properties of these compounds and others in which these compounds are used. It is important to mention here that some of these topological indices are derived directly by using techniques and definitions available in the literature.
Conceptualization, Mobeen Munir and Jiabao Liu; Investigation, Cheng Zhonglin and Cheng-Peng Li; Writing original draft, Kalsoom Yasmin.
We are highly thankful to reviewer's comments to improve the quality of article.
This research is funded from Major natural science research projects in Colleges and universities of Anhui Province in 2019 (No. KJ2019 ZD77).
The authors declare that they have no competing interests.
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