# On Computation and Analysis of Topological Index-Based Invariants for Complex Coronoid Systems

Authors: Muhammad Aamer Rashid; Sarfraz Ahmad; Muhammad Kamran Siddiqui; Mohammed K. A. Kaabar
Journal: Complexity
 (2021)

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## Abstract

In chemical graph theory, benzenoid systems are interrogated as they exhibit the chemical compounds known as benzenoid hydrocarbons. Benzenoid schemes are circumscribed as planar connected finite graphs having no cut vertices wherein the entire internal sections are collaboratively congruent regular hexagon. The past couple of decennium has acknowledged an extravagant development regarding implementation of information theoretic framework in miscellaneous ramification of science, for instance, in social sciences, biological, physical, and engineering. Explicitly, this tremendous improvement has been outstanding in the field of soft computing, molecular biology, and information technology. The information theory, delineated by Claud Shannon, has no less importance when it was considered. Shannon put forwarded the apprehension of entropy to enumerate upper bounds in transmission rates in telephonic channels, in optical communication, and in wireless. The prestigious feature of entropy is that it entitles the amount of uncertainty in a system. The substantial participation of this paper is to explore characteristics of graph entropies and then keep moving forward to talk about the formation of coronoid polycyclic aromatic hydrocarbons. Likewise, we estimate entropies through precise topological indices established on degree of terminal nodes.


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## Body

## 1. Introduction

ConsiderD=DV,DE be a graph containing DV and DE as the vertex set and the edge set of D correspondingly. The size and the order of D are expressed by m and n correspondingly, and §^a is characterized as the degree of any vertex a. Topological descriptors of a chemical structure are molecular descriptors. In QSPR/QSAR analyses, miscellaneous molecular descriptor is operated to correlate different biological and physico-chemical activities. In this study, we will talk about some degree-based indices.To determine the unpredictability of a scheme, entropy is used [1]. This consideration was grown for analyzing the fundamental information of graphs. Laterally, it was employed substantially in graphs and chemical networks. The graph entropy [2] consideration demonstrated on the denominations of vertex orbits. Utilization of graph entropy is interdisciplinary [3].In the literature, diverse graph entropies are estimated by means of degree of vertex, order of the graphs, eccentricity of the vertices, and characteristic polynomials [4, 5]. Over the past few years, graph entropies are estimated which are established on matchings, independent sets, and degree of vertices [6]. Mowshowits and Dehmer talked about few relations between the complexity of graphs and Hosoya entropy. We postulated that the presented degree-based entropy can be employed to assess network diversity. Equivalent entropy measures which are established on vertex-degrees to distinguish network diversity have been suggested by Tan and Wu [7].In chemical graph theory, benzenoid structures are interrogated [8] since they exhibit the chemical compounds known as benzenoid hydrocarbons. Benzenoid schemes are circumscribed as planar connected finite graphs having no cut vertices wherein the entire internal sections are collaboratively congruent regular hexagons.In [9], interpretation of the entropy was put forwarded for the edge weighted graph D=Dv;DE;ψaz, in which DV, DE, and ψaz symbolize the set of vertices, the set of edges, and the edge weight of the edge az in D correspondingly. Subsequently the entropy of the edge weighted graph is portrayed in the following equation. The relation between topological indices and corresponding entropy measures is presented in Table 1.(1)ENTψD=−∑a′z′∈Deψa′z′∑az∈DEψazlogψa′z′∑az∈DEψaz.Table 1
Degree-based topological indices together with their corresponding edge weightψaz of the edge az.
Degree-based topological indicesEdge weightψaz of the edge azEntropiesThe randic´ index [10]§^r×§^sα, α=1,−1,1/2,−1/2The randic´ entropy [11]The atom bond connectivity index [12]§^r+§^s−2/§^r×§^sThe atom bond connectivity entropy [11]The geometric arithmetic index [13]2§^r×§^s/§^r+§^s.The geometric arithmetic entropy [11]


