Ratio Mathematica Volume 45, 2023 ` The Connected Vertex Strong Geodetic Number of a Graph C. Saritha* T. Muthu Nesa Beula† Abstract In this paper we introduce the concept of connected vertex strong geodetic number 𝑐𝑔𝑠π‘₯ (𝐺) of a graph 𝐺 at a vertex π‘₯ and investigate its properties. We determinebounds for it and find the same for some special classes of graphs. We prove that𝑠𝑔π‘₯ (𝐺) ≀ 𝑐𝑠𝑔π‘₯ (𝐺) for any vertex π‘₯ in 𝐺is connected graphs of order 𝑛 β‰₯ 2with one are characterized for some vertex π‘₯ in 𝐺.Necessary conditions for𝑠𝑔π‘₯ (𝐺) to be 𝑛 or 𝑛 βˆ’ 1 are given for some vertex π‘₯ in 𝐺. It is shown for every pair of integersπ‘Ž and 𝑏 with 2 ≀ π‘Ž ≀ 𝑏, there exists a connected graph 𝐺 such that 𝑠𝑔π‘₯ (𝐺) = π‘Ž and 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑏 for some vertex π‘₯ in 𝐺. Keywords: strong geodetic number;vertex strong geodetic number; connected strong geodetic number. 2010 AMS subject classification: 05C15‑. *Register Number 20123182092003, Research Scholar, Department of Mathematics, Women’s Christian College, Nagercoil629 001, Affiliated to Manonmaniam Sundaranar University, Abishekapatti, Tirunelveli-627 012, Tamil Nadu, India. saritha.c2012@gmail.com. †Assistant Professor, Department of Mathematics, Women’s Christian College, Nagercoil - 629 001, Affiliated to Manonmaniam Sundaranar University, Abishekapatti, Tirunelveli-627 012, Tamil Nadu, India.tmnbeula@gmail.com. ‑Received on July 28, 2022. Accepted on October 15, 2022. Published on January 25, 2023. doi: 10.23755/rm.v45i0.978. ISSN: 1592-7415. eISSN: 2282-8214. Β©The Authors. This paper is published under the CC-BY license agreement. 52 mailto:saritha.c2012@gmail.com C. Saritha and T. Muthu Nesa Beula 1. Introduction By a graph 𝐺 = (𝑉, 𝐸), we mean a finite, undirected connected graph without loops or multiple edges. The order and size of 𝐺 are denoted by 𝑛 and π‘š respectively. For basic graph theoretic terminology, we refer to [1]. Two vertices 𝑒 and 𝑣 are said to be adjacent if 𝑒𝑣 is an edge of 𝐺. Two edges of 𝐺 are said to be adjacent if they have a common vertex. The distance𝑑(𝑒, 𝑣) between two vertices 𝑒 and v in a connected graph 𝐺 is the length of a shortest 𝑒-𝑣 path in 𝐺. An π‘’βˆ’π‘£ path of length 𝑑(𝑒, 𝑣) is called an π‘’βˆ’π‘£geodesic.An π‘₯ βˆ’ 𝑦 path of length 𝑑(π‘₯, 𝑦) is called geodesic. A vertex 𝑣 is said to lie on a geodesic 𝑃 if 𝑣 is an internal vertex of 𝑃. The closed interval 𝐼[π‘₯, 𝑦] consists of π‘₯, 𝑦 and all vertices lying on some π‘₯ βˆ’ 𝑦 geodesic of 𝐺 and for a non-empty