2-group symmetries arise in physics when a 0-form symmetry G[0] and a 1-form symmetry H[1] intertwine, forming a generalised group-like structure. Specialising to the case where both G[0] and H[1] are compact, connected, abelian groups (i.e. tori), we analyse anomalies in such ‘toric 2-group symmetries’ using the cobordism classification. As a warm up example, we use cobordism to study various ’t Hooft anomalies (and the phases to which they are dual) in Maxwell theory defined on non-spin manifolds. For our main example, we compute the 5th spin bordism group of B|\U0001d53e| where \U0001d53e is any 2-group whose 0-form and 1-form symmetry parts are both U(1), and |\U0001d53e| is the geometric realisation of the nerve of the 2-group \U0001d53e. By leveraging a variety of algebraic methods, we show that {varOmega}_5^{textrm{Spin}}left(Bleft|mathbbm{G}right|right)cong mathbb{Z}/m where m is the modulus of the Postnikov class for \U0001d53e, and we reproduce the expected physics result for anomalies in 2-group symmetries that appear in 4d QED. Moving down two dimensions, we recap that any (anomalous) U(1) global symmetry in 2d can be enhanced to a toric 2-group symmetry, before showing that its associated local anomaly reduces to at most an order 2 anomaly, when the theory is defined with a spin structure.