## 2. Structure of Coronoid Polycyclic Aromatic Hydrocarbons

Coronoids are derived by these benzenoid systems by removing some interior vertices or edges. This will create a different interior region enclosed by a polygon having greater than six edges. By using the abovementioned conditions, more than one hexagon can be trimmed from the originator benzenoid structure. Coronoid is a benzenoid with a hole. It may have more than one hole. Graphical illustration of coronoid and noncoronoid systems is provided in Figures1(a) and 1(b). It is to be noted that Figure 1(b) is noncoronoid because some of its edges do not belong to any of its hexagons [14].Figure 1
Coronoid and noncoronoid systems.
(a)(b)tCycloarenes are macrocyclic combined compounds constituted by circumferentially connected benzene loops that enclose a hole with inner-directed carbon-hydrogen bonds. As a consequence, cycloarenes are connected with a subclass of circulenes or coronoids. The background of cycloarenes traces back to 1987; meanwhile, the main example with 12 benzene rings, categorized as kekulene, was disclosed by Staab and Diederich [15]. There have been countless hypothetical investigations focusing on the magnetic tendency, vibrational rate of occurrences of cycloarenes, and aromaticity [16]. Kekulene and cyclo decakis benzene were the merely two substantial patterns accessible for analysis [17].Afterwards, Kumar et al. [18] synthesized another model of cycloarene, with 14 benzene rings, specifically septulene. The synthesis of kekulene and septulene has kick started numerous theoretical and experimental studies on coronoids [19]. The study of coronoids is also gaining momentum due to their superaromaticity. Superaromaticity or macrocyclic aromaticity is described as an additional thermodynamic consolidation as a consequence of macrocyclic association in tremendous-ring molecules like kekulene, and it constitutes a little contribution of universal aromaticity.Whole coronoids investigated until now are approximately superaromatic through constructive superaromatic stabilization energies (SSEs). Intriguingly, the extent of SSE oscillates between single-layered and several-layered species. SSEs for even-layered coronoids [9, 20–22] are high, while those for odd-layered ones [5, 23, 24] are pretty low [23]. This provides an impetus for a deeper study into the properties of coronoid systems and their relationship with the underlying molecular structures. This study might be applicable to various fields of nanotechnology. As an illustration, the eradication of a unique carbon atom with a graphite framework establishes a one-atom hole referred to as a Schottky defect [25]. Individual-wall nanocones, [26] grime platelets, [27], and extended graphite layers [24] may contain vacancy hole defects involving larger (multiatom) holes which can be studied by modeling them as coronoids [28]. Graphenes are nanosized polycyclic aromatic hydrocarbons with potential uses in the fabrication of organic electronic devices [29]. The origination of coronoids by demonstrating a cavity in nanographene might be an efficacious approach to regulate their electronic and optical properties without amendments to their exterior structures. The cavities, that make an integral part of the coronoids, act as prototypes for scheming and synthesizing novel nanomaterials of significance in nano and biotechnology and the incipient field of nano-medicines. They have also been used in the design and synthesis of distinct porous and mesoporous materials grounded on calixarenes and mesoporous silica for the sequestration and complexation of toxic nuclear waste and other environmental pollutants [30] Coronoid systems are also widely examined in the study of coronoid hydrocarbons.It has been proved that it is possible to compute the totalπ-electron energy, the resonance energy, and the enumeration of coronoid hydrocarbons accurately using the knowledge of coronoid structures [20]. The conjugate graph-theoretical circuit theory, inspired by Clar’s aromatic sextet, correlates to the description of diverse enclosed consolidated cycles existing in the polycyclic aromatic compounds [31, 32]. This theory also provides combinatorial and graph-theoretical methods for efficient determination of the relative stabilities of coronoid structures, graphenes, cycloarenes, carbon nanotubes, and nanotori. For further information on the comprehensive research issued on coronoid systems by both Dias with coauthors and Cyvin with coauthors, refer to [21]. In comparison to the computationally intensive quantum chemical calculations, the graph-theoretical techniques are considerably more productive in obtaining the properties of coronoid systems. During a recent investigation, Aihara et al. [23] emphasized that the graph theory is not merely an extremely valuable mechanism in estimating topological resonance energies but additionally in uncovering significant challenges along the previous speculations of aromaticity. By employing graph-theoretical approaches, the investigation of coronoid networks has gained increased importance [22].


## 3. Coronoid SystemC1u,v,w,x

In this fragment, we will take into consideration the single coronoid system. This system is also recognised as one hole benzenoid. It is extracted by eradicating few of the interior edges or vertices from the benzenoid system. In this procedure, a hole is created within the system having a lowest size of two benzenes. Thex-circumscribed basic coronoid system is defined as Cku,v,w,x, k=1,2, in which u≥3, v,w≥1, and x≥1. The coronoid structure fluctuates correspondingly to its parameters u, v, w, and x bringing escalation to the particular cases. In [21, 33], some particular cases are discussed, and these exclusive models are employed to prognosticate the resonance energy of aromatic molecules. In theoretical chemistry, these models are considered as ideal models to investigate conjugation circuits of π electrons.These special cases are used to predict the resonance energy of aromatic molecules and have attracted a great deal of interest in the field of theoretical chemistry as ideal models to explore conjugation circuits ofπ-electrons [34, 35]. We will represent coronoid structure as C1u,v,w,x in which u≥3 and 1≤v≤w≤u. Figure 2 illustrates C1u,v,w,x graphically.Figure 2
Coronoid system ofC1u,v,w,x [34].Table2 portrays the edge partition of C1u,v,w,x on the basis of degrees of terminal vertices of each edge.Table 2
Edge partition of the coronoid systemC1u,v,w,x on the basis of degrees of terminal vertices of each edge.
§^a,§^zNumber of replicationClasses of edges2,26DE12,34u+6v+2w+22DE23,36x+8u+9x+12v+3x+4w+9x2+3x−58DE3


### 3.1. Results for Coronoid SystemC1u,v,w,x

#### 3.1.1. Randic´ Entropy of C1u,v,w,x

We enumerate the Randic´ index for α=1,−1,1/2,−1/2 with the help of Tables 1 and 2 as follows:(2)RαC1u,v,w,x=6×4α+4u+6v+2w+22×6α+6x+8u+9x+12v+3x+4w+9x2+3x−58×9α.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(3)ENTRαC1u,v,w,x=logRα−1Rα∑i=13∑az∈DEi§^a×§^zαlog§^a×§^zα,ENTRαC1u,v,w,x=logRα−6Rα4αlog4α−4u+6v+2w+22Rα6αlog6α−6x+8u+9x+12v+3x+4w+9x2+3x−58Rα9αlog9α,ENTR1C1u,v,w,x=log96+54xu+144+81xv+48+27xw+81x2+27x−366−24log496+54xu+144+81xv+48+27xw+81x2+27x−366−64u+6v+2w+22log696+54xu+144+81xv+48+27xw+81x2+27x−366−96x+8u+9x+12v+3x+4w+x2+3x−58log996+54xu+144+81xv+48+27xw+81x2+27x−366,ENTR1/2C1u,v,w,x=log46+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−12log246+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−64u+6v+2w+22log646+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−36x+8u+9x+12v+3x+4w+x2+3x−58log346+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162,ENTR−1C1u,v,w,x=log149+2x3u+73+xv+79+x3w+x2+x3−2318+3/2log414/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18+1/64u+6v+2w+22log614/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18+1/96x+8u+9x+12v+3x+4w+x2+3x−58log914/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18,ENTR−1/2C1u,v,w,x=log46+2x+83u+6+3x+4v+26+x+43w+3x2+x+226−493+3/2log24/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3+1/64u+6v+2w+22log64/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3+1/36x+8u+9x+12v+3x+4w+x2+3x−58log34/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3.


#### 3.1.2. The Atom Bond Connectivity Entropy ofC1u,v,w,x

Simple calculations with Tables1 and 2 yield the atom bond connectivity index as follows:(4)ABCC1u,v,w,x=22+4x+163u+32+6x+8v+2+2x+83w+6x2+2x+142−1163.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(5)ENTABCC1u,v,w,x=logABC−1ABC∑i=13∑az∈DEi§^a+§^z−2§^a×§^zlog§^a+§^z−2§^a×§^z,ENTABCC1u,v,w,x=log22+4x+163u+32+6x+8v+2+2x+83w+6x2+2x+142−1163−61/2log1/222+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3−4u+6v+2w+221/2log1/222+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3−6x+8u+9x+12v+3x+4w+x2+3x−582/3log2/322+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3.


#### 3.1.3. The Geometric Arithmetic EntropyC1u,v,w,x

Simple calculations with Tables1 and 2 yield the geometric arithmetic index as follows:(6)GAG=865+6x+8u+1265+9x+12v+465+3x+4w+9x2+3x−52+4465.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(7)ENTGAC1u,v,w,x=logGA−1GA∑i=13∑az∈DEi2§^a×§^z§^a+§^zlog2§^a×§^z§^a+§^z,ENTGAC1u,v,w,x=log865+6x+8u+1265+9x+12v+465+3x+4w+9x2+3x−52+4465−4u+6v+2w+2226/5log26/586/5+6x+8u+126/5+9x+12v+46/5+3x+4w+9x2+3x−52+446/5.