set 𝑆 βŠ† 𝑉 (𝐺), 𝐼[𝑆] = βˆͺπ‘₯,π‘¦βˆˆπ‘† 𝐼[π‘₯, 𝑦]. A set 𝑆 βŠ† 𝑉 (𝐺) in a connected graph 𝐺 is a geodetic set of 𝐺 if 𝐼[𝑆] = 𝑉 (𝐺). The geodetic number of 𝐺, denoted by 𝑔(𝐺), is the minimum cardinality of a geodetic set of 𝐺.The geodetic concept were studied in [1, 3, 4]. Let π‘₯ be a vertex of 𝐺 and 𝑆 βŠ† 𝑉 βˆ’ {π‘₯}. Then for each vertex𝑦 ∈ 𝑆, π‘₯ β‰  𝑦. Let οΏ½ΜƒοΏ½π‘₯ [𝑦] be a selected fixed shortest π‘₯-𝑦 path. Then we set 𝐼π‘₯ [𝑆] = {οΏ½ΜƒοΏ½π‘₯ (𝑦): 𝑦 ∈ 𝑆} and let 𝑉(𝐼π‘₯ [𝑆]) = ⋃ 𝑉(𝑃) π‘βˆˆπΌπ‘₯[𝑆] . If 𝑉(𝐼π‘₯ [𝑆]) = 𝑉 for some 𝐼π‘₯ [𝑆]then the set 𝑆 is called a vertex strong geodetic set of 𝐺. The minimum cardinality of a vertex strong geodetic set of 𝐺 is called the vertex strong geodetic number of 𝐺 and is denoted by 𝑠𝑔π‘₯ (𝐺).The following theorem is used in sequel. Theorem 1.1[4] Each extreme vertex of a connected graph belong to every geodetic set of 𝐺. 2. The connected vertex strong geodetic number of a graph Definition 2.1. Let π‘₯ be a vertex of 𝐺 and 𝑆 βŠ† 𝑉 βˆ’ {π‘₯}. Then for each vertex𝑦 ∈ 𝑆, π‘₯ β‰  𝑦. Let οΏ½ΜƒοΏ½π‘₯ [𝑦] be a selected fixed shortest π‘₯-𝑦 path. Then we set 𝐼π‘₯ [𝑆] = {οΏ½ΜƒοΏ½π‘₯ (𝑦): 𝑦 ∈ 𝑆} and let 𝑉(𝐼π‘₯ [𝑆]) = ⋃ 𝑉(𝑃) π‘βˆˆπΌπ‘₯[𝑆] . If 𝑉(𝐼π‘₯ [𝑆]) = 𝑉 for some 𝐼π‘₯ [𝑆]then the set 𝑆 is called a vertex strong geodetic set of 𝐺. A vertex strong geodetic set S of x of G is called a connected vertex strong geodetic set of G if G[S] is connected. The minimum cardinality of a connected vertex strong geodetic set of 𝐺 is called the connected vertex strong geodetic number of 𝐺 and is denoted by 𝑐𝑠𝑔π‘₯ (𝐺). Example 2.2.For the graph 𝐺 given in Figure 2.1,𝑐𝑠𝑔π‘₯-sets and 𝑐𝑠𝑔π‘₯ (𝐺) for each vertex π‘₯ is given in the following Table 2.1. 53 The Connected Vertex Strong Geodetic Number of a Graph Table 2.1 Observation 2.3. Let π‘₯ be any vertex of a connected graph𝐺. (i) If 𝑦 β‰  π‘₯ be a simplicial vertex of 𝐺, then 𝑦 belongs to every connected π‘₯- vertex strong geodetic set of 𝐺. (ii) The eccentric vertices of π‘₯ belong to every connected π‘₯-vertex strong geodetic set of 𝐺. In the following we determine the connected vertex strong geodetic number of some standard graphs 𝐺 for each vertex in 𝐺. Theorem 2.4.For the path𝐺 = 𝑃𝑛 (𝑛 β‰₯ 3), 𝑐𝑠𝑔π‘₯ (𝐺) = { 1 𝑖𝑓 π‘₯ 𝑖𝑠 π‘Žπ‘› 𝑒𝑛𝑑 π‘£π‘’π‘Ÿπ‘‘π‘’π‘₯ π‘œπ‘“ 𝐺 𝑛 𝑖𝑓 π‘₯ 𝑖𝑠 π‘Ž 𝑐𝑒𝑑 π‘£π‘’π‘Ÿπ‘‘π‘’π‘₯ π‘œπ‘“ 𝐺 Proof. Let 𝑃𝑛 be 𝑣1, 𝑣2, … , 𝑣𝑛. If π‘₯ = 𝑣1, then 𝑆 = {𝑣𝑛 } is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 1. Similarly if π‘₯ = 𝑣𝑛, then 𝑐𝑠𝑔π‘₯ (𝐺) = 1. Let π‘₯ be a cut vertex of 𝐺. Then by Observation 2.3 (i) Vertex 𝑐𝑠𝑔π‘₯-sets 𝑐𝑠𝑔π‘₯ (𝐺) 𝑣1 {𝑣3, 𝑣4}, {𝑣4, 𝑣5} 2 𝑣2 {𝑣4, 𝑣5, 𝑣6} 3 𝑣3 {𝑣1, 𝑣6}, {𝑣5, 𝑣6} 2 𝑣4 {𝑣1, 𝑣6}, {𝑣1, 𝑣2} 2 𝑣5 {𝑣1, 𝑣2, 𝑣3} 3 𝑣6 {𝑣3, 𝑣4}, {𝑣2, 𝑣3} 2 𝑣1 𝑣4 𝑣5 𝐺 Figure 2.1 𝑣2 𝑣3 𝑣6 54 C. Saritha and T. Muthu Nesa Beula {𝑣1, 𝑣𝑛 } is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺. Let 𝑆 be a 𝑐𝑠𝑔π‘₯-set of 𝐺. Since 𝐺[𝑆] is connected, it follows that 𝑆 = 𝑉(𝐺) is the unique 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛.∎ Theorem 2.5.For the cycle 𝐺 = 𝐢𝑛(𝑛 β‰₯ 4), 𝑐𝑠𝑔π‘₯ (𝐺) = 2, for every π‘₯ ∈ 𝐺. Proof. Let 𝑉(𝐢𝑛) = {𝑣1, 𝑣2, … , 𝑣𝑛}. Without loss of generality let us assume that π‘₯ = 𝑣1. Case (i) Let 𝑛 be even. Let 𝑛 = 2π‘˜ (π‘˜ β‰₯ 2). Then π‘£π‘˜+1 is the eccentric vertex of 𝐺. By Observation 2.3(ii) since {π‘£π‘˜+1} is not a 𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 2. Let 𝑆 = {π‘£π‘˜+1, π‘£π‘˜+2}. Then 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 2. Case (ii) Let 𝑛 be odd. Let 𝑛 = 2π‘˜ + 1 (π‘˜ β‰₯ 2). Then 𝑆 = {π‘£π‘˜+1,π‘£π‘˜+2} is the eccentric vertices of 𝐺. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 2. Since 𝑆 is a 𝑠𝑔π‘₯-set of 𝐺 and 𝐺[𝑆] is connected, 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 sothat 𝑐𝑠𝑔π‘₯ (𝐺) = 2.∎ Theorem 2.6.For the complete graph 𝐺 = 𝐾𝑛(𝑛 β‰₯ 4), 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1, for every π‘₯ ∈ 𝐺. Proof. Let π‘₯ be a vertex of 𝐺. Let 𝑆 = 𝑉(𝐺) βˆ’ {π‘₯}. Since every vertex of 𝐺 is an extreme vertex of 𝐺, it follows from Observation 2.3(i), 𝑆 is the unique 𝑐𝑠𝑔π‘₯-set of 𝐺 so that𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 1 for every vertex π‘₯ in 𝐺.∎ Theorem 2.7.For the fan graph 𝐺 = 𝐾1 + π‘ƒπ‘›βˆ’1(𝑛 β‰₯ 5). 𝑐𝑠𝑔π‘₯ (𝐺) = { 𝑛 βˆ’ 1 𝑖𝑓 π‘₯ ∈ 𝑉(𝐾1) 𝑛 βˆ’ 3 𝑖𝑓 π‘₯ 𝑖𝑠 𝑒π‘₯π‘‘π‘Ÿπ‘’π‘šπ‘’ π‘£π‘’π‘Ÿπ‘‘π‘’π‘₯ π‘œπ‘“ π‘ƒπ‘›βˆ’1 𝑛 βˆ’ 2 𝑖𝑓 π‘₯ 𝑖𝑠 π‘–π‘›π‘‘π‘’π‘Ÿπ‘›π‘Žπ‘™ π‘£π‘’π‘Ÿπ‘‘π‘’π‘₯ π‘œπ‘“ π‘ƒπ‘›βˆ’1 Proof. Let 𝑉(𝐾1) = 𝑦 and 𝑉(π‘ƒπ‘›βˆ’1) = {𝑣1, 𝑣2, … , π‘£π‘›βˆ’1}. Case (i) Letπ‘₯ = 𝑦, Then 𝑆 = {𝑣1, 𝑣2, … , 𝑣𝑛 } is a set of all eccentric vertices for π‘₯. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 1. Since 𝐺[𝑆] is connected, 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1. Let π‘₯ ∈ 𝑉(π‘ƒπ‘›βˆ’1). Let π‘₯ = 𝑣1. Then 𝑆 = {𝑣3, 𝑣4, … , π‘£π‘›βˆ’1} are eccentric vertices of 𝐺. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯ -set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 3. Now 𝑆 is a 𝑠𝑔π‘₯-set of 𝐺 and 𝐺[𝑆] is connected. Therefore 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 3. If π‘₯ = π‘£π‘›βˆ’1, by the similar way we can prove that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 3. Let π‘₯ ∈ {𝑣2, 𝑣3, … , π‘£π‘›βˆ’2}. Without loss of generality let us assume that π‘₯ = 𝑣2. Then {𝑣1, π‘£π‘›βˆ’1} is set of extreme vertices of 𝐺. By Observation 2.3 (i) {𝑣1, π‘£π‘›βˆ’1} is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺. {𝑣4, 𝑣5, … , π‘£π‘›βˆ’2} is the set of eccentric vertices of 𝑣2. Then {𝑣4, 𝑣5, … , π‘£π‘›βˆ’2}is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺. Let 𝑆 β€² = {𝑣1, 𝑣4, 𝑣5, … , π‘£π‘›βˆ’2,π‘£π‘›βˆ’1,}. Then 𝑆′ is a 𝑠𝑔π‘₯-set of 𝐺 but 𝐺[𝑆 β€²] is not connected. Therefore 𝑆′ βˆͺ {𝑦} is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 2.∎ Theorem 2.8.For the wheel graph 𝐺 = 𝐾1 + πΆπ‘›βˆ’1(𝑛 β‰₯ 5). 𝑐𝑠𝑔π‘₯ (𝐺) = { 𝑛 βˆ’ 1 𝑖𝑓 π‘₯ ∈ 𝑣1 𝑛 βˆ’ 3 𝑖𝑓 π‘₯ ∈ 𝑉(πΆπ‘›βˆ’1) Proof. Let 𝑉(𝐾1) = 𝑦 and 𝑉(πΆπ‘›βˆ’1) = {𝑣1, 𝑣2, … , π‘£π‘›βˆ’1}. 55 The Connected Vertex Strong Geodetic Number of a Graph Case(i) Letπ‘₯ = 𝑦, Then 𝑆 = {𝑣1, 𝑣2, … , π‘£π‘›βˆ’1} is a set of all eccentric vertices for π‘₯. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 1. Since 𝐺[𝑆] is connected, 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1. Case (ii) Let π‘₯ ∈ 𝑉(πΆπ‘›βˆ’1). Without loss of generality, let us assume that π‘₯ = 𝑣1. Then 𝑆 = {𝑣3, 𝑣4, … , π‘£π‘›βˆ’1} are eccentric vertices of 𝐺. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯ -set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 3. Now 𝑆 is a 𝑠𝑔π‘₯-set of 𝐺 and 𝐺[𝑆] is connected. Therefore 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 3.∎ Theorem 2.9.For the star graph 𝐺 = 𝐾1,π‘›βˆ’1(𝑛 β‰₯ 3), 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1 for every π‘₯ ∈ 𝐺. Proof. Let𝑦 be the cut vertex of 𝐺 and {𝑣1, 𝑣2, … , π‘£π‘›βˆ’1} is a set of all eccentric vertices of 𝐺.Letπ‘₯ = 𝑦, Then 𝑆 = {𝑣1, 𝑣2, … , π‘£π‘›βˆ’1} is a set of all eccentric vertices for π‘₯. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 1. Since 𝐺[𝑆] is connected, 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1. Let π‘₯ ∈ {𝑣1, 𝑣2, … , π‘£π‘›βˆ’1} Without loss of generality, let us assume that π‘₯ = 𝑣1. Then 𝑆 = {𝑣2, 𝑣3, … , π‘£π‘›βˆ’1} are set of eccentric vertices of 𝑣1. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑠𝑔π‘₯-set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 2. Now 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 but 𝐺[𝑆] is not a 𝑐𝑠𝑔π‘₯-set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 1. Let 𝑆 β€² = 𝑆 βˆͺ {π‘₯}. Then 𝑆′ is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1.