Isospectral flows are abundant in mathematical physics; the rigid body, the the Toda lattice, the Brockett flow, the Heisenberg spin chain, and point vortex dynamics, to mention but a few. Their connection on the one hand with integrable systems and, on the other, with Lie-Poisson systems motivates the research for optimal numerical schemes to solve them. Several works about numerical methods to integrate isospectral flows have produced a large varieties of solutions to this problem. However, many of these algorithms are not intrinsically defined in the space where the equations take place and/or rely on computationally heavy transformations. In the literature, only few examples of numerical methods avoiding these issues are known, for instance, the spherