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ISSN 2229 – 5046

HYPER-WIENER INDEX USING DEGREE SEQUENCE

SHIGEHALLI V. S.

1

, SHANMUKH KUCHABAL*

2

1

Professor, Department of Mathematics,

Rani Channamma University, Vidya Sangama, Belagavi- 591 156, India.

2

Research Scholar, Department of Mathematics,

Rani Channamma University, Vidya Sangama, Belagavi- 591 156, India.

(Received On: 15-10-15; Revised & Accepted On: 07-11-15)

ABSTRACT

L

et G be the connected graph. The Wiener index 𝑊𝑊(𝐺𝐺) is the sum of all distances between vertices of G, whereas the hyper-Wiener index 𝑊𝑊𝑊𝑊(𝐺𝐺) is defined as 𝑊𝑊𝑊𝑊(𝐺𝐺) =𝑊𝑊(𝐺𝐺) +1

2∑{𝑢𝑢,𝑣𝑣}⊆𝑉𝑉{𝐺𝐺}𝑑𝑑(𝑢𝑢,𝑣𝑣)2. In this paper we prove some

general results on the hyper-Wiener index of graphs using degree sequence.

Keywords: molecular graphs and hyper-Wiener index.

2000 Mathematics subject classification: 05C12, 92E10.

1. INTRODUCTION

In mathematical terms a graph is represented as 𝐺𝐺= (𝑉𝑉,𝐸𝐸) where 𝑉𝑉 is the set of vertices and 𝐸𝐸 is the set of edges. Let

𝐺𝐺 be an undirected connected graph without loops or multiple edges with 𝑛𝑛 vertices, denoted by 1,2, … ,𝑛𝑛. The

topological distance between the vertices 𝑢𝑢 and 𝑣𝑣 of 𝑉𝑉(𝐺𝐺) is denoted by 𝑑𝑑(𝑢𝑢,𝑣𝑣) or 𝑑𝑑𝑢𝑢𝑣𝑣 and it is defined as the number

of edges in a minimal path connecting the vertices 𝑢𝑢 and 𝑣𝑣.

The Wiener index 𝑊𝑊(𝐺𝐺) of a connected graph 𝐺𝐺 is defined as the sum the distances between all unordered pairs of

vertices of 𝐺𝐺. It was put forward by Harold Wiener [5]. The Wiener index is a graph invariant intensively studied both

in mathematics and chemical literature, see for details[5−10].

The hyper-Wiener index was proposed by Randic [6] for a tree and extended by Klein et al.[1] to a connected graph. It

is used to predict physicochemical properties of organic compounds. The hyper-Wiener index defined as,

𝑊𝑊𝑊𝑊(𝐺𝐺) = � �𝑑𝑑𝑢𝑢𝑣𝑣+ 1

2 �

{𝑢𝑢,𝑣𝑣}⊆𝑉𝑉(𝐺𝐺)

=𝑊𝑊(𝐺𝐺) +12 � 𝑑𝑑(𝑢𝑢,𝑣𝑣)2 {𝑢𝑢,𝑣𝑣}⊆𝑉𝑉(𝐺𝐺)

The hyper-Wiener index is studied both from a theoretical point of view and applications. We encourage the reader to

consult [4, 5, 10 𝑎𝑎𝑛𝑛𝑑𝑑 12−15] for further readings. The hyper-Wiener index of complete graph-𝐾𝐾𝑝𝑝, path graph-𝑃𝑃𝑛𝑛, star

graph-𝐾𝐾1,(𝑛𝑛−1) and cycle graph 𝐶𝐶𝑛𝑛 is given by the expressions

𝑊𝑊𝑊𝑊(𝐾𝐾𝑛𝑛) =𝑛𝑛(𝑛𝑛 −2 1),𝑊𝑊𝑊𝑊(𝑃𝑃𝑛𝑛) =𝑛𝑛

4+ 2𝑛𝑛3− 𝑛𝑛22𝑛𝑛

24 , 𝑊𝑊𝑊𝑊�𝐾𝐾1,(𝑛𝑛−1)�= 1

2(𝑛𝑛 −1)(3𝑛𝑛 −4) And

𝑊𝑊𝑊𝑊(𝐶𝐶𝑛𝑛) =

𝑛𝑛2(𝑛𝑛+ 1)(𝑛𝑛+ 2)

