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Article

The Complexity of Classes of Pyramid Graphs Based on the Fritsch Graph and Its Related Graphs

1
Department of Mathematics, Applied College at Mahail Aseer, King Khalid University, Abha 61421, Saudi Arabia
2
Department of Mathematics, Faculty of Science, Taibah University, Al-Madinah Al-Nunawara 30001, Saudi Arabia
3
Department of Mathematics and Computer Sciences, Faculty of Science, Menoufia University, Shebin El Kom 32511, Egypt
*
Author to whom correspondence should be addressed.
Axioms 2025, 14(8), 622; https://doi.org/10.3390/axioms14080622
Submission received: 5 June 2025 / Revised: 29 July 2025 / Accepted: 6 August 2025 / Published: 8 August 2025
(This article belongs to the Special Issue Graph Theory and Combinatorics: Theory and Applications)

Abstract

A quantitative study of the complicated three-dimensional structures of artificial atoms in the field of intense matter physics requires a collaborative method that combines a statistical analysis of unusual graph features related to atom topology. Simplified circuits can also be produced by using similar transformations to streamline complex circuits that need laborious mathematical calculations during analysis. These modifications can also be used to determine the number of spanning trees required for specific graph families. The explicit derivation of formulas to determine the number of spanning trees for novel pyramid graph types based on the Fritsch graph, which is one of only six graphs in which every neighborhood is a 4- or 5-vertex cycle, is the focus of our study. We conduct this by utilizing our understanding of difference equations, weighted generating function rules, and the strength of analogous transformations found in electrical circuits.

1. Introduction

A spanning tree is a subgraph of an undirected, connected graph that contains every vertex in the original graph but only utilizes the fewest edges required to join them, creating a tree structure (i.e., no cycles). It basically connects every node in a network without forming unnecessary loops.
The complexity τ ( G ) of G is another name for the number of spanning trees τ ( G ) , which is equal to the total number of different spanning subgraphs of G that are trees.
Determining closed-form expressions for the complexity (number of spanning trees) in various graph types has garnered significant interest. Eulerian circuit counting [1], network analysis techniques in psychological networks [2], chemical isomer enumeration [3,4], and solving intractable issues like the traveling salesman and Steiner tree problems [5] are some of the important applications of this field of study. It is also possible to identify the most complex graphs by examining various graph types, which have applications in network resilience [6,7].
A graph must have a spanning tree since every node in the network it represents needs to be able to communicate with every other node. Dependability can be raised by increasing the number of spanning trees.
A Kirchhoff classical result [8] from 1847 can be used to determine the number of spanning trees for a connected graph G = ( V , E ) with n vertices. With A representing the adjacency matrix of G and D representing the diagonal matrix of its degrees, the Kirchhoff matrix is a characteristic matrix L = D A , where L = [ a i j ] is defined as follows:
L = [ a i j ] = deg ( v i )   i f     i = j 1   i f     ( v i , v j ) E ( G ) 0   i f     ( v i , v j ) E ( G )
All co-factors of L are equal to the number of spanning trees in the graph G .
Another technique to calculate the complexity of a graph G   w i t h   n   v e r t i c e s is as follows: Let μ 1 μ 2 μ n ( = 0 ) represent the L matrix’s eigenvalues. Kelmans and Chelnokov [9] demonstrated the following in 1974:
τ ( G ) = 1 n i = 1 n 1 μ i
One common method for counting the number of spanning trees is the deletion–contraction strategy. This method is dependable for determining the number of spanning trees τ ( G ) in a multigraph G . This technique makes use of the fact that
τ ( G ) = τ ( G e ) + τ ( G / e )
where G e indicates the graph that is produced by deleting an arbitrary edge e , and G / e indicates the graph that is produced by contracting an arbitrary edge e [10,11]. Numerous works have focused on counting and maximizing the number of spanning trees for various graph families [12,13,14].
Kirchhoff’s interest in electrical networks stemmed from the possibility that an edge-weighted graph, whose weights represent the conductance of the associated edges, may be thought of as an electrical network. It is possible to express the effect conductance between two vertices u , v as the quotient of the (weighted) number of spanning trees and the (weighted) number of so-called thickets, which are spanning forests that have exactly two components and the characteristic that each component contains exactly one of the vertices u , v [15,16]. Below are the effects of several simple changes on the number of spanning trees. τ G is the weighted number of spanning trees. Let G be an edge weighted graph and H be its electrically equivalent graph.
  • Parallel edges: The count of spanning trees, τ ( H ) , stays the same when two parallel edges in G with conductances of x and y are combined to form a single edge in H with a conductance of x + y .
  • Serial edges:  τ ( H ) is equal to ( 1 / ( x + y ) times τ G if two serial edges in G with conductances x and y are linked to generate a single edge in H with a conductance x y / ( x + y ) .
  • Δ-Y transformation: The number of spanning trees in H , τ ( H ) , can be computed as ( xy + yz + z x ) 2 / x y z times τ ( G ) once a triangle in G with conductances x , y , and z is transformed into an electrically equivalent star graph in H with conductances u = ( xy + yz + z x ) / x , v = ( xy + yz + z x ) / y , and w = ( xy + yz + z x ) / z .
  • Y-Δ transformation is the process of converting a star graph in G with conductances x , y , and z into an electrically equivalent triangle in H with conductances u = y z / ( x + y + z ) , v = x z / ( ( x + y + z ) , and w = x y / ( ( x + y + z ) . The result τ ( H ) is given by 1 / ( ( x + y + z ) multiplied by τ ( G ) .

2. Main Results

The Fritsch graph has nine vertices and twenty-one edges, making it a maximum planar graph. It is isomorphic to the triaugmented triangular prism’s skeleton. The Fritsch graph plays a crucial role in demonstrating flaws in Kempe’s attempted proof of the four-color theorem. The graph is notable because it highlights how Kempe chains, used in the flawed proof, can interact in a way that invalidates the color swapping strategy.
Creating a new structure from an old one is always the aim in mathematics. Graphs are another area where this is true, as a given set of graphs can be used to create many new graphs. The number of spanning trees of three new forms of pyramidal graphs made from the Fritsch graph and two of their related graphs, represented by F r , F r ¯ and F r ¯ ¯ respectively, will be precisely determined in this work, as illustrated in Figure 1.