## 3.1. Results for Coronoid SystemC1u,v,w,x

### 3.1.1. Randic´ Entropy of C1u,v,w,x

We enumerate the Randic´ index for α=1,−1,1/2,−1/2 with the help of Tables 1 and 2 as follows:(2)RαC1u,v,w,x=6×4α+4u+6v+2w+22×6α+6x+8u+9x+12v+3x+4w+9x2+3x−58×9α.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(3)ENTRαC1u,v,w,x=logRα−1Rα∑i=13∑az∈DEi§^a×§^zαlog§^a×§^zα,ENTRαC1u,v,w,x=logRα−6Rα4αlog4α−4u+6v+2w+22Rα6αlog6α−6x+8u+9x+12v+3x+4w+9x2+3x−58Rα9αlog9α,ENTR1C1u,v,w,x=log96+54xu+144+81xv+48+27xw+81x2+27x−366−24log496+54xu+144+81xv+48+27xw+81x2+27x−366−64u+6v+2w+22log696+54xu+144+81xv+48+27xw+81x2+27x−366−96x+8u+9x+12v+3x+4w+x2+3x−58log996+54xu+144+81xv+48+27xw+81x2+27x−366,ENTR1/2C1u,v,w,x=log46+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−12log246+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−64u+6v+2w+22log646+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−36x+8u+9x+12v+3x+4w+x2+3x−58log346+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162,ENTR−1C1u,v,w,x=log149+2x3u+73+xv+79+x3w+x2+x3−2318+3/2log414/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18+1/64u+6v+2w+22log614/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18+1/96x+8u+9x+12v+3x+4w+x2+3x−58log914/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18,ENTR−1/2C1u,v,w,x=log46+2x+83u+6+3x+4v+26+x+43w+3x2+x+226−493+3/2log24/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3+1/64u+6v+2w+22log64/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3+1/36x+8u+9x+12v+3x+4w+x2+3x−58log34/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3.


### 3.1.2. The Atom Bond Connectivity Entropy ofC1u,v,w,x

Simple calculations with Tables1 and 2 yield the atom bond connectivity index as follows:(4)ABCC1u,v,w,x=22+4x+163u+32+6x+8v+2+2x+83w+6x2+2x+142−1163.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(5)ENTABCC1u,v,w,x=logABC−1ABC∑i=13∑az∈DEi§^a+§^z−2§^a×§^zlog§^a+§^z−2§^a×§^z,ENTABCC1u,v,w,x=log22+4x+163u+32+6x+8v+2+2x+83w+6x2+2x+142−1163−61/2log1/222+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3−4u+6v+2w+221/2log1/222+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3−6x+8u+9x+12v+3x+4w+x2+3x−582/3log2/322+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3.


### 3.1.3. The Geometric Arithmetic EntropyC1u,v,w,x

Simple calculations with Tables1 and 2 yield the geometric arithmetic index as follows:(6)GAG=865+6x+8u+1265+9x+12v+465+3x+4w+9x2+3x−52+4465.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(7)ENTGAC1u,v,w,x=logGA−1GA∑i=13∑az∈DEi2§^a×§^z§^a+§^zlog2§^a×§^z§^a+§^z,ENTGAC1u,v,w,x=log865+6x+8u+1265+9x+12v+465+3x+4w+9x2+3x−52+4465−4u+6v+2w+2226/5log26/586/5+6x+8u+126/5+9x+12v+46/5+3x+4w+9x2+3x−52+446/5.


## 3.1.1. Randic´ Entropy of C1u,v,w,x

We enumerate the Randic´ index for α=1,−1,1/2,−1/2 with the help of Tables 1 and 2 as follows:(2)RαC1u,v,w,x=6×4α+4u+6v+2w+22×6α+6x+8u+9x+12v+3x+4w+9x2+3x−58×9α.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(3)ENTRαC1u,v,w,x=logRα−1Rα∑i=13∑az∈DEi§^a×§^zαlog§^a×§^zα,ENTRαC1u,v,w,x=logRα−6Rα4αlog4α−4u+6v+2w+22Rα6αlog6α−6x+8u+9x+12v+3x+4w+9x2+3x−58Rα9αlog9α,ENTR1C1u,v,w,x=log96+54xu+144+81xv+48+27xw+81x2+27x−366−24log496+54xu+144+81xv+48+27xw+81x2+27x−366−64u+6v+2w+22log696+54xu+144+81xv+48+27xw+81x2+27x−366−96x+8u+9x+12v+3x+4w+x2+3x−58log996+54xu+144+81xv+48+27xw+81x2+27x−366,ENTR1/2C1u,v,w,x=log46+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−12log246+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−64u+6v+2w+22log646+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162−36x+8u+9x+12v+3x+4w+x2+3x−58log346+18x+24u+66+27x+36v+26+9x+12w+27x2+9x+226−162,ENTR−1C1u,v,w,x=log149+2x3u+73+xv+79+x3w+x2+x3−2318+3/2log414/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18+1/64u+6v+2w+22log614/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18+1/96x+8u+9x+12v+3x+4w+x2+3x−58log914/9+2x/3u+7/3+xv+7/9+x/3w+x2+x/3−23/18,ENTR−1/2C1u,v,w,x=log46+2x+83u+6+3x+4v+26+x+43w+3x2+x+226−493+3/2log24/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3+1/64u+6v+2w+22log64/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3+1/36x+8u+9x+12v+3x+4w+x2+3x−58log34/6+2x+8/3u+6+3x+4v+2/6+x+4/3w+3x2+x+22/6−49/3.