48 , 𝑖𝑖𝑖𝑖𝑛𝑛𝑖𝑖𝑖𝑖𝑒𝑒𝑣𝑣𝑒𝑒𝑛𝑛

𝑛𝑛(𝑛𝑛21)(𝑛𝑛+ 3)

48 , 𝑖𝑖𝑖𝑖𝑛𝑛𝑖𝑖𝑖𝑖𝑜𝑜𝑑𝑑𝑑𝑑

Corresponding Author: Shanmukh Kuchabal*

2

2

Research Scholar, Department of Mathematics,

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For example: Consider a graph G with vertices 𝑣𝑣1,𝑣𝑣2,𝑣𝑣3 and 𝑣𝑣4 as labeled in the figure below.

Here 𝑑𝑑(𝑣𝑣1,𝑣𝑣2) = 1,𝑑𝑑(𝑣𝑣1,𝑣𝑣3) = 2,𝑑𝑑(𝑣𝑣1,𝑣𝑣4) = 2,𝑑𝑑(𝑣𝑣2,𝑣𝑣3) = 1,𝑑𝑑(𝑣𝑣2,𝑣𝑣4) = 1,𝑑𝑑(𝑣𝑣3,𝑣𝑣4) = 1.

Therefore 𝑊𝑊𝑊𝑊(𝐺𝐺) =∑ �𝑑𝑑𝑢𝑢𝑣𝑣+ 1

2 �

{𝑢𝑢,𝑣𝑣}⊆𝑉𝑉(𝐺𝐺)

=2 × 12 +3 × 22 +3 × 22 +2 × 12 +2 × 12 +2 × 12

= 1 + 3 + 3 + 1 + 1 + 1

= 10

2. EXISTING RESULTS

Theorem 2.1: [4,6] If 𝐺𝐺(𝑝𝑝,𝑞𝑞) is a is a graph, with ∆(𝐺𝐺) =𝑝𝑝 −1 then 𝑊𝑊(𝐺𝐺) =𝑝𝑝2− 𝑝𝑝 − 𝑞𝑞.

Theorem 2.2: [6] If 𝐺𝐺(𝑝𝑝,𝑞𝑞) is a connected graph then the Wiener Index of 𝐺𝐺+𝑥𝑥 is 𝑝𝑝2− 𝑝𝑝.

Theorem 2.3: [6] If 𝐺𝐺(𝑝𝑝,𝑞𝑞) be a graph and 𝑥𝑥 is any vertex in 𝐺𝐺 of degree 𝑝𝑝 −1 such that the graph 𝐺𝐺 − 𝑥𝑥 is connected

then Wiener index of 𝐺𝐺 − 𝑥𝑥 is (𝑝𝑝 −1)2− 𝑞𝑞

Theorem 2.4: [6] If 𝐺𝐺1(𝑝𝑝1,𝑞𝑞1) and 𝐺𝐺2(𝑝𝑝2,𝑞𝑞2) are two connected graphs then the Wiener index of 𝐺𝐺1+𝐺𝐺2 is

𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =𝑝𝑝1(𝑝𝑝1−1) +𝑝𝑝2(𝑝𝑝2−1) +𝑝𝑝1𝑝𝑝2− 𝑞𝑞1𝑞𝑞2.

Theorem 2.5: [6] The Wiener index of 𝑊𝑊(𝐺𝐺1) = 𝑚𝑚(𝑚𝑚 −1) +𝑝𝑝(𝑝𝑝 −1) +𝑚𝑚𝑝𝑝 − 𝑞𝑞.

3. MAIN RESULTS

3.1 Bounds for the hyper-Wiener index in terms of Order, Size and Maximum Degree:

Lemma 3.1.1: Let G be the graph with n vertices m edges, then 𝑊𝑊𝑊𝑊(𝐺𝐺)≥3𝑛𝑛2−3𝑛𝑛−4𝑚𝑚

2 .

Proof: Len 𝑛𝑛𝑖𝑖 be any vertex of G. Then,

𝑑𝑑(𝑛𝑛𝑖𝑖|𝐺𝐺)≥deg(𝑣𝑣𝑖𝑖) + 2{𝑛𝑛 −1−deg(𝑣𝑣𝑖𝑖)} = 2𝑛𝑛 −2−deg(𝑣𝑣𝑖𝑖)

𝑑𝑑(𝑛𝑛𝑖𝑖|𝐺𝐺)2{𝑑𝑑(𝑛𝑛𝑖𝑖|𝐺𝐺) + 1} ×𝑑𝑑(𝑛𝑛𝑖𝑖|𝐺𝐺)

2

= 2𝑛𝑛 −2−deg(𝑣𝑣𝑖𝑖) +𝑛𝑛 −1−deg(𝑣𝑣𝑖𝑖)

= 3𝑛𝑛 −3−2 deg(𝑣𝑣𝑖𝑖)

Since deg(𝑣𝑣𝑖𝑖) number of vertices are adjacent to 𝑢𝑢𝑖𝑖 and the remaining vertices are at distance greater than or equal to

two from 𝑢𝑢𝑖𝑖.

𝑊𝑊𝑊𝑊(𝐺𝐺) =12� 𝑑𝑑(𝑢𝑢𝑖𝑖|𝐺𝐺)2 𝑛𝑛

𝑖𝑖=1

≥12�{3𝑛𝑛 −3−2deg(𝑣𝑣𝑖𝑖)}

𝑛𝑛

𝑖𝑖=1

=12�(3𝑛𝑛 −3)− �2deg(𝑣𝑣𝑖𝑖)

𝑛𝑛

𝑖𝑖=1 𝑛𝑛

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=𝑛𝑛(3𝑛𝑛 −2 3)−42 𝑚𝑚 �deg(𝑣𝑣𝑖𝑖) 𝑛𝑛

𝑖𝑖=1

= 2𝑚𝑚

=𝑛𝑛(3𝑛𝑛 −23)−4𝑚𝑚

𝑊𝑊𝑊𝑊(𝐺𝐺)≥3𝑛𝑛2−32𝑛𝑛 −4𝑚𝑚

The bounds in the above lemma is sharp, for any graph G of diameter two, which we will see in the following theorem,

Theorem 3.1.2: If G(n,m) is a graph with ∆(𝐺𝐺) =𝑛𝑛 −1 then WW(G) = 𝟑𝟑𝟑𝟑𝟐𝟐−𝟑𝟑𝟑𝟑−𝟒𝟒𝟒𝟒

𝟐𝟐 .

Proof: Let 𝑊𝑊𝑊𝑊(𝐺𝐺) =𝑊𝑊(𝐺𝐺) +1

2∑{𝑢𝑢,𝑣𝑣}⊑𝑉𝑉(𝐺𝐺)𝑑𝑑(𝑢𝑢,𝑣𝑣)2

By taking 𝑊𝑊(𝐺𝐺) =𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚 in the theorem 2.1

We get 𝑊𝑊𝑊𝑊(𝐺𝐺) =𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚+1

2∑{𝑢𝑢,𝑣𝑣}⊑𝑉𝑉(𝐺𝐺)𝑑𝑑(𝑢𝑢,𝑣𝑣)2

Let 𝑉𝑉=𝑣𝑣1,𝑣𝑣2, … ,𝑣𝑣𝑛𝑛 and deg(𝑣𝑣𝑛𝑛) =𝑛𝑛 −1. For any arbitrary pair of vertices (𝑣𝑣𝑖𝑖,𝑣𝑣𝑗𝑗). If 𝑑𝑑�𝑣𝑣𝑖𝑖,𝑣𝑣𝑗𝑗�> 2 then we take shortest path �𝑣𝑣𝑖𝑖,𝑣𝑣𝑗𝑗�, (𝑣𝑣𝑛𝑛,𝑣𝑣𝑗𝑗) so that 𝑑𝑑�𝑣𝑣𝑖𝑖,𝑣𝑣𝑗𝑗�= 2 i.e. 𝑑𝑑(𝑣𝑣𝑖𝑖,𝑣𝑣𝑗𝑗)≤2 always. The meaning of deg(𝑣𝑣𝑖𝑖) is the cardinality of 𝑁𝑁𝑁𝑁𝑁𝑁(𝑣𝑣𝑖𝑖). Number of vertices lie at distance 1 from 𝑣𝑣𝑖𝑖. Therefore (𝑛𝑛 −1)−deg(𝑣𝑣𝑖𝑖) is the number of vertices 𝑣𝑣𝑗𝑗.

Which is not in the neighborhood of 𝑣𝑣𝑖𝑖. i.e. (𝑛𝑛 −1)−deg(𝑣𝑣𝑖𝑖) vertices has the distance 2 from 𝑣𝑣𝑖𝑖.