2.1. Number of Spanning Trees of Pyramid Graph F r n Created by Fritsch F r

The pyramid graph F r n is defined recursively using the graph F r 2 and the graph F r 1 (triangle or K 3 ) as follows: F r n ( n 3 ) is created by replacing the center triangle in F r n 1 with F r 2 . See Figure 2. According to this construction, the total vertices V ( F r n ) and edges E ( F r n ) are V ( F r n ) = 27 n 24 and E ( F r n ) = 78 n 75 , n = 1,2 , . The average degree of F r n is in the large n limit which is 5.8 .
Theorem 1.
The number of spanning trees in a pyramid graph, F r n , created by the Fritsch graph series for n 1 , is determined by
3 × 71221248 n 1 ×     628563359 + 25097 627267309   1296050 n 1       412155311 + 16565 627267309   + 1909     3155 627267309     628563359 + 25097 627267309 1296050   n 1     370187855 + 14656 627267309   + 47990351   2 × (   47081 2 + 392999919 3 209089103 2 25097 + 627267309   n 2 +   47081 2 392999919 3 209089103 2     25097 627267309 n 2 ) 2
Proof. 
By applying the electrically equivalent transformation, F r i is converted to F r i 1 . Figure 3 illustrates the process of converting F r 2 to F r 1 .
The result of combining these thirteen transformations is
τ F r 2 = x 2 3 9 9 2 x 2 + 1 6 × 7 9 × 4 x 2 + 3 3 × 5 9 × 4 x 2 + 1 x 2 3 × 7 3 9 7 × 4 x 2 + 3 2 x 2 + 1 2 × 207 35 9 × 2 x 2 + 1 2 12 x 2 + 11 4 x 2 + 1 4 x 2 + 3 3 × 648 161 3 × 72 2 x 2 + 1 2 4 x 2 + 3 12 x 2 + 11 × 276 x 2 + 253 9 757 x 2 + 646 × 3279 x 2 + 2862 276 x 2 + 253 3 × 252 757 x 2 + 646 23 1093 x 2 + 954 τ F r 1 .
Thus
τ ( F r 2 ) = 71221248 ( 25139 x 2 + 21942 ) 2 τ ( F r 1 ) .
Additionally
τ ( F r n ) = i = 2 n 71221248 ( 25139 x i + 21942 ) 2 τ ( F r 1 ) = 3 × 7122124 8 n 1 x 1 2 [   i = 2 n ( 25139 x i + 21942 ) ] 2
where x i 1 = 28252 x i + 24556 25139 x i + 21942 , i = 2,3 , . . . , n .
The equation for its characteristic is 25139 λ 2 6310 λ 24556 = 0 with roots λ 1 = 3155 627267309 25139 and λ 2 = 3155 + 627267309 25139 . These two roots can be subtracted from both sides of x i 1 = 28252 x i + 24556 25139 x i + 21942 , to obtain
x i 1 3155 627267309 25139 = 28252 x i + 24556 25139 x i + 21942 3155 627267309 25139 = ( 25097 + 627267309 ) [ x i 3155 627267309 25139 ] ( 25139 x i + 21942 )
x i 1 3155 + 627267309 25139 = 28252 x i + 24556 25139 x i + 21942 3155 + 627267309 25139 = ( 25097 627267309 ) [ x i 3155 + 627267309 25139 ] ( 25139 x i + 21942 )
Let y i = x i 3155 627267309 25139 x i 3155 + 627267309 25139 . Then by Equations (5) and (6), we get the following:
y i 1 = ( 628563359 + 25097 627267309 1296050 ) y i   and   y i = ( 628563359 + 25097 627267309 1296050 ) n i y n .
Therefore
x i = ( 628563359 + 25097 627267309 1296050 ) n i ( 3155 + 627267309 25139 ) y n 3155 627267309 25139 ( 628563359 + 25097 627267309 1296050 ) n i y n 1 .
Thus
x 1 = ( 628563359 + 25097 627267309 1296050 ) n 1 ( 3155 + 627267309 25139 ) y n 3155 627267309 25139 ( 628563359 + 25097 627267309 1296050 ) n 1 y n 1
With the coefficients of 28252 x n + 24556 and 25139 x n + 21942 , represented by the symbols α n and β n , respectively, and using the formula x i 1 = 28252 x i + 24556 25139 x i + 21942 , we have
25139 x n + 21942 = α 0 ( 28252 x n + 24556 ) + β 0 ( 25139 x n + 21942 ) ,
25139 x n 1 + 21942 = α 1 ( 28252 x n + 24556 ) + β 1 ( 25139 x n + 21942 ) α 0 ( 28252 x n + 24556 ) + β 0 ( 25139 x n + 21942 ) ,
25139 x n 2 + 21942 = α 2 ( 28252 x n + 24556 ) + β 2 ( 25139 x n + 21942 ) α 1 ( 28252 x n + 24556 ) + β 1 ( 25139 x n + 21942 ) ,
25139 x n i + 21942 = α i ( 28252 x n + 24556 ) + β i ( 25139 x n + 21942 ) α i 1 ( 28252 x n + 24556 ) + β i 1 ( 25139 x n + 21942 ) ,
25139 x n ( i + 1 ) + 21942 = α i + 1 ( 28252 x n + 24556 ) + β i + 1 ( 25139 x n + 21942 ) α i ( 28252 x n + 24556 ) + β i ( 25139 x n + 21942 ) ,
25139 x 2 + 21942 = α n 2 ( 28252 x n + 24556 ) + β n 2 ( 25139 x n + 21942 ) α n 3 ( 28252 x n + 24556 ) + β n 3 ( 25139 x n + 21942 )
When Equation (10) is substituted into Equation (4), we get
τ ( F r n ) = 3 × 7122124 8 n 1 x 1 2 [ α n 2 ( 28252 x n + 24556 ) + β n 2 ( 25139 x n + 21942 ) ] 2
where α 0 = 0 , β 0 = 1 and α 1 = 25139 , β 1 = 21942 . By the expression x i 1 = 28252 x i + 24556 25139 x i + 21942 and using Equations (8) and (9), we have
α i + 1 = 50194 α i 2592100 α i 1 ; β i + 1 = 50194 β i 2592100 β i 1
Equation (12) has the characteristic equation μ 2 50194 μ + 2592100 = 0 . Its roots are μ 1 = 25097 + 627267309 and μ 2 = 25097 627267309 .
The general solutions of Equation (12) are α i = h 1 μ 1 i + h 2 μ 2 i ; β i = k 1 μ 1 i + k 2 μ 2 i .
Given the initial conditions α 0 = 0 , β 0 = 1 and α 1 = 25139 , β 1 = 21942 , we obtain
α i = 25139 627267309 125454618 [ ( 25097 + 627267309 ) i ( 25097 627267309 ) i ] ; β i = ( 627267309 3155 627267309 125454618 ) ( 25097 + 627267309 ) i + ( 627267309 + 3155 627267309 125454618 ) ( 25097 627267309 ) i
If x n = 1 , this means that F r n is without any electrically equivalent transformation.
When Equation (13) is inserted into Equation (11), we obtain
τ F r n = 3 × x 1 2 × ( 71221248 ) n 1 [   47081 2 + 392999919 3 209089103 2 25097 + 627267309 n 2 + 47081 2 392999919 3 209089103 2 25097 627267309 n 2 ] 2 , n 2 .
Equation (14) is satisfied for n = 1 and τ ( F r 1 ) = 3 . Thus, the number of spanning trees in the pyramid graph F r n is determined by
τ F r n = 3 × x 1 2 × ( 71221248 ) n 1 [   47081 2 + 392999919 3 209089103 2 25097 + 627267309 n 2 + 47081 2 392999919 3 209089103 2 25097 627267309 n 2 ] 2 , n 1 .
where
x 1 = 628563359 + 25097 627267309 1296050 n 1       412155311 + 16565 627267309   + 1909     3155 627267309       628563359 + 25097 627267309 1296050   n 1     370187855 + 14656 627267309 + 47990351 , n 1
The result is obtained by inserting Equation (16) into Equation (15). □

2.2. Number of Spanning Trees of Pyramid Graph F r n ¯ Created by Related Fritsch Graph F r ¯

The pyramid graph F r n ¯ is defined recursively using the graph F r 2 ¯ and the graph F r 1 ¯ (triangle or K 3 ) as follows: F r n ¯   ( n 3 ) is created by replacing the center triangle in F r n 1 ¯ with F r 2 ¯ . See Figure 4. According to this construction, the total vertices V (   F r n ¯ ) and edges E (   F r n ¯ ) are V (   F r n ¯ ) = 30 n 27 and E (   F r n ¯ ) = 78 n 75 , n = 1,2 , . . . . The average degree of F r n ¯   is in the large n limit which is 5.2.
Theorem 2.
The number of spanning trees in a pyramid graph, F r n ¯ , created by the related Fritsch graph series F r ¯ for n 1 , is determined by
3 × ( 13589544960 ) n 1 ( ( 992209 + 997 990409 1800 ) n 1 ( 993209 + 1003 990409 ) 100 ( 28 + 990409 ) 7 ( 992209 + 997 990409 1800 ) n 1 ( 128987 + 129 990409 ) + 87500 ) 2 ( ( 950 + 135050 7 141487 ) ( 997 + 990409 ) n 2 + ( 950 135050 7 141487 ) ( 997 990409 ) n 2 ) 2
Proof. 
By applying the electrically equivalent transformation, F r i ¯ is converted to F r i 1 ¯ . Figure 5 illustrates the process of converting F r 2 ¯ to F r 1 ¯ .
The result of combining these ten transformations is
τ   F r 2 ¯ = 3 12 × 1 12 3 × 1 9 x 2 + 3 × 20 3 9 × 9 x 2 + 11 3 3 × 24 5 3 × 24 3 x 2 + 1 9 x 2 + 11 × 1 9 × 45 x 2 + 55 121 x 2 + 139 × 105 x 2 + 123 9 x 2 + 11 3 × 54 121 x 2 + 139 25 35 x 2 + 41 τ   F r 1 ¯ .
Thus
τ ( F r 2 ¯ ) = 13589544960 ( 875 x 2 + 1025 ) 2 τ ( F r 1 ¯ ) .
Additionally
τ ( F r n ¯ ) = i = 2 n 13589544960 ( 875 x i + 1025 ) 2 τ ( F r 1 ¯ ) = 3 × 1358954496 0 n 1 x 1 2 [ i = 2 n ( 875 x i + 1025 ) ] 2
where x i 1 = 969 x i + 1131 875 x i + 1025 , i = 2,3 , . . . , n .
This has a characteristic equation 875 λ 2 + 56 λ 1131 = 0 with the roots λ 1 = 28 990409 875 and λ 2 = 28 + 990409 875 . These two roots can be subtracted from both sides of x i 1 = 969 x i + 1131 875 x i + 1025 , to obtain
x i 1 + 28 + 990409 875 = 969 x i + 1131 875 x i + 1025 + 28 + 990409 875 = ( 997 + 990409 ) [ x i + 28 + 990409 875 ] ( 875 x i + 1025 )
x i 1 + 28 990409 875 = 969 x i + 1131 875 x i + 1025 + 28 990409 875 = ( 997 990409 ) [ x i + 28 990409 875 ] ( 875 x i + 1025 )
Let y i = x i + 28 + 990409 875 x i 28 990409 875 . Then by Equations (19) and (20), we get y i 1 = ( 992209 + 997 990409 1800 ) y i and y i = ( 992209 + 997 990409 1800 ) n i y n .
Therefore
x i = (   992209 + 997 990409 1800   ) n i   (   28 + 990409 875   )   y n + 28 + 990409 875 (   992209 + 997 990409 1800   ) n i y n 1
Thus
x 1 = (   992209 + 997 990409   1800   ) n 1   28 + 990409 875   y n + 28 + 990409 875 (   992209 + 997 990409 1800   ) n 1   y n 1
Using the formula x i 1 = 969 x i + 1131 875 x i + 1025 and designating the coefficients of 969 x n + 1131   a n d   875 x n + 1025 as α n and β n , we have
875 x n + 1025 = α 0 ( 969 x n + 1131 ) + β 0 ( 875 x n + 1025 ) ,
875 x n 1 + 1025 = α 1 ( 969 x n + 1131 ) + β 1 ( 875 x n + 1025 ) α 0 ( 969 x n + 1131 ) + β 0 ( 875 x n + 1025 ) ,
875 x n 2 + 1025 = α 2 ( 969 x n + 1131 ) + β 2 ( 875 x n + 1025 ) α 1 ( 969 x n + 1131 ) + β 1 ( 875 x n + 1025 ) ,
875 x n i + 1025 = α i ( 969 x n + 1131 ) + β i ( 875 x n + 1025 ) α i 1 ( 969 x n + 1131 ) + β i 1 ( 875 x n + 1025 ) ,
875 x n ( i + 1 ) + 1025 = α i + 1 ( 969 x n + 1131 ) + β i + 1 ( 875 x n + 1025 ) α i ( 969 x n + 1131 ) + β i ( 875 x n + 1025 )
875 x 2 + 1025 = α n 2 ( 969 x n + 1131 ) + β n 2 ( 875 x n + 1025 ) α n 3 ( 969 x n + 1131 ) + β n 3 ( 875 x n + 1025 ) .
When Equation (24) is substituted into Equation (18), we get
τ ( F r n ¯ ) = 3 × 1358954496 0 n 1 x 1 2 [ α n 2 ( 969 x n + 1131 ) + β n 2 ( 875 x n + 1025 ) ] 2
where α 0 = 0 , β 0 = 1 and α 1 = 875 , β 1 = 1025 . By the expression x n 1 = 969 x n + 1131 875 x n + 1025 and Equations (23) and (24), we have
α i + 1 = 1994 α i 3600 α i 1 ; β i + 1 = 1994 β i 3600 β i 1
Equation (26) has the characteristic equation μ 2 1994 μ + 3600 = 0 . Its roots are μ 1 = 997 + 990409 and μ 1 = 997 990409 .
The general solutions of Equation (26) are α i = h 1 μ 1 i + h 2 μ 2 i ; β i = k 1 μ 1 i + k 2 μ 2 i .
Given the initial conditions α 0 = 0 , β 0 = 1 and α 1 = 875 ,   β 1 = 1025 , we have
α i = 875 990409 1980818 [ ( 997 + 990409 ) i ( 997 990409 ) i ] ; β i = ( 990409 + 28 990409 1980818 ) ( 997 + 990409 ) i + ( 990409 28 990409 1980818 ) ( 997 990409 ) i
If x n = 1 , this means that F r n ¯ is without any electrically equivalent transformation.
When Equation (27) is inserted into Equation (25), we obtain the following:
τ F r n ¯ = 3 × x 1 2 × ( 13589544960   ) n 1   (   950 + 135050 7 141487     997 + 990409   n 2 + (   950 135050 7 141487   )   (   997 990409   ) n 2 ) 2 , n 2
Equation (28) is satisfied for n = 1 and τ ( F r 1 ¯ ) = 3 . Thus, the number of spanning trees in the pyramid graph F r n ¯ is determined by
τ F r n ¯ = 3 × x 1 2 × ( 13589544960 ) n 1 ( ( 950 + 135050 7 141487 )   997 + 990409 n 2 + 950 135050 7 141487 ( 997 990409 ) n 2 ) 2 , n 1
where
x 1 =   992209 + 997 990409 1800   n 1 993209 + 1003   990409   100   (   28 + 990409   ) 7   992209 + 997 990409 1800   n 1 (   128987 + 129 990409   ) + 87500 , n 1
The result is obtained by inserting Equation (30) into Equation (29). □

