Let σgph := (E) be the usual signature for graphs. a. Extend the signature to a larger signature σ so that the σ -structures correspond to 3-coloured graphs, i.e., graphs whose each vertex is assigned one of the three colours represented as {0,1,2}. (You cannot add a function symbol whose interpretation in a structure with underlying set V is a function V → {0, 1, 2} (the function symbols’s interpretations always have codomain V ).) b. Define a σ-theory whose models are precisely the properly 3-coloured graphs, i.e. 3-coloured graphs in which no two adjacent vertices have the same colour
Let σgph := (E) be the usual signature for graphs. a. Extend the signature to a larger signature σ so that the σ -structures correspond to 3-coloured graphs, i.e., graphs whose each vertex is assigned one of the three colours represented as {0,1,2}. (You cannot add a function symbol whose interpretation in a structure with underlying set V is a function V → {0, 1, 2} (the function symbols’s interpretations always have codomain V ).) b. Define a σ-theory whose models are precisely the properly 3-coloured graphs, i.e. 3-coloured graphs in which no two adjacent vertices have the same colour
Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
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Let σgph := (E) be the usual signature for graphs.
a. Extend the signature to a larger signature σ so that the σ -structures correspond to 3-coloured graphs, i.e., graphs whose each vertex is assigned one of the three colours represented as {0,1,2}.
(You cannot add a function symbol whose interpretation in a structure with underlying set V is a function V → {0, 1, 2} (the function symbols’s interpretations always have codomain V ).)
b. Define a σ-theory whose models are precisely the properly 3-coloured graphs, i.e. 3-coloured graphs in which no two adjacent vertices have the same colour.
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