𝑊𝑊𝑊𝑊(𝐺𝐺) =𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚+1

2[�{𝑑𝑑�𝑣𝑣1,𝑣𝑣𝑗𝑗�2+𝑑𝑑�𝑣𝑣2,𝑣𝑣𝑗𝑗�2+⋯+𝑑𝑑�𝑣𝑣𝑛𝑛,𝑣𝑣𝑗𝑗�2} 𝑛𝑛

𝑗𝑗=1

]

𝑊𝑊𝑊𝑊(𝐺𝐺) =𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚+1

2 {� 𝑑𝑑�𝑣𝑣1,𝑣𝑣𝑗𝑗�

2

+� 𝑑𝑑�𝑣𝑣2,𝑣𝑣𝑗𝑗�2 𝑛𝑛

𝑗𝑗=1

+⋯

𝑛𝑛

𝑗𝑗=1

+� 𝑑𝑑�𝑣𝑣𝑛𝑛,𝑣𝑣𝑗𝑗�2 𝑛𝑛

𝑗𝑗=1

=𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚+1

2[(𝑛𝑛 −1)−deg(𝑣𝑣1) + (𝑛𝑛 −1)−deg(𝑣𝑣2) +⋯+ (𝑛𝑛 −1)−deg(𝑣𝑣𝑖𝑖)]

=𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚+1

2{�(𝑛𝑛 −1)− �deg(𝑣𝑣𝑖𝑖)

𝑛𝑛

𝑖𝑖=1 𝑛𝑛

𝑖𝑖=1

}

=𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚+1

2{𝑛𝑛(𝑛𝑛 −1)−2𝑚𝑚} =𝑛𝑛2− 𝑛𝑛 − 𝑚𝑚+𝑛𝑛(𝑛𝑛 −1)

2 − 𝑚𝑚

=3𝑛𝑛(𝑛𝑛 −2 1)− 𝑚𝑚

𝑊𝑊𝑊𝑊(𝐺𝐺) = 3𝑛𝑛2−32𝑛𝑛 −4𝑚𝑚

Illustration: Following is the example for 𝑑𝑑𝑖𝑖𝑎𝑎𝑚𝑚 ≤2 of graph,

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Corollary 3.1.3 If 𝐺𝐺(𝑛𝑛,𝑚𝑚) is a connected graph then the hyper-Wiener index of 𝐺𝐺+𝑥𝑥 is 3𝑛𝑛2−𝑛𝑛−4𝑚𝑚

2

Proof: Let G be a graph with n vertices (𝑣𝑣1,𝑣𝑣2,𝑣𝑣3, … ,𝑣𝑣𝑛𝑛). The graph 𝐺𝐺+𝑥𝑥 is obtained from 𝐺𝐺 by adding ‘𝑛𝑛’ new

edges by joining all the vertices of 𝐺𝐺 to the vertex 𝑥𝑥. Let vertex set of the graph 𝐺𝐺+𝑥𝑥 be (𝑣𝑣1,𝑣𝑣2,𝑣𝑣3, … ,𝑣𝑣𝑛𝑛,𝑥𝑥) and the

edge set be (𝑒𝑒1,𝑒𝑒2, … ,𝑒𝑒𝑚𝑚,𝑒𝑒𝑚𝑚+1, … ,𝑒𝑒𝑛𝑛+𝑚𝑚). The graph 𝐺𝐺+𝑥𝑥 has 𝑛𝑛+ 1 vertices and 𝑛𝑛+𝑚𝑚 edges. Hence substituting

number of vertices as 𝑝𝑝=𝑛𝑛+ 1 and number of edges as 𝑞𝑞=𝑛𝑛+𝑚𝑚 in the previous Theorem,

𝑊𝑊𝑊𝑊(𝐺𝐺+𝑥𝑥) =𝟑𝟑(𝟑𝟑+𝟏𝟏)𝟐𝟐− 𝟑𝟑(𝟑𝟑𝟐𝟐+𝟏𝟏)− 𝟒𝟒(𝟑𝟑+𝟒𝟒)