2.3. Number of Spanning Trees of Pyramid Graph F r n ¯ ¯ Created by Graph F r ¯ ¯

The pyramid graph F r n ¯ ¯ is defined recursively using the graph F r 2 ¯ ¯ and the graph F r 1 ¯ ¯ (triangle or K 3 ) as follows: F r n ¯ ¯ ( n 3 ) is created by replacing the center triangle in F r n 1 ¯ ¯ with F r 2 ¯ ¯ . See Figure 6. According to this construction, the total vertices V ( F r n ¯ ¯ ) and edges E ( F r n ¯ ¯ ) are V ( F r n ¯ ¯ ) = 39 n 36 and E ( F r n ¯ ¯ ) = 114 n 111 , n = 1,2 , . The average degree of F r n ¯ ¯ is in the large n limit which is 5.85 .
Theorem 3.
The number of spanning trees in a pyramid graph F r n ¯ ¯ , created by the related Fritsch graph series F r ¯ ¯ for n 1 , is determined by
3 × 106758347898180000 n 1   ( ( 2445697 + 1565 2442169 3528 n 1 ( 2237383 + 1531 2442169 ) + 558 ( 367 2442169 ) ) / ( 2445697 + 1565 2442169 3528 n 1 ( 1694449 + 973 2442169 ) + 747720 ) ) 2 ( ( 1269 2 + 1982457 2 2442169 ) ( 1565 + 2442169 2 ) n 2 + ( 1269 2 1982457 2 2442169 ) ( 1565 2442169 2 ) n 2 ) 2
Proof. 
By applying the electrically equivalent transformation, F r i ¯ ¯ is converted to F r i 1 ¯ ¯ . Figure 7 illustrates the process of converting F r 2 ¯ ¯ to F r 1 ¯ ¯ .
The result of combining these fifteen transformations is
τ ( F r 2 ¯ ¯ ) = 3 12 × 1 9 9 × x 2 3 ( 2 x 2 + 1 ) 6 × 7 9 × ( 4 x 2 + 3 ) 3 × ( 17 3 ) 9 × ( 14   x 2 + 3 3   x 2 ) 3 × ( 7 3 9 7 ) × ( 4   x 2 + 3 ) ( 2   x 2 + 1 ) 2 × ( 729 119 ) 9 × ( 3 ( 2 x 2 + 1 ) 2 ( 14 x 2 + 13 ) ( 4 x 2 + 3 ) ( 14   x 2 + 3 ) ) 3 × ( 30 7 ) 3 × ( 90 ( 2 x 2 + 1 ) 2 ( 4   x 2 + 3 ) ( 14   x 2 + 13 ) ) × ( 42 x 2 + 39 ) 9 ( 158   x 2 + 139 ) × ( 670 x 2 + 599 42   x 2 + 39 ) 3 × 6 ( 1106   x 2 + 973 ) ( 670   x 2 + 599 ) τ ( ) .
Thus
τ ( F r 2 ¯ ¯ ) = 1067583647898180000 ( 670 x 2 + 599 ) 2 τ ( F r 2 ¯ ¯ ) .
Additionally
τ F r n ¯ ¯ = i = 2 n 1067583647898180000 ( 670 x i + 599 ) 2 τ ( F r 1 ¯ ¯ ) = 3 × 106758364789818000 0 n 1 x 1 2 [ i = 2 n ( 670 x i + 599 ) ] 2
where x i 1 = 966 x i + 861 670 x i + 599 , i = 2,3 , , n . Its characteristic equation is 670 λ 2 367 λ 861 = 0 , with roots λ 1 = 367 2442169 1340 and λ 2 = 367 + 2442169 1340 . Subtracting these two roots on both sides of x i 1 = 966 x i + 861 670 x i + 599 , we get
x i 1 367 2442169 1340 = 966 x i + 861 670 x i + 599 367 2442169 1340 = 1565 + 2442169     [   x i 367 2442169 1340   ] 2 (   670 x i + 599   )
x i 1 367 + 2442169 1340 = 966 x i + 861 670 x i + 599 367 + 2442169 1340 =   1565 2442169     [   x i 367 + 2442169 1340   ] 2 ( 670 x i + 599   )
Let y i = x i 367 2442169 1340 x i 367 + 2442169 1340 .
Then by Equations (33) and (34), we get y i 1 = 2445697 + 1565 2442169 3528 y i and
y i = (   2445697 + 1565 2442169 3528   ) n i y n .
Therefore
x i = (   2445697 + 1565 2442169 3528   ) n i   367 + 2442169 1340     y n 367 2442169 1340 (   2445697 + 1565 2442169 3528   ) n i   y n 1 .
Thus
x 1 = (   2445697 + 1565 2442169 3528   ) n 1 (   367 + 2442169 1340   ) y n 367 2442169 1340 (   2445697 + 1565 2442169 3528   ) n 1 y n 1
Using the formula x i 1 = 966 x i + 861 670 x i + 599 and designating the coefficients of 966 x n + 861 and 670 x n + 599 as α n and β n , we have
670 x n + 599 = α 0 ( 966 x n + 861 ) + β 0 ( 670 x n + 599 ) ,
670 x n 1 + 599 = α 1 ( 966 x n + 861 ) + β 1 ( 670 x n + 599 ) α 0 ( 966 x n + 861 ) + β 0 ( 670 x n + 599 ) ,
670 x n 2 + 599 = α 2 ( 966 x n + 861 ) + β 2 ( 670 x n + 599 ) α 1 ( 966 x n + 861 ) + β 1 ( 670 x n + 599 ) ,
670 x n i + 599 = α i ( 966 x n + 861 ) + β i ( 670 x n + 599 ) α i 1 ( 966 x n + 861 ) + β i 1 ( 670 x n + 599 ) ,
670 x n ( i + 1 ) + 599 = α i + 1 ( 966 x n + 861 ) + β i + 1 ( 670 x n + 599 ) α i ( 966 x n + 861 ) + β i ( 670 x n + 599 ) ,
670 x 2 + 599 = α n 2 ( 966 x n + 861 ) + β n 2 ( 670 x n + 599 ) α n 3 ( 966 x n + 861 ) + β n 3 ( 670 x n + 599 ) .
