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Correlation of domination parameters with physicochemical properties of octane isomers


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Introduction

Let G = (V,E) be a graph. The number of vertices of G we denote by n and the number of edges we denote by m, thus |V(G)| = n and |E(G)| = m. For undefined terminologies, we refer the reader to [7].

Chemical graph theory is the branch of mathematical chemistry. It is concerned with handling chemical graphs that represent chemical system. Hence chemical graph theory deals with analysis of all consequences of connectivity in a chemical system. It has found to be a useful tool in QSAR (Quantitative Structure-Activity Relationships) and QSPR (Quantitative Structure-Property Relationship) [4,10,16]. Numerous studies have been made relating to the above mentioned fields by using what are called topological indices.In 1975, Randić [13] proposed a topological index that has become one of the most widely used in both QSAR and QSPR studies.

One of the fastest growing areas in graph theory is the study of domination and related subset problems such as independence, irredundance, covering and matching. An excellent treatment of fundamentals of domination in graphs is given by the book by Haynes et. al [5]. Surveys of several advances topics in domination are given in the book edited by Haynes et. al [6].

Let G = (V,E) be a graph. A subset S of V is called a dominating set of G if every vertex in VS is adjacent to at least one vertex in S. The domination number γ(G) of a graph G is the minimum cardinality of a dominating set of G.

Sampathkumar and Walikar [15] have introduced an important domination invariant called connected domination number, which is defined as follows. Let G = (V,E) be a graph. A subset S of V is called a connected dominating set of G if every vertex in VS is adjacent to at least one vertex in S and the subgraph induced by the set S is connected. The connected domination number γc(G) of a graph G is the minimum cardinality of a connected dominating set of G.

E. J. Cockayne et. al [3] have introduced the concept of total domination as follows. Let G = (V,E) be a graph. A subset S of V is called a total dominating set of G if every vertex G is adjacent some vertex in S. The total domination number γt(G) of a graph G is the minimum cardinality of a total dominating set of G.

The total edge domination is an analogues concept total domination, which is introduced and studied in [9]. For more details on domination see [1, 2].

Octane isomers

Octane isomers have become an important set of organic molecules to test the applicability of various topological parameters in quantitative structure-property/activity relationships (QSPR/QSAR). These compounds are structurally diverse enough to yield considerable variation in shape, branching and non polarity [14]. In a comprehensive study of numerous properties of octane isomers, Randić et. al [10,12,14] have used single molecular descriptors and concluded that different physicochemical properties depend on different descriptors.

So far in the literature of chemical graph theory, domination parameters have not been used to predict the physical properties of chemical compounds. Therefore, in the present study an attempt has been made to study physical properties of octane isomers by using domination parameters.

The values of γc, γt and γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$ of molecular graph of 2,2,3,3−tetramethyl butane are illustrated below.

From Fig. 1, it is clear that the minimal connected dominating set Dc = {2,5}, the total dominating set Dt = {2,5}, and the total edge dominating set Dt={2,5,7}$\begin{array}{} \displaystyle D_t^\prime = \left\{ {2,5,7} \right\} \end{array}$. Hence, γc(G) = |Dc| = 2, γt(G) = |Dt| = 2, and γt(G)=|Dt|=3$\begin{array}{} \displaystyle \gamma _t^\prime \left( G \right) = \left| {D_t^\prime } \right| = 3 \end{array}$.

Fig. 1

2,2,3,3−tetramethylbutane and its molecular graph.

Data based and analytical method

Eight physicochemical properties of octane isomers have been selected on the availability [8] of a suitable body of data: boiling point (BP), critical temperature (CT), critical pressure (CP), entropy (S), density (D), mean radius (Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$), and heat of vaporization (Hν), heat of formation (Hf). The values are compiled in Table 1.

Domination parameters and physicochemical properties of octane isomers.

Alkaneγcγtγt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$BPTCPCSDRm2$\begin{array}{} \displaystyle R_m^2 \end{array}$−ΔHf−ΔHν
n−octane654125.70296.2024.64111.670.70252.0449208.641.49
2M544117.6288.024.80109.840.69801.8913215.439.67
3M544118.9292.025.60111.260.70581.7984212.539.83
4M554117.7290.025.60109.320.70461.7673210.739.64
3E554118.5292.025.74109.430.71361.7673210.739.64
22MM443106.8279.025.60103.420.69531.6744224.637.28
23MM443115.6293.026.60108.020.71211.6464213.838.78
24MM443109.4282.025.80106.980.70041.6142219.237.76
25MM443109.1279.025.00105.720.69351.6449222.537.85
33MM443112.0290.827.20104.740.71001.7377220.037.53
34MM443117.7298.027.40106.590.72001.5230212.838.97
2M3E443115.6295.027.40106.060.71931.5525211.038.52
3M3E443118.3305.028.90101.480.72741.5212214.837.99
223MMM332109.8294.028.20101.310.71611.4306220.036.91
224MMM33299.24271.125.50104.090.69191.4010224.035.14
233MM332114.8303.029.00102.060.72621.4931216.337.27
234MMM332113.5295.027.60102.390.71911.3698217.337.75
2233MMMM222106.5270.824.5093.060.82421.4612225.642.90

Next, we obtain a cross-correlation matrix of domination parameters, which is shown in Table 2.

Cross correlation matrix of domination parameters.

 γcγtγt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$
γc1.000  
γt0.9261.000 
γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$0.9490.8781.000

Table 3 contains the correlation of domination parameters with physicochemical properties of octane isomers.

Correlation of Domination parameters with physicochemical properties of octane isomers.

 BPTCPCSDRm2$\begin{array}{} \displaystyle R_m^2 \end{array}$ΔHfΔHν
γc0.7300.316-0.3490.902-0.5790.9030.7160.305
γt0.6440.334-0.2160.840-0.5990.7660.6820.159
γt0.6830.196-0.4490.825-0.4150.8950.6530.446

Results and Discussion

From Table 2, it is found that the cross correlation coefficient of domination parameters are found to be high (0.878 − 0.949). Also from Table 3, the correlation coefficient of domination parameters with physico-chemical properties of isomers are found to be good except critical pressure (CP) and density (D). For these two physicochemical properties of octane isomers the domination parameters are not well-correlated.

A generalized linear regression model has been proposed for the relationship of physicochemical properties of octane isomers with the domination parameters γc, γt, and γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$, respectively.

P=a+i=13biγi,$$\begin{array}{} \displaystyle P = a + \sum\limits_{i = 1}^3 {{b_i}} {\gamma _i}, \end{array}$$

where P refers to a physicochemical property, a is constant, and bi is the sensitivity of γi towards P. For our convince, we assume that γ1 = γc, γ2 = γt, and γ3=γt$\begin{array}{} \displaystyle {\gamma _3} = \gamma _t^\prime \end{array}$.

We first consider the regression model containing single descriptors connected domination number γc, total domination number γt and total edge domination γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$ separately.

P =a+bγc.$$\begin{array}{} \displaystyle P{\rm{ }} = a + b{\gamma _c}. \end{array}$$

P =a+bγt.$$\begin{array}{} \displaystyle P{\rm{ }} = a + b{\gamma _t}. \end{array}$$

P =a+bγt.$$\begin{array}{} \displaystyle P{\rm{\;}} = a + b\gamma _t^\prime . \end{array}$$

In Tables 4, 5, and 6, statistical parameters for the linear QSPR models in Eqs. (2)-(4) are given.

Statistical parameters for the linear QSPR model (2).

Physical propertyRSF
BP0.7304.309718.307
TC0.3169.61821.778
PC0.3491.38822.223
S0.9022.00870.017
D0.5790.02478.063
γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$0.9030.080070.944
−ΔHf0.7163.736016.826
ΔHν0.3051.74631.638

Statistical parameters for the linear QSPR model (3).

Physical propertyRSF
BP0.6444.827411.343
TC0.3349.55472.015
PC0.2161.44670.780
S0.8402.527738.299
D0.5990.02428.973
Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$0.7660.120022.696
−ΔHf0.6823.915113.891
ΔHν0.1591.18020.415

Statistical parameters for the linear QSPR model (4).

Physical propertyRSF
BP0.6834.606514.028
TC0.1969.94240.637
PC0.4491.32364.046
S0.8252.629734.168
D0.4150.02753.320
Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$0.8950.083164.657
−ΔHf0.6534.052911.893
ΔHν0.4461.64083.979

Next, we consider the multiple regression model containing two descriptors of the combination of connected domination number γc, total domination number γt, and total edge domination γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$, separately.

P=a+i=12biγi.$$\begin{array}{} \displaystyle P = a + \sum\limits_{i = 1}^2 {{b_i}} {\gamma _i}. \end{array}$$

In Table 7, statistical parameters for the regression model containing two descriptors γc and γt are provided. Table 8 collects the statistical parameters for the regression model containing two descriptors γc and γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$. In Table 9, statistical parameters for the regression model containing two descriptors γt and γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$ appear.

Statistical parameters for the QSPR model (5).

Physical propertyRSF
BP0.7354.41628.836
TC0.3359.86630.947
PC0.4511.36571.914
S0.9022.073432.852
D0.6030.02494.280
Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$0.9220.074442.743
−ΔHf0.7183.84867.966
ΔHν0.4461.69471.864

Statistical parameters for the QSPR model (5).

Physical propertyRSF
BP0.7314.44678.613
TC0.4579.31401.979
PC0.5111.31532.650
S0.9072.021134.964
D0.7190.02178.007
Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$0.9110.079336.801
−ΔHf0.7213.83128.107
ΔHν0.5831.53853.861

Statistical parameters for the QSPR model (5).

Physical propertyRSF
BP0.6904.72016.800
TC0.3929.63161.364
PC0.5851.24113.900
S0.8602.457321.228
D0.6440.02395.302
Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$0.8960.085430.663
−ΔHf0.6913.99466.856
ΔHν0.6611.42135.812

Finally, we consider the multiple regression model containing three descriptors, connected domination number γc, total domination number γt, and total edge domination γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$.

P=a+i=13biγi.$$\begin{array}{} \displaystyle P = a + \sum\limits_{i = 1}^3 {{b_i}} {\gamma _i}. \end{array}$$

In Table 10, statistical parameters for the regression model containing three descriptors γc, γt, and γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$ are shown.

Statistical parameters for the QSPR model (6).

Physical propertyRSF
BP0.7364.56665.518
TC0.4709.56661.323
PC0.5851.28442.430
S0.9072.091221.777
D0.7380.02185.580
Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$0.9300.073130.018
−ΔHf0.7223.95545.095
ΔHν0.6681.45893.757

The correlation coefficients of physicochemical properties with individual γi values show some significant results. The entropy and the mean radius values, which generally do not show good relationships with any single descriptor, are found to have a good correlation coefficient (0.825 − 0.902) and (0.766 − 0.903), respectively. The critical temperature,pressure, density, and enthalpy of vaporization values are found to have poor correlation coefficient (−0.599 − 0.446).

The regression analysis of models (2)-(4) with single descriptors, reveals some interesting results for mean radius Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$ and entropy S.

From Table 4, we can see that for entropy S, R = 0.902 (standard error of 2.008°C) and F = 70.017, and for mean radius Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$, R = 0.903 (standard error of 0.0800°C) and F = 70.944.

From Table 5, we can see that for entropy S, R = 0.840 (standard error of 2.5277°C) and F = 38.299, and for mean radius Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$, R = 0.766 (standard error of 0.1200°C) and F = 22.696.

From Table 6, we can see that for entropy S, R = 0.825 (standard error of 2.6297°C) and F = 34.168, and for mean radius Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$, R = 0.895 (standard error of 0.0831°C) and F = 64.657.

The use of two descriptors, the combination of γc, γt, and γt$\begin{array}{} \displaystyle \gamma _t^\prime \end{array}$ gave a good correlation coefficients for entropy ranging from R = (0.860 − 0.907) having standard error ranging from (2.0211 − 2.4573) and F = (21.228 − 34.964). For mean radius Rm2$\begin{array}{} \displaystyle R_m^2 \end{array}$, R = (0.896 − 0.922) having standard error ranging from (0.0744 − 0.0854) and F = (30.663 − 42.743).

However, the addition of third descriptor does not produce any significant improvement in the regression model. Hence, for other physical properties of the octane isomers, the relationship with domination parameters can be seen in Tables 4-10.

Conclusions

The results of QSPR studies reveals that the regression model (2) is the most significant model to predict the physicochemical properties like entropy and mean radius of isomers. Hence, domination parameters be used as candidate to represent the molecular structure for predicting physicochemical properties.

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