=𝟑𝟑(𝟑𝟑𝟐𝟐+𝟏𝟏+𝟐𝟐𝟑𝟑)− 𝟑𝟑𝟐𝟐(𝟑𝟑+𝟏𝟏)− 𝟒𝟒𝟑𝟑 − 𝟒𝟒𝟒𝟒

𝑊𝑊𝑊𝑊(𝐺𝐺+𝑥𝑥) =3𝑛𝑛2− 𝑛𝑛 −2 4𝑚𝑚

Illustration: Following is the example for join of two graphs

𝑛𝑛= 4,𝑚𝑚= 4 and 𝑊𝑊𝑊𝑊(𝐺𝐺) = 14

Corollary 3.1.4: If 𝐺𝐺(𝑛𝑛,𝑚𝑚) be a graph and 𝑥𝑥 is any vertex in 𝐺𝐺 of degree 𝑛𝑛 −1 such that the graph 𝐺𝐺 − 𝑥𝑥is connected

then hyper-Wiener index of 𝐺𝐺 − 𝑥𝑥is 3𝑛𝑛2−5𝑛𝑛−4𝑚𝑚+2

2

Proof: Let 𝐺𝐺 be a graph without pendent vertices. If there exists at least one vertex 𝑣𝑣 such that 𝑑𝑑𝑒𝑒𝑑𝑑(𝑣𝑣) =𝑛𝑛 −1. The

vertex 𝑣𝑣 is named as 𝑥𝑥, we remove the vertex 𝑥𝑥 from 𝐺𝐺 is 𝐺𝐺 − 𝑥𝑥. The vertex of 𝐺𝐺 − 𝑥𝑥 is 𝑛𝑛 −1 and the edges be

𝑚𝑚 − 𝑛𝑛+ 1 then by the theorem 3.1.2. 𝑊𝑊𝑊𝑊(𝐺𝐺) = 3𝑛𝑛2−3𝑛𝑛−4𝑚𝑚2

𝑊𝑊𝑊𝑊(𝐺𝐺 − 𝑥𝑥) =3(𝑛𝑛 −1)2−3(𝑛𝑛 −21)−4(𝑚𝑚 − 𝑛𝑛+ 1)

=3(𝑛𝑛2+ 1−2𝑛𝑛)−3𝑛𝑛2+ 3−4𝑚𝑚+ 4𝑛𝑛 −4

=3𝑛𝑛2+ 3−6𝑛𝑛 −3𝑛𝑛2+ 3−4𝑚𝑚+ 4𝑛𝑛 −4

𝑊𝑊𝑊𝑊(𝐺𝐺 − 𝑥𝑥) =3𝑛𝑛2−5𝑛𝑛 −2 4𝑚𝑚+ 2

Illustration: Example for connected 𝐺𝐺 − 𝑥𝑥 of graph

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Theorem 3.1.5: If 𝐺𝐺1(𝑛𝑛1,𝑚𝑚1) and 𝐺𝐺2(𝑛𝑛2,𝑚𝑚2) are two connected graphs then the hyper-Wiener index of 𝐺𝐺1+𝐺𝐺2 is

𝑊𝑊𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =3𝑛𝑛1(𝑛𝑛21−1)+3𝑛𝑛2(𝑛𝑛22−1)+𝑛𝑛1𝑛𝑛2−2𝑚𝑚1−2𝑚𝑚2.

Proof: By definition;

𝑊𝑊𝑊𝑊 =𝑊𝑊(𝐺𝐺) +12 � 𝑑𝑑(𝑢𝑢,𝑣𝑣)2 {𝑢𝑢,𝑣𝑣}⊑𝑉𝑉(𝐺𝐺)

From theorem 2.4

𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =𝑛𝑛1(𝑛𝑛1−1) +𝑛𝑛2(𝑛𝑛2−1) +𝑛𝑛1𝑛𝑛2− 𝑚𝑚1− 𝑚𝑚2

Therefore,

𝑊𝑊𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =𝑛𝑛1(𝑛𝑛1−1) +𝑛𝑛2(𝑛𝑛2−1) +𝑛𝑛1𝑛𝑛2− 𝑚𝑚1− 𝑚𝑚2+12 � 𝑑𝑑(𝑢𝑢,𝑣𝑣)2 {𝑢𝑢,𝑣𝑣}⊑𝑉𝑉(𝐺𝐺)

The graph 𝐺𝐺1 has 𝑛𝑛1 vertices with degree sequence (𝑑𝑑1,𝑑𝑑2,𝑑𝑑3, … ,𝑑𝑑𝑛𝑛1). The graph 𝐺𝐺2 has 𝑛𝑛2 vertices with degree

sequence (𝑑𝑑1,𝑑𝑑2,𝑑𝑑3, … ,𝑑𝑑𝑛𝑛2). In 𝐺𝐺1+𝐺𝐺2 graph all the vertices of 𝑛𝑛1 and 𝑛𝑛2 are at distance one. In graph

𝐺𝐺1, (𝑛𝑛1−1)−deg(𝑣𝑣𝑖𝑖𝑛𝑛1) vertices are at distance two and similarly graph 𝐺𝐺2, (𝑛𝑛2−1)−deg(𝑣𝑣𝑖𝑖𝑛𝑛2) vertices are at

distance two.