When Equation (38) is substituted into Equation (32), we get
τ ( F r 2 ¯ ¯ ) = 3 × 106758364789818000 0 n 1 x 1 2 [ α n 2 ( 966 x n + 861 ) + β n 2 ( 670 x n + 599 ) ] 2
where α 0 = 0 , β 0 = 1 and α 1 = 670 , β 1 = 599 . By the expression x i 1 = 966 x i + 861 670 x i + 599 and Equations (36) and (37), we have
α i + 1 = 1565 α i 1764 α i 1 ;   β i + 1 = 1565 β i 1764 β i 1
Equation (40) has the characteristic equation μ 2 1565 μ + 1764 = 0 . Its roots are μ 1 = 1565 + 2442169 2 and μ 2 = 1565 2442169 2 .
The general solutions of Equation (40) are α i = h 1 μ 1 i + h 2 μ 2 i ; β i = k 1 μ 1 i + k 2 μ 2 i .
Given the initial conditions α 0 = 0 , β 0 = 1 and α 1 = 670 , β 1 = 599 , we have
α i = 670 2442169 2442169 [ ( 1565 + 2442169 2 ) i ( 1565 + 2442169 2 ) i ] ; β i = ( 2442169 367 2442169 4884338 ) ( 1565 + 2442169 2 ) i + (   2442169 + 367 2442169 4884338 ) ( 1565 2442169 2   ) i
If x n = 1 , this means that F r n ¯ ¯ is without any electrically equivalent transformation.
When Equation (41) is inserted into Equation (39), we obtain
τ F r n ¯ ¯ = 3 × x 1 2 × 106758347898180000 n 1 1269 2 + 1982457 2 2442169 1565 + 2442169 2 n 2 + 1269 2 1982457 2 2442169 1565 2442169 2 n 2 2 , n 2 .
Equation (42) is satisfied for n = 1 and τ F r n ¯ ¯ = 3 . Thus, the number of spanning trees in the sequence of the graph F r n ¯ ¯ is determined by
τ ( F r n ¯ ¯ ) = 3 × x 1 2 × 106758347898180000 n 1 ( 1269 2 + 1982457 2 2442169 1565 + 2442169 2 n 2 + 1269 2 1982457 2 2442169 1565 2442169 2 n 2 ) 2 , n 1
where
x 1 =   2445697 + 1565 2442169 3528   n 1   2237383 + 1531 2442169   + 558   367 2442169     2445697 + 1565 2442169   3528 n 1 (   1694449 + 973 2442169   ) + 747720
The result is obtained by inserting Equation (44) into Equation (43). □

3. Numerical Results

The values of the number of spanning trees in the graphs τ ( F r n ) , τ ( F r n ¯ ) , and τ ( F r n ¯ ¯ ) are shown in the following Table 1, Table 2 and Table 3:

4. Spanning Tree Entropy

Once we have exact formulas for the number of spanning trees of the three pyramid graphs, F r n , F r n   ¯ , and F r n ¯ ¯ , we can compute the spanning tree entropy Z, a finite number and an interesting metric defining the network topology. In [17,18], this is explained as follows: With reference to graph G ,
Z ( G ) = l i m n ln τ ( G ) V ( G ) .
Z ( F r n ) = 1 27 ln 71221248 + 2 ln 25097 + 627267309 = 1.47 ,
Z ( F r n   ¯ ) = 1 27 25 ln 2 + ln 405 + 2 ln 997 + 990409 = 1.43 ,
Z ( F r n ¯ ¯ ) = 1 39   ( l n [ 26689586974545000 ] + 2   l n [ 1565 + 2442169 ] ) = 1.38 .
Despite having the same number of vertices, edges, and average degree, the pyramid graph F r n has a higher entropy than the pyramid graph F r n   ¯ . Similarly, even though the pyramid graph F r n ¯ ¯ has more vertices, edges, and average degrees than the pyramid graphs F r n and F r n   ¯ , its entropy is lower. Additionally, the apollonian graph [19], which has an average degree of 5 (entropy 1.354), has a lower entropy than all pyramid graphs F r n , F r n   ¯ , and F r n ¯ ¯ .
The entropy of the graphs under investigation is also higher than that of the square grid graph, which has an average degree of 4 and an entropy of 1.166, and lower than that of the triangle grid graph, which has an average degree of 6 and an entropy of 1.62 [20].

5. Conclusions

In this study, we use electrically equivalent transformations to determine the number of spanning trees of particular pyramid graphs produced from the Fritsch graph and other related graphs. This technique’s strength is its ability to avoid the laborious computation of Laplacian spectra, which is a requirement for a general approach to spanning tree determination. Furthermore, our findings indicate a relationship between entropy and the graph’s average degree.