## 3.1.2. The Atom Bond Connectivity Entropy ofC1u,v,w,x

Simple calculations with Tables1 and 2 yield the atom bond connectivity index as follows:(4)ABCC1u,v,w,x=22+4x+163u+32+6x+8v+2+2x+83w+6x2+2x+142−1163.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(5)ENTABCC1u,v,w,x=logABC−1ABC∑i=13∑az∈DEi§^a+§^z−2§^a×§^zlog§^a+§^z−2§^a×§^z,ENTABCC1u,v,w,x=log22+4x+163u+32+6x+8v+2+2x+83w+6x2+2x+142−1163−61/2log1/222+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3−4u+6v+2w+221/2log1/222+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3−6x+8u+9x+12v+3x+4w+x2+3x−582/3log2/322+4x+16/3u+32+6x+8v+2+2x+8/3w+6x2+2x+142−116/3.


## 3.1.3. The Geometric Arithmetic EntropyC1u,v,w,x

Simple calculations with Tables1 and 2 yield the geometric arithmetic index as follows:(6)GAG=865+6x+8u+1265+9x+12v+465+3x+4w+9x2+3x−52+4465.Therefore, equation (1) with Tables 1 and 2 is in the form as follows:(7)ENTGAC1u,v,w,x=logGA−1GA∑i=13∑az∈DEi2§^a×§^z§^a+§^zlog2§^a×§^z§^a+§^z,ENTGAC1u,v,w,x=log865+6x+8u+1265+9x+12v+465+3x+4w+9x2+3x−52+4465−4u+6v+2w+2226/5log26/586/5+6x+8u+126/5+9x+12v+46/5+3x+4w+9x2+3x−52+446/5.


## 4. Coronoid SystemC1u,v,w,x

The coronoid system ofD is delineated as C2n,p,q,r, in which x≥1, u≥3, and 1≤v<w≤u. Figure 3 shows the coronoid system of C2u,v,w,x [34, 35].Figure 3
Coronoid system ofC2u,v,w,x [35].The approach we will use here is to form the partitions of the edges ofC2u,v,w,x of terminal vertices of each edge (see Table 3).Table 3
Edge partition ofC2u,v,w,x established on degrees of terminal vertices of each edge.
§^a,§^zNumber of replicationClasses of edges2,26GE12,34u+4v+4w+24GE23,36u+6v+6wx+9x2−9x−40GE3


### 4.1. Results for Coronoid SystemC2u,v,w,x

#### 4.1.1. Randic´ Entropy of C2u,v,w,x

We enumerate the Randic´ index for α=1,−1,1/2,−1/2 with the help of Tables 3 and 1 as follows:(8)RαC2u,v,w,x=6×4α+4u+4v+4w+24×6α+6u+6v+6wx+9x2−9x−40×9α.As a consequence, equation (1) with Tables 1 and 3 is embodied in the form as follows:(9)ENTRαC2u,v,w,x=logRα−1Rα∑i=13∑az∈DEi§^a×§^zαlog§^a×§^zα,ENTR1C2u,v,w,x=log24+54xu+v+w+81x2−81x−192−24log424+54xu+v+w+81x2−81x−192−64u+4v+4w+24log624+54xu+v+w+81x2−81x−192−96u+6v+6wr+9x2−9x−40log924+54xu+v+w+81x2−81x−192,ENTR−1C2u,v,w,x=log231+xu+v+wx2−x+1918+3/2log42/31+xu+v+wx2−x+19/18+1/64u+4v+4w+24log62/31+xu+v+wx2−x+19/18+1/96u+6v+6wx+9x2−9x−40log92/31+xu+v+wx2−x+19/18,ENTR1/2K2n,p,q,r=log46+18n+p+q+27r2−27r+246−108−12log246+18n+p+q+27r2−27r+246−108−64u+4v+4w+24log646+18n+p+q+27r2−27r+246−108−36u+6v+6wx+9x2−9x−40log346+18n+p+q+27r2−27r+246−108,ENTR−1/2C2u,v,w,x=log46+2xu+v+w+3x2−3x+46−313+3/2log24/6+2xu+v+w+3x2−3x+46−31/3+64u+4v+4w+24log64/6+2xu+v+w+3x2−3x+46−31/3+1/36u+6v+6wx+9x2−9x−40log34/6+2xu+v+w+3x2−3x+46−31/3.


#### 4.1.2. The Atom Bond Connectivity Entropy ofC2u,v,w,x

Simple calculations with Tables1 and 3 yield the atom bond connectivity index as follows:(10)ABCC2u,v,w,x=22+4xu+v+w+6x2−6x+52−803.Therefore, equation (1) with Tables 1 and 3 is in the form as follows:(11)ENTABCC2u,v,w,x=logABC−1ABC∑i=13∑az∈DEi§^a+§^z−2§^a×§^zlog§^a+§^z−2§^a×§^z,ENTABCC2u,v,w,x=logABC−6/2ABClog12−4u+4v+4w+24ABC12log12−6u+6v+6wx+9x2−9x−40ABC23log23.


#### 4.1.3. The Geometric Arithmetic Entropy ofC2u,v,w,x

Simple calculations with Tables1 and 3 yield the geometric arithmetic index as follows:(12)GAG=865+6xu+v+w+9x2−9x−34+4865.Therefore, equation (1) with Tables 1 and 3 is in the form as follows:(13)ENTGAC2u,v,w,x=logGA−1GA∑i=13∑az∈DEi2§^a×§^z§^a+§^zlog2§^a×§^z§^a+§^z,ENTGAC2u,v,w,x=log865+6xu+v+w+9x2−9x−34+4865−4u+4v+4w+2426/5log26/586/5+6xu+v+w+9x2−9x−34+486/5.


## 4.1. Results for Coronoid SystemC2u,v,w,x

### 4.1.1. Randic´ Entropy of C2u,v,w,x

We enumerate the Randic´ index for α=1,−1,1/2,−1/2 with the help of Tables 3 and 1 as follows:(8)RαC2u,v,w,x=6×4α+4u+4v+4w+24×6α+6u+6v+6wx+9x2−9x−40×9α.As a consequence, equation (1) with Tables 1 and 3 is embodied in the form as follows:(9)ENTRαC2u,v,w,x=logRα−1Rα∑i=13∑az∈DEi§^a×§^zαlog§^a×§^zα,ENTR1C2u,v,w,x=log24+54xu+v+w+81x2−81x−192−24log424+54xu+v+w+81x2−81x−192−64u+4v+4w+24log624+54xu+v+w+81x2−81x−192−96u+6v+6wr+9x2−9x−40log924+54xu+v+w+81x2−81x−192,ENTR−1C2u,v,w,x=log231+xu+v+wx2−x+1918+3/2log42/31+xu+v+wx2−x+19/18+1/64u+4v+4w+24log62/31+xu+v+wx2−x+19/18+1/96u+6v+6wx+9x2−9x−40log92/31+xu+v+wx2−x+19/18,ENTR1/2K2n,p,q,r=log46+18n+p+q+27r2−27r+246−108−12log246+18n+p+q+27r2−27r+246−108−64u+4v+4w+24log646+18n+p+q+27r2−27r+246−108−36u+6v+6wx+9x2−9x−40log346+18n+p+q+27r2−27r+246−108,ENTR−1/2C2u,v,w,x=log46+2xu+v+w+3x2−3x+46−313+3/2log24/6+2xu+v+w+3x2−3x+46−31/3+64u+4v+4w+24log64/6+2xu+v+w+3x2−3x+46−31/3+1/36u+6v+6wx+9x2−9x−40log34/6+2xu+v+w+3x2−3x+46−31/3.


### 4.1.2. The Atom Bond Connectivity Entropy ofC2u,v,w,x

Simple calculations with Tables1 and 3 yield the atom bond connectivity index as follows:(10)ABCC2u,v,w,x=22+4xu+v+w+6x2−6x+52−803.Therefore, equation (1) with Tables 1 and 3 is in the form as follows:(11)ENTABCC2u,v,w,x=logABC−1ABC∑i=13∑az∈DEi§^a+§^z−2§^a×§^zlog§^a+§^z−2§^a×§^z,ENTABCC2u,v,w,x=logABC−6/2ABClog12−4u+4v+4w+24ABC12log12−6u+6v+6wx+9x2−9x−40ABC23log23.


### 4.1.3. The Geometric Arithmetic Entropy ofC2u,v,w,x

Simple calculations with Tables1 and 3 yield the geometric arithmetic index as follows:(12)GAG=865+6xu+v+w+9x2−9x−34+4865.Therefore, equation (1) with Tables 1 and 3 is in the form as follows:(13)ENTGAC2u,v,w,x=logGA−1GA∑i=13∑az∈DEi2§^a×§^z§^a+§^zlog2§^a×§^z§^a+§^z,ENTGAC2u,v,w,x=log865+6xu+v+w+9x2−9x−34+4865−4u+4v+4w+2426/5log26/586/5+6xu+v+w+9x2−9x−34+486/5.


## 4.1.1. Randic´ Entropy of C2u,v,w,x

We enumerate the Randic´ index for α=1,−1,1/2,−1/2 with the help of Tables 3 and 1 as follows:(8)RαC2u,v,w,x=6×4α+4u+4v+4w+24×6α+6u+6v+6wx+9x2−9x−40×9α.As a consequence, equation (1) with Tables 1 and 3 is embodied in the form as follows:(9)ENTRαC2u,v,w,x=logRα−1Rα∑i=13∑az∈DEi§^a×§^zαlog§^a×§^zα,ENTR1C2u,v,w,x=log24+54xu+v+w+81x2−81x−192−24log424+54xu+v+w+81x2−81x−192−64u+4v+4w+24log624+54xu+v+w+81x2−81x−192−96u+6v+6wr+9x2−9x−40log924+54xu+v+w+81x2−81x−192,ENTR−1C2u,v,w,x=log231+xu+v+wx2−x+1918+3/2log42/31+xu+v+wx2−x+19/18+1/64u+4v+4w+24log62/31+xu+v+wx2−x+19/18+1/96u+6v+6wx+9x2−9x−40log92/31+xu+v+wx2−x+19/18,ENTR1/2K2n,p,q,r=log46+18n+p+q+27r2−27r+246−108−12log246+18n+p+q+27r2−27r+246−108−64u+4v+4w+24log646+18n+p+q+27r2−27r+246−108−36u+6v+6wx+9x2−9x−40log346+18n+p+q+27r2−27r+246−108,ENTR−1/2C2u,v,w,x=log46+2xu+v+w+3x2−3x+46−313+3/2log24/6+2xu+v+w+3x2−3x+46−31/3+64u+4v+4w+24log64/6+2xu+v+w+3x2−3x+46−31/3+1/36u+6v+6wx+9x2−9x−40log34/6+2xu+v+w+3x2−3x+46−31/3.


## 4.1.2. The Atom Bond Connectivity Entropy ofC2u,v,w,x

Simple calculations with Tables1 and 3 yield the atom bond connectivity index as follows:(10)ABCC2u,v,w,x=22+4xu+v+w+6x2−6x+52−803.Therefore, equation (1) with Tables 1 and 3 is in the form as follows:(11)ENTABCC2u,v,w,x=logABC−1ABC∑i=13∑az∈DEi§^a+§^z−2§^a×§^zlog§^a+§^z−2§^a×§^z,ENTABCC2u,v,w,x=logABC−6/2ABClog12−4u+4v+4w+24ABC12log12−6u+6v+6wx+9x2−9x−40ABC23log23.


## 4.1.3. The Geometric Arithmetic Entropy ofC2u,v,w,x

Simple calculations with Tables1 and 3 yield the geometric arithmetic index as follows:(12)GAG=865+6xu+v+w+9x2−9x−34+4865.Therefore, equation (1) with Tables 1 and 3 is in the form as follows:(13)ENTGAC2u,v,w,x=logGA−1GA∑i=13∑az∈DEi2§^a×§^z§^a+§^zlog2§^a×§^z§^a+§^z,ENTGAC2u,v,w,x=log865+6xu+v+w+9x2−9x−34+4865−4u+4v+4w+2426/5log26/586/5+6xu+v+w+9x2−9x−34+486/5.


## 5. Comparisons and Discussion forC1u,v,w,x

In QSPR/QSAR discussions, topological indices are applied to connect the biological functions of the anatomies with their corporeal properties like distortion, strain energy, stability, and melting point. These determinations can be accomplished by employing degree-based indices as these indices have clarity of decision and rapidity. In this research, we asseverated some degree-based entropies. We proposed a new approach to estimate the entropy by estimating its topological indices. The degree-based entropy can also be exerted to structural chemistry, ecological networks, biology, national security, social network, and so on. Additionally, to investigate structural symmetry and asymmetry in real networks, the values of entropies have a significant role. Entropy is monotonically increasing function as in all situations. Here, we estimated mathematically all degree-based entropies for diverse values ofuandx keeping p=1 and q=1 for C1u,v,w,x. Besides, we construct Tables 4 and 5 for tiny values of u,x, p=1 and q=1 for degree-based entropy to numerical comparison for the structure of C1u,v,w,x. Now, numerical comparison is represented in Tables 4 and 5. Also, the graphical comparison is depicted in Figures 4–6.Table 4
Comparison of Randic entropies forC1u,1,1,x.
u,xENTR1ENTR−1ENTR1/2ENTR−1/23,10.11321.84451.85421.85404,20.99642.18012.19062.09105,31.37322.42132.42962.28416,41.62022.60942.61572.45607,51.80652.76342.76842.62198,61.95712.89392.89802.75119,72.08393.00723.03052.870910,82.19383.10723.17013.013411,92.29073.19693.27933.125312,102.37763.27813.38023.2018Table 5
Comparison ofENTABC and ENTGA entropies for C1u,v,w,x.
u,sENTABCENTGA3,11.85721.83604,22.2032.28015,32.44122.52206,42.62692.70977,52.78932.88348,62.89872.99989,73.01113.096710,83.08063.166711,93.16973.256312,103.26053.3574Figure 4
Comparison of Randic entropies forα=1 and for α=−1.Figure 5
Comparison of Randic entropies forα=1/2 and for α=−1/2.Figure 6
Comparison of atom bond connectivity entropy and geometric arithmetic entropy.


## 6. Comparisons and Discussion forC2u,v,w,x

Multiple exploitations of complex networks deserted on the entropy corresponding with structural information are discussed. In [36–39], many methods were suggested to check the structural complexity. However, the entropy approach is considered to be the most significant approach to discriminate the structural information of the complex networks. Besides, degree-based indices have theoretical role on account of having the capability of computing pharmaceutical properties. Therefore, we have listed mathematically some degree-based entropies for little considerations of parameters uandx keeping v=1 and w=2 for C2u,v,w,x as depicted in Tables 6 and 7. Also, the graphical comparison is depicted in Figures 7–9.Table 6
Comparison of Randic entropies forC2u,v,w,x.
u,xENTR1ENTR−1ENTR1/2ENTR−1/23,11.83781.83801.84332.46694,22.17152.26892.17912.51815,32.41432.52082.41952.63596,42.60322.74012.70702.75947,52.75792.91522.76082.87548,62.88903.01232.89122.98149,73.00263.13073.00453.07810,83.10303.21143.10463.166111,93.19303.29153.19433.246912,103.27443.37323.27563.3213Table 7
Comparison ofENTABC and ENTGA entropies for C2u,v,w,x.
u,xENTABCENTGA3,11.75961.84514,22.09442.18185,32.34022.42166,42.53472.60857,52.71222.78198,62.82492.89219,72.94973.005210,83.05833.100811,93.15123.191212,103.25313.2731Figure 7
Comparison of Randic entropies forα=1 and for α=−1 for the coronoid system C2u,v,w,x.Figure 8
Comparison of Randic entropies forα=1/2 and for α=−1/2 for the coronoid system C2u,v,w,x.Figure 9
Comparison of Randic entropies forα=1/2 and for α=−1/2 for the coronoid system C2u,v,w,x.


## 7. Conclusion

In this research, we have appropriated some degree-based indices for the characterization of the unambiguous graph-theoretical system of biochemical concern. We talked about topological indices, for instance, general Randic´ index, atomic bond connectivity index, and geometric arithmetic index for coronoid polycyclic aromatic hydrocarbons. Besides, we enumerated the corresponding entropies. The enumerated results link individual physico-chemical characteristics like distortion, stability, melting points, and strain energy of chemical compounds. The mathematical findings for these coronoid systems are helpful for the chemist to understand the biochemical applications of these coronoid systems C1u,v,w,x and C2u,v,w,x.



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*Source: 4646501-2021-10-18.xml*