Then,

𝑊𝑊𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =𝑛𝑛1(𝑛𝑛1−1) +𝑛𝑛2(𝑛𝑛2−1) +𝑛𝑛1𝑛𝑛2− 𝑚𝑚1− 𝑚𝑚2

+12�{(𝑛𝑛1−1)−deg�𝑣𝑣𝑛𝑛1�+ (𝑛𝑛1−1)−deg(𝑣𝑣𝑖𝑖𝑛𝑛1)}

𝑛𝑛

1

𝑊𝑊𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =𝑛𝑛1(𝑛𝑛1−1) +𝑛𝑛2(𝑛𝑛2−1) +𝑛𝑛1𝑛𝑛2− 𝑚𝑚1− 𝑚𝑚2

+12{�(𝑛𝑛1−1)− �deg�𝑣𝑣𝑛𝑛1�

𝑛𝑛

1

+�(𝑛𝑛1−1)

𝑛𝑛

1

− �deg(𝑣𝑣𝑖𝑖𝑛𝑛1)

𝑛𝑛

1

}

𝑛𝑛

1

𝑊𝑊𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =𝑛𝑛1(𝑛𝑛1−1) +𝑛𝑛2(𝑛𝑛2−1) +𝑛𝑛1𝑛𝑛2− 𝑚𝑚1− 𝑚𝑚2+12{𝑛𝑛1(𝑛𝑛1−1)−2𝑚𝑚1+𝑛𝑛2(𝑛𝑛2−1)−2𝑚𝑚2}

𝑊𝑊𝑊𝑊(𝐺𝐺1+𝐺𝐺2) =3𝑛𝑛1(𝑛𝑛21−1)+3𝑛𝑛2(𝑛𝑛22−1)+𝑛𝑛1𝑛𝑛2−2𝑚𝑚1−2𝑚𝑚2

Illustration: Example for 𝐺𝐺1+𝐺𝐺2 of two graphs

𝑛𝑛1= 3,𝑛𝑛2= 2,𝑚𝑚1= 2,𝑚𝑚2= 1 and 𝑊𝑊𝑊𝑊(𝐺𝐺) = 12.

Theorem 3.6: The hyper-Wiener index of 𝑊𝑊𝑊𝑊(𝐺𝐺1) =3𝑙𝑙(𝑙𝑙−1)

2 +

3𝑛𝑛(𝑛𝑛−1)

2 +𝑛𝑛𝑙𝑙 −2𝑚𝑚. Where 𝐺𝐺1=𝐺𝐺+𝑙𝑙𝐾𝐾1

Proof: Let 𝐺𝐺(𝑛𝑛,𝑚𝑚) be a connected graph. The graph 𝐺𝐺1 =𝐺𝐺+𝑙𝑙𝐾𝐾1 is obtained from graph 𝐺𝐺 by joining all the vertices

of graph 𝐺𝐺 to the new 𝑙𝑙 vertices of graph 𝐺𝐺 to the new 𝑙𝑙 vertices of (𝑥𝑥1,𝑥𝑥2,𝑥𝑥3, … ,𝑥𝑥𝑙𝑙), the vertex set of 𝐺𝐺1 be

𝑉𝑉(𝐺𝐺1) = {𝑣𝑣

1,𝑣𝑣2, …𝑣𝑣𝑛𝑛,𝑥𝑥1,𝑥𝑥2,𝑥𝑥3, … ,𝑥𝑥𝑙𝑙} and the edge set be 𝐸𝐸(𝐺𝐺1) =𝐸𝐸(𝐺𝐺)⊔{𝑣𝑣𝑖𝑖𝑥𝑥𝑗𝑗: 1 <𝑖𝑖<𝑛𝑛, 1 <𝑗𝑗<𝑙𝑙}.

By definition:

𝑊𝑊𝑊𝑊(𝐺𝐺1) =𝑊𝑊(𝐺𝐺1) +1

2{𝑢𝑢,𝑣𝑣}⊑𝑉𝑉(𝐺𝐺)� 𝑑𝑑(𝑢𝑢,𝑣𝑣)2

From theorem 2.5

(6)

Therefore,

𝑊𝑊𝑊𝑊(𝐺𝐺1) =𝑙𝑙(𝑙𝑙 −1) +𝑛𝑛(𝑛𝑛 −1) +𝑙𝑙𝑛𝑛 − 𝑚𝑚+1

2 � 𝑑𝑑(𝑢𝑢,𝑣𝑣)2

{𝑢𝑢,𝑣𝑣}⊑𝑉𝑉(𝐺𝐺)

𝑊𝑊𝑊𝑊(𝐺𝐺1) =𝑙𝑙(𝑙𝑙 −1) +𝑛𝑛(𝑛𝑛 −1) +𝑙𝑙𝑛𝑛 − 𝑚𝑚+1

2 {�(𝑛𝑛 −1)

𝑛𝑛

𝑖𝑖=1

− � 𝑑𝑑𝑒𝑒𝑑𝑑𝑣𝑣𝑖𝑖+ 1 + 1 +���������⋯+ 1

𝑙𝑙(𝑙𝑙−1) 𝑛𝑛

𝑖𝑖=1

}

𝑊𝑊𝑊𝑊(𝐺𝐺1) =𝑙𝑙(𝑙𝑙 −1) +𝑛𝑛(𝑛𝑛 −1) +𝑙𝑙𝑛𝑛 − 𝑚𝑚+1

2 {𝑛𝑛(𝑛𝑛 −1)−2𝑚𝑚+𝑙𝑙(𝑙𝑙 −1)}

𝑊𝑊𝑊𝑊(𝐺𝐺1) =3𝑙𝑙(𝑙𝑙 −1)

2 +

3𝑛𝑛(𝑛𝑛 −1)

2 +𝑛𝑛𝑙𝑙 −2𝑚𝑚

Illustration: Example for 𝐺𝐺1of graphs

𝑙𝑙= 2,𝑛𝑛= 3,𝑚𝑚= 3 and 𝑊𝑊𝑊𝑊(𝐺𝐺1) = 12

REFERENCES

[1] D. J. Klein, I. Lukovits, I. Gutman, On the definition of the hyper-Wiener index for cycle-containing

structures, J. Chem. Inf. Comput. Sci. 35 (1995).

[2] F. Buckley, F. Harary, Distances in Graphs, Addison-Wesley, Redwood, 1990.

[3] H. B. Walikar, H. S. Ramane, V. S. Shigehalli, Wiener number of Dendrimers, In: Proc. National Conf. on

Mathematical and Computational Models, (Eds. R. Nadarajan and G. Arulmozhi), Applied Publishers, New Delhi, 2003, 361-368.

[4] H. B. Walikar, V. S. Shigehalli, H. S. Ramane, Bounds on the Wiener number of a graph, MATCH comm.

Math. Comp. Chem., 50 (2004), 117-132.

[5] H. Wiener, Structural determination of paraffin boiling points, J. Amer. Chem. Soc., 69 (1947), 17-20.

[6] J. Baskar Babujee and J. Senbagamalar, “Wiener Index of Graphs using Degree Sequence”, Applied

Mathematical Sciences, Vol. 6, 2012, no. 88, 4387-4395.

[7] Randic, M., Novel molecular description for structure-property studies, Chem. Phys. Lett., 211 (1993),

478-483.

[8] Shigehalli V. S. and Shanmukh Kuchabal, “On the invariance of topological indices”, International Journal of

Mathematical Archive-5(12), 2014,122-125.

[9] Shigehalli V. S. and Shanmukh Kuchabal, On the hyper-Wiener index of thorny-cocktail party graphs,

International Journal of Mathematical Archive-6(3), 2015,1-6.

[10]Shigehalli V. S. and Shanmukh Kuchabal, On the hyper-Wiener index of thorny-complete graph”, Journal of

Global Research in Mathematical Archives, Volume 2, No. 6, June 2014 Page No. 55-61, 2014.

[11]Shigehalli V. S. and Shanmukh Kuchabal, On the hyper-Wiener index of thorny-wheel graphs”, Bulletin of

Mathematics and Statistics Research, Vol. 3. Issue. 1. Page No. 25-33 2015.

Source of support: Nil, Conflict of interest: None Declared

References

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