Author Contributions

Methodology, A.A. and S.N.D.; Software, A.A. and S.N.D.; Validation, A.A. and S.N.D.; Formal analysis, A.A. and S.N.D.; Investigation, A.A. and S.N.D.; Resources, A.A. and S.N.D.; Data curation, A.A. and S.N.D.; Writing—original draft, A.A. and S.N.D.; Writing—review & editing, A.A. and S.N.D.; Visualization, A.A. and S.N.D.; Supervision, A.A. and S.N.D.; Project administration, A.A. and S.N.D.; Funding acquisition, A.A. All authors have read and agreed to the published version of the manuscript.

Funding

The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work through Larg Groups (Project under grant number (RGP.2/372/45)).

Data Availability Statement

Data is contained within the article.

Acknowledgments

The authors wish to extend their gratitude to the anonymous referees for their valuable feedback, which significantly enhanced the quality of the manuscript.

Conflicts of Interest

The authors declare no conflicts of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript; or in the decision to publish the results.

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Figure 1. The Fritsch graph F r and two related graphs F r ¯ and F r ¯ ¯ .
Figure 1. The Fritsch graph F r and two related graphs F r ¯ and F r ¯ ¯ .
Axioms 14 00622 g001
Figure 2. The pyramid graph F r 2 .
Figure 2. The pyramid graph F r 2 .
Axioms 14 00622 g002
Figure 3. The electrically equivalent transformations from F r 2 to F r 1 . Utilizing the Δ-Y transformation rule on (a), we arrive at the following: τ ( H 1 ) = 9 9 2 x 2 + 1 6 x 2 3 τ ( F r 2 ) . Using the Y-Δ transformation rule on (b), we get τ ( H 2 ) = 1 7 9   ( 1 4 x 2 + 3 ) 3 τ ( H 1 ) . Reapplying the Y-Δ transformation rule on (c) yields the following: τ ( H 3 ) = 1 5 9 x 2 4 x 2 + 1 3 τ ( H 2 ) . When the parallel edge transformation rule is used on (d), we get τ ( H 4 ) = τ ( H 3 ) . When the Δ-Y transformation rule is applied on (e), we get τ ( H 5 ) = ( 9 7 7 3 ) ( 2 x 2 + 1 ) 2 ( 4 x 2 + 3 ) τ ( H 4 ) . Using the Y-Δ transformation rule on (f), we get τ ( H 6 ) = ( 35 207 ) 9 [ 4 x 2 + 1 4 x 2 + 3 2 x 2 + 1 2 12 x 2 + 11 ] 3 τ ( H 5 ) . Applying the parallel edge transformation rule on (g), we obtain the following: τ ( H 7 ) = τ ( H 6 ) . Utilizing the Y-Δ transformation rule on (h), we arrive at the following: τ ( H 8 ) = 161 648 3 4 x 2 + 3 12 x 2 + 11 72 2 x 2 + 1 2 τ ( H 7 ) . Applying the parallel edge transformation rule on (i), we obtain the following: τ ( H 9 ) = τ ( H 8 ) . Applying the Δ-Y transformation rule on (j), we obtain the following: τ ( H 10 ) = 9 ( 757 x 2 + 646 ) ( 276 x 2 + 253 ) τ ( H 9 ) . When we use the Y-Δ transformation rule on (k), we get τ ( H 11 ) = [   276 x 2 + 253 3279 x 2 + 2862   ] 3 τ ( H 10 ) . The parallel edge transformation rule is applied on (l), and we get τ ( H 12 ) = τ ( H 11 ) . Applying the Y-Δ transformation rule on (m),we obtain the following: τ ( H 13 ) = 23 ( 1093 x 2 + 954 ) 252 ( 757 x 2 + 646 ) τ ( H 12 ) . Applying the parallel edge transformation rule on (n), we obtain the following: τ ( F r 1 ) = τ ( H 14 ) .
Figure 3. The electrically equivalent transformations from F r 2 to F r 1 . Utilizing the Δ-Y transformation rule on (a), we arrive at the following: τ ( H 1 ) = 9 9 2 x 2 + 1 6 x 2 3 τ ( F r 2 ) . Using the Y-Δ transformation rule on (b), we get τ ( H 2 ) = 1 7 9   ( 1 4 x 2 + 3 ) 3 τ ( H 1 ) . Reapplying the Y-Δ transformation rule on (c) yields the following: τ ( H 3 ) = 1 5 9 x 2 4 x 2 + 1 3 τ ( H 2 ) . When the parallel edge transformation rule is used on (d), we get τ ( H 4 ) = τ ( H 3 ) . When the Δ-Y transformation rule is applied on (e), we get τ ( H 5 ) = ( 9 7 7 3 ) ( 2 x 2 + 1 ) 2 ( 4 x 2 + 3 ) τ ( H 4 ) . Using the Y-Δ transformation rule on (f), we get τ ( H 6 ) = ( 35 207 ) 9 [ 4 x 2 + 1 4 x 2 + 3 2 x 2 + 1 2 12 x 2 + 11 ] 3 τ ( H 5 ) . Applying the parallel edge transformation rule on (g), we obtain the following: τ ( H 7 ) = τ ( H 6 ) . Utilizing the Y-Δ transformation rule on (h), we arrive at the following: τ ( H 8 ) = 161 648 3 4 x 2 + 3 12 x 2 + 11 72 2 x 2 + 1 2 τ ( H 7 ) . Applying the parallel edge transformation rule on (i), we obtain the following: τ ( H 9 ) = τ ( H 8 ) . Applying the Δ-Y transformation rule on (j), we obtain the following: τ ( H 10 ) = 9 ( 757 x 2 + 646 ) ( 276 x 2 + 253 ) τ ( H 9 ) . When we use the Y-Δ transformation rule on (k), we get τ ( H 11 ) = [   276 x 2 + 253 3279 x 2 + 2862   ] 3 τ ( H 10 ) . The parallel edge transformation rule is applied on (l), and we get τ ( H 12 ) = τ ( H 11 ) . Applying the Y-Δ transformation rule on (m),we obtain the following: τ ( H 13 ) = 23 ( 1093 x 2 + 954 ) 252 ( 757 x 2 + 646 ) τ ( H 12 ) . Applying the parallel edge transformation rule on (n), we obtain the following: τ ( F r 1 ) = τ ( H 14 ) .
Axioms 14 00622 g003aAxioms 14 00622 g003bAxioms 14 00622 g003cAxioms 14 00622 g003dAxioms 14 00622 g003eAxioms 14 00622 g003fAxioms 14 00622 g003gAxioms 14 00622 g003h