∎ Theorem 2.10.For the Peterson graph 𝐺, 𝑐𝑠𝑔π‘₯ (𝐺) = 6 for every π‘₯ ∈ 𝐺. Proof. Case (i) Letπ‘₯ ∈ {𝑣1, 𝑣2, 𝑣3, 𝑣4, 𝑣5}. Without loss of generality let us assume that π‘₯ = 𝑣1. Then 𝑆 = {𝑣2, 𝑣5, 𝑣7, 𝑣8, 𝑣9, 𝑣10} is the set of all eccentric vertices for π‘₯. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯ -set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 6. Since 𝑆 is a 𝑠𝑔π‘₯-set of 𝐺 and 𝐺[𝑆] is connected, 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 6. Case (ii) Letπ‘₯ ∈ {𝑣6, 𝑣7, 𝑣8, 𝑣9, 𝑣10}. Without loss of generality let us assume that π‘₯ = 𝑣6. Then 𝑆 = {𝑣2, 𝑣3, 𝑣4, 𝑣5, 𝑣8, 𝑣9} is the set of all eccentric vertices for π‘₯. By Observation 2.3 (ii) 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯ -set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 6. Since 𝑆 is a 𝑠𝑔π‘₯-set of 𝐺 and 𝐺[𝑆] is connected, 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 6.∎ 56 C. Saritha and T. Muthu Nesa Beula Theorem 2.11.Let 𝐺 be a connected graph. Then 1 ≀ 𝑠𝑔π‘₯ (𝐺) ≀ 𝑐𝑠𝑔π‘₯ (𝐺) ≀ 𝑛 for every vertex π‘₯ in 𝐺. Proof. Let π‘₯ be a vertex of 𝐺. Since every 𝑠𝑔π‘₯-set of 𝐺 needs at least one vertex 𝑠𝑔π‘₯ (𝐺) β‰₯ 1. Since every connected strong vertex geodetic set of 𝐺 is a strong vertex geodetic set of 𝐺, 𝑠𝑔π‘₯ (𝐺) ≀ 𝑐𝑠𝑔π‘₯ (𝐺). Since 𝑉(𝐺) is a connected strong vertex geodetic set of 𝐺, 𝑐𝑠𝑔π‘₯ (𝐺) ≀ 𝑛. Therefore 1 ≀ 𝑠𝑔π‘₯ (𝐺) ≀ 𝑐𝑠𝑔π‘₯ (𝐺) ≀ 𝑛.∎ Theorem 2.12.Let 𝐺 be a connected graph. Then 𝑐𝑠𝑔π‘₯ (𝐺) = 1 if and only if π‘₯ is an end vertex of 𝑃𝑛(𝑛 β‰₯ 2). Proof. Let π‘₯ be an end vertex of 𝑃𝑛. Then by Theorem 2.4, 𝑐𝑠𝑔π‘₯ (𝐺) = 1. Conversely let 𝑐𝑠𝑔π‘₯ (𝐺) = 1. Let 𝑆 = {𝑦} be the 𝑐𝑠𝑔π‘₯-set of π‘₯. We prove that π‘₯ is an end vertex of 𝑃𝑛. On the contrary suppose that π‘₯ is not an end vertex of 𝑃𝑛. Then there are at least two π‘₯ βˆ’ 𝑦 geodesics, which is a contradiction to 𝑆 a 𝑐𝑠𝑔π‘₯-set of 𝐺. Therefore π‘₯ is an end vertex of 𝑃𝑛.∎ Theorem 2.13.Let 𝐺 be a connected graph and π‘₯ ∈ 𝐺. If π‘₯ is a universal vertex of 𝐺. Then 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1. Proof. Let π‘₯ be a universal vertex of 𝐺. Then 𝑉(𝐺) βˆ’ {π‘₯} is set of all eccentric vertices for π‘₯. By Observation 2.3 (ii), 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺 and so 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 1. Since 𝐺[𝑆] is connected, 𝑆 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛 βˆ’ 1.