Partial trace is not cyclic, unlike the normal trace, which can be demonstrated through examples and definitions. The partial trace operates only on a specific subsystem of a larger quantum system, leading to different results when the order of matrices is swapped. A common example involves the density matrix of an entangled state, where the partial trace over one subsystem yields a reduced density matrix. The discussion seeks a proof for the equality Tr_B(ρσ) = Tr_B(σρ) for density matrices ρ and σ in a bipartite system. Understanding the non-cyclic nature of the partial trace is crucial for quantum mechanics applications.