Figure 4. The pyramid graph F r 2 ¯ .
Figure 4. The pyramid graph F r 2 ¯ .
Axioms 14 00622 g004
Figure 5. The electrically equivalent transformations from F r 2 ¯ to F r 1 ¯ . Utilizing the Y-Δ transformation method on (a), we arrive at τ ( H 1 ) = 1 3 12   τ ( F r 2 ¯ ) . Applying the parallel edge transformation rule on (b), we obtain the following: τ ( H 2 ) = τ ( H 1 ) . Using the Δ-Y transformation rule on (c), we get the following: τ ( H 3 ) = ( 12 ) 3 ( 9 x 2 + 3 ) τ ( H 2 ) . Applying the Y-Δ transformation rule on (d), we obtain the following: τ ( H 4 ) = ( 3 20 ) 9 ( 3 9 x 2 + 11 ) 3 τ ( H 3 ) . Applying the parallel edge transformation rule on (e), we obtain the following: τ ( H 5 ) = τ ( H 4 ) . Applying the Δ-Y transformation rule on (f), we obtain the following: τ ( H 6 ) = ( 5 24 ) 3 ( 9 x 2 + 11 ) 24 ( 3 x 2 + 1 ) τ ( H 5 ) . Applying the parallel edge transformation rule on (g), we obtain the following: τ ( H 7 ) = τ ( H 6 ) . Utilizing the Δ-Y transformation rule on (h), we arrive at the following: τ ( H 8 ) = 9 ( 121 x 2 + 139 ) ( 45 x 2 + 55 ) τ ( H 7 ) . Applying the Y-Δ transformation rule on (i), we obtain the following: τ ( H 9 ) = ( 9 x 2 + 11 105 x 2 + 123 ) 3   τ ( H 8 ) . Applying the parallel edge transformation rule on (j), we obtain the following: τ ( H 10 ) = τ ( H 9 ) . Utilizing the Y-Δ transformation rule on (k), we arrive at the following: τ ( H 11 ) = 25 ( 35 x 2 + 41 ) 54 ( 121 x 2 + 139 ) τ ( H 10 ) . By using the transformation rule for parallel edges on (l), we get the following: τ ( F r 1 ¯ ) = τ ( H 11 ) .
Figure 5. The electrically equivalent transformations from F r 2 ¯ to F r 1 ¯ . Utilizing the Y-Δ transformation method on (a), we arrive at τ ( H 1 ) = 1 3 12   τ ( F r 2 ¯ ) . Applying the parallel edge transformation rule on (b), we obtain the following: τ ( H 2 ) = τ ( H 1 ) . Using the Δ-Y transformation rule on (c), we get the following: τ ( H 3 ) = ( 12 ) 3 ( 9 x 2 + 3 ) τ ( H 2 ) . Applying the Y-Δ transformation rule on (d), we obtain the following: τ ( H 4 ) = ( 3 20 ) 9 ( 3 9 x 2 + 11 ) 3 τ ( H 3 ) . Applying the parallel edge transformation rule on (e), we obtain the following: τ ( H 5 ) = τ ( H 4 ) . Applying the Δ-Y transformation rule on (f), we obtain the following: τ ( H 6 ) = ( 5 24 ) 3 ( 9 x 2 + 11 ) 24 ( 3 x 2 + 1 ) τ ( H 5 ) . Applying the parallel edge transformation rule on (g), we obtain the following: τ ( H 7 ) = τ ( H 6 ) . Utilizing the Δ-Y transformation rule on (h), we arrive at the following: τ ( H 8 ) = 9 ( 121 x 2 + 139 ) ( 45 x 2 + 55 ) τ ( H 7 ) . Applying the Y-Δ transformation rule on (i), we obtain the following: τ ( H 9 ) = ( 9 x 2 + 11 105 x 2 + 123 ) 3   τ ( H 8 ) . Applying the parallel edge transformation rule on (j), we obtain the following: τ ( H 10 ) = τ ( H 9 ) . Utilizing the Y-Δ transformation rule on (k), we arrive at the following: τ ( H 11 ) = 25 ( 35 x 2 + 41 ) 54 ( 121 x 2 + 139 ) τ ( H 10 ) . By using the transformation rule for parallel edges on (l), we get the following: τ ( F r 1 ¯ ) = τ ( H 11 ) .
Axioms 14 00622 g005aAxioms 14 00622 g005bAxioms 14 00622 g005cAxioms 14 00622 g005dAxioms 14 00622 g005eAxioms 14 00622 g005f
Figure 6. The pyramid graph F r 2 ¯ ¯ .
Figure 6. The pyramid graph F r 2 ¯ ¯ .
Axioms 14 00622 g006
Figure 7. The electrically equivalent transformations from F r 2 ¯ ¯ to F r 1 ¯ ¯ . Applying the Y-Δ transformation rule on (a), we obtain the following: τ ( H 1 ) = 1 3 12 τ ( F r 2 ¯ ¯ ) . Applying the parallel edge transformation rule on (b), we obtain the following: τ ( H 2 ) = τ ( H 1 ) . Applying the Δ-Y transformation rule on (c), we obtain the following: τ ( H 3 ) = 9 9 ( 2 x 2 + 1 ) 6 x 2 3 τ ( H 2 ) . Applying the Y-Δ transformation rule on (d), we obtain the following: τ ( H 4 ) = ( 1 7 ) 9 ( 1 4 x 2 + 3 ) 3 τ ( H 3 ) . Reapplying the Y-Δ transformation rule on (e) yields the following: τ ( H 5 ) = ( 3 17 ) 9 ( 3 x 2 14 x 2 + 3 ) 3 τ ( H 4 ) . Applying the parallel edge transformation rule on (f), we obtain the following:   τ ( H 6 ) = τ ( H 5 ) . Utilizing the Δ-Y transformation rule on (g), we arrive at the following: τ ( H 7 ) = ( 9 7 7 3 ) ( 2 x 2 + 1 ) 2 ( 4 x 2 + 3 ) τ ( H 6 ) . Applying the Y-Δ transformation rule on (h), we obtain the following: τ ( H 8 ) = ( 119 729 ) 9 ( ( 4 x 2 + 3 ) ( 14 x 2 + 3 ) 3 ( 2 x 2 + 1 ) 2 ( 14 x 2 + 13 ) ) 3   τ ( H 7 ) . Applying the parallel edge transformation rule on (i), we obtain the following: τ ( H 9 ) = τ ( H 8 ) . When we use the Y-Δ transformation rule on (j), we get the following: τ ( H 10 ) = ( 7 30 ) 3 ( 4 x 2 + 3 ) ( 14 x 2 + 13 ) 90 ( 2 x 2 + 1 ) 2 τ ( H 9 ) . Using the rule of parallel edge transformation on (k), we get the following: τ ( H 11 ) = τ ( H 10 ) . When we use the Δ-Y transformation rule on (l), we get the following: τ ( H 12 ) = 9 ( 158 x 2 + 139 ) ( 42 x 2 + 39 ) τ ( H 11 ) . Applying the Y-Δ transformation rule on (m), we obtain the following: τ ( H 13 ) = ( 42 x 2 + 39 670 x 2 + 599 ) 3 τ ( H 12 ) . Applying the parallel edge transformation rule on (n), we obtain the following:   τ ( H 14 ) = τ ( H 13 ) . Applying the Y-Δ transformation rule on (o), we obtain the following: τ ( H 15 ) = ( 670 x 2 + 599 ) 6 ( 1106 x 2 + 973 ) τ ( H 14 ) . Applying the parallel edge transformation rule on (p), we obtain the following: τ ( F r 1 ¯ ¯ ) = τ ( H 15 ) .
Figure 7. The electrically equivalent transformations from F r 2 ¯ ¯ to F r 1 ¯ ¯ . Applying the Y-Δ transformation rule on (a), we obtain the following: τ ( H 1 ) = 1 3 12 τ ( F r 2 ¯ ¯ ) . Applying the parallel edge transformation rule on (b), we obtain the following: τ ( H 2 ) = τ ( H 1 ) . Applying the Δ-Y transformation rule on (c), we obtain the following: τ ( H 3 ) = 9 9 ( 2 x 2 + 1 ) 6 x 2 3 τ ( H 2 ) . Applying the Y-Δ transformation rule on (d), we obtain the following: τ ( H 4 ) = ( 1 7 ) 9 ( 1 4 x 2 + 3 ) 3 τ ( H 3 ) . Reapplying the Y-Δ transformation rule on (e) yields the following: τ ( H 5 ) = ( 3 17 ) 9 ( 3 x 2 14 x 2 + 3 ) 3 τ ( H 4 ) . Applying the parallel edge transformation rule on (f), we obtain the following:   τ ( H 6 ) = τ ( H 5 ) . Utilizing the Δ-Y transformation rule on (g), we arrive at the following: τ ( H 7 ) = ( 9 7 7 3 ) ( 2 x 2 + 1 ) 2 ( 4 x 2 + 3 ) τ ( H 6 ) . Applying the Y-Δ transformation rule on (h), we obtain the following: τ ( H 8 ) = ( 119 729 ) 9 ( ( 4 x 2 + 3 ) ( 14 x 2 + 3 ) 3 ( 2 x 2 + 1 ) 2 ( 14 x 2 + 13 ) ) 3   τ ( H 7 ) . Applying the parallel edge transformation rule on (i), we obtain the following: τ ( H 9 ) = τ ( H 8 ) . When we use the Y-Δ transformation rule on (j), we get the following: τ ( H 10 ) = ( 7 30 ) 3 ( 4 x 2 + 3 ) ( 14 x 2 + 13 ) 90 ( 2 x 2 + 1 ) 2 τ ( H 9 ) . Using the rule of parallel edge transformation on (k), we get the following: τ ( H 11 ) = τ ( H 10 ) . When we use the Δ-Y transformation rule on (l), we get the following: τ ( H 12 ) = 9 ( 158 x 2 + 139 ) ( 42 x 2 + 39 ) τ ( H 11 ) . Applying the Y-Δ transformation rule on (m), we obtain the following: τ ( H 13 ) = ( 42 x 2 + 39 670 x 2 + 599 ) 3 τ ( H 12 ) . Applying the parallel edge transformation rule on (n), we obtain the following:   τ ( H 14 ) = τ ( H 13 ) . Applying the Y-Δ transformation rule on (o), we obtain the following: τ ( H 15 ) = ( 670 x 2 + 599 ) 6 ( 1106 x 2 + 973 ) τ ( H 14 ) . Applying the parallel edge transformation rule on (p), we obtain the following: τ ( F r 1 ¯ ¯ ) = τ ( H 15 ) .
Axioms 14 00622 g007aAxioms 14 00622 g007bAxioms 14 00622 g007cAxioms 14 00622 g007dAxioms 14 00622 g007eAxioms 14 00622 g007fAxioms 14 00622 g007gAxioms 14 00622 g007hAxioms 14 00622 g007iAxioms 14 00622 g007j
Table 1. This table shows some of the numbers for the pyramid graph F r n spanning tree count.
Table 1. This table shows some of the numbers for the pyramid graph F r n spanning tree count.
n τ ( F r n )
13
2595840848878370816
3106707180749521149279206454746677248
419107851727493992841163289907951233946454397491871744
53421606268097367048895726265969595422130168100899195236894586523615232
Table 2. This table shows some of the numbers for the pyramid graph F r n   ¯ spanning tree count.
Table 2. This table shows some of the numbers for the pyramid graph F r n   ¯ spanning tree count.
n τ ( F r n ¯ )
13
2179789679820800000
39697793127051120495361523712000000
4523046936889575576192567454766298592675102720000000
528210343478816088618974934925711446742498999448683259573043200000000
Table 3. This table shows some of the numbers for the pyramid graph F r n ¯ ¯   spanning tree count.
Table 3. This table shows some of the numbers for the pyramid graph F r n ¯ ¯   spanning tree count.
n τ ( F r n ¯ ¯ )
13
21069055356324272207660000
3279186674647567005563231690975473914913200000000
472895214842904525037897880850154069102870750125233146218424000000000000
519032826541987370547012520501914939903996473462422852589142424061545049132730080000000000000000
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Asiri, A.; Daoud, S.N. The Complexity of Classes of Pyramid Graphs Based on the Fritsch Graph and Its Related Graphs. Axioms 2025, 14, 622. https://doi.org/10.3390/axioms14080622

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Asiri A, Daoud SN. The Complexity of Classes of Pyramid Graphs Based on the Fritsch Graph and Its Related Graphs. Axioms. 2025; 14(8):622. https://doi.org/10.3390/axioms14080622

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Asiri, Ahmad, and Salama Nagy Daoud. 2025. "The Complexity of Classes of Pyramid Graphs Based on the Fritsch Graph and Its Related Graphs" Axioms 14, no. 8: 622. https://doi.org/10.3390/axioms14080622

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Asiri, A., & Daoud, S. N. (2025). The Complexity of Classes of Pyramid Graphs Based on the Fritsch Graph and Its Related Graphs. Axioms, 14(8), 622. https://doi.org/10.3390/axioms14080622

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