∎ Theorem 2.14.Let 𝐺 be a connected graph and π‘₯ ∈ 𝐺. If π‘₯ is a cut vertex and universal vertex of 𝐺. Then𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛. Proof. Since π‘₯ is a universal vertex of 𝐺, then 𝑉(𝐺) βˆ’ {π‘₯} is set of all eccentric vertices for π‘₯. By Observation 2.3 (ii), 𝑆 is a subset of every 𝑐𝑠𝑔π‘₯-set of 𝐺 and so 𝑣9 𝑣10 G Figure 2.2 𝑣4 𝑣2 𝑣6 𝑣8 𝑣3 𝑣5 𝑣1 𝑣7 57 The Connected Vertex Strong Geodetic Number of a Graph 𝑐𝑠𝑔π‘₯ (𝐺) β‰₯ 𝑛 βˆ’ 1. Since 𝐺[𝑆] is not connected, 𝑆 is not a 𝑐𝑠𝑔π‘₯-set of 𝐺. Therefore 𝑆 = 𝑉(𝐺) is the unique 𝑐𝑠𝑔π‘₯-set of 𝐺. Hence 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑛.∎ Theorem 2.15. For every pair of integersπ‘Ž and 𝑏 with 2 ≀ π‘Ž ≀ 𝑏, there exists a connected graph 𝐺 such that 𝑠𝑔π‘₯ (𝐺) = π‘Ž and 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑏 for some vertex π‘₯ in 𝐺. Proof.For π‘Ž = 𝑏, let 𝐺 = πΎπ‘Ž+1. Then by Theorem 2.11𝑠𝑔π‘₯ (𝐺) = 𝑐𝑠𝑔π‘₯ (𝐺) = π‘Ž for every vertex π‘₯ in 𝐺. For 𝑏 = π‘Ž + 1,let 𝐺 = 𝐾1,π‘Ž. Let π‘₯ be a universal vertex of 𝐺. Then by Theorem 2.14,𝑠𝑔π‘₯ (𝐺) = π‘Ž and 𝑐𝑠𝑔π‘₯ (𝐺) = π‘Ž + 1. So, let 𝑏 β‰₯ π‘Ž + 2. Let 𝑃0: 𝑒0, 𝑒1, 𝑒2, … , π‘’π‘βˆ’π‘Ž, π‘’π‘βˆ’π‘Ž+1be a path of order 𝑏 βˆ’ π‘Ž + 2. Let 𝐺 be the graph obtained from 𝑃 by adding the new vertices 𝑧1, 𝑧2, … , π‘§π‘Žβˆ’1 and introducing the edges 𝑧𝑖 𝑒 (1 ≀ 𝑖 ≀ 𝑏 βˆ’ π‘Ž + 1). The graph 𝐺is shown in Figure 2.3. Let π‘₯ = π‘’π‘βˆ’π‘Ž+1. First we prove that 𝑠𝑔π‘₯(𝐺) = π‘Ž.Let𝑆 = {𝑒0, 𝑧1, 𝑧2, … , π‘§π‘Žβˆ’1, π‘’π‘βˆ’π‘Ž+1}be the end vertices of 𝐺. By Observation 2.3(i), 𝑆1 = 𝑆 βˆ’ {π‘’π‘βˆ’π‘Ž+1} is a subset of every 𝑠𝑔π‘₯-set of 𝐺 and so 𝑠𝑔π‘₯ (𝐺) β‰₯ π‘Ž. Since 𝑆1 is a 𝑠𝑔π‘₯-set of 𝐺, 𝑠𝑔π‘₯ (𝐺) = π‘Ž. Next we prove that 𝑐𝑠𝑔π‘₯ (𝐺)= 𝑏.By Observation, 𝑆1 is a subset of every𝑐𝑠𝑔π‘₯-set of 𝐺. Since 𝐺[𝑆1] is not connected 𝑆1 is not a 𝑐𝑠𝑔π‘₯-set of 𝐺. let 𝑆2 = 𝑆1 βˆͺ {𝑒1, 𝑒2, … , π‘’π‘βˆ’π‘Ž}. Then 𝑆2 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 and𝐺[𝑆2] is connected. Therefore 𝑆2 is a 𝑐𝑠𝑔π‘₯-set of 𝐺 so that , 𝑐𝑠𝑔π‘₯ (𝐺) = 𝑏.∎ 3. Conclusions In this article we explore the concept of the forcing strong geodetic number of a graph. We extend this concept to some other distance related parameters in graphs. 𝑧1 𝑧2 π‘§π‘Žβˆ’1 𝑒2 π‘’π‘βˆ’π‘Ž 𝐺 Figure 2.3 𝑒0 𝑒1 π‘’π‘βˆ’π‘Ž+1 58 C. Saritha and T. Muthu Nesa Beula References [1] F. Buckley and F. Harary, Distance in Graphs, Addison-Wesley, Redwood City, CA, 1990. [2] L. G. Bino Infanta and D. Antony Xavier, Strong upper geodetic number of graphs, Communications in Mathematics and Applications 12(3), (2021)737–748. [3]G. Chartrand and P. Zhang, The forcing geodetic number of a graph, Discuss. Math. 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