There are several different definitions of the barbell graph.
Most commonly and in this work, the -barbell graph is the simple graph obtained by connecting two copies of a complete graph
by a bridge (Ghosh et al. 2006, Herbster and Pontil 2006). The 3-barbell graph is isomorphic to the kayak paddle graph
.
Precomputed properties of barbell graphs are available in the Wolfram Language as GraphData["Barbell", n
].
Barbell graphs are geodetic. The -barbell graph is ungraceful from
up to at least
(E. Weisstein, Sep. 19, 2025) and likely for all larger
.
By definition, the -barbell graph has cycle polynomial is given by
| (1) |
where is the cycle polynomial of the complete graph
. Its graph circumference is therefore
.
The -barbell graph has chromatic polynomial and independence polynomial
| (2) | |||
| (3) |
and the latter has recurrence equation
| (4) |
Wilf (1989) adopts the alternate barbell convention by defining the -barbell graph to consist of two copies of
connected by an
-path.
Northrup (2002) calls the graphs obtained by joining bridges on either side of a 2-path graph "barbell graphs." This version might perhaps be better called a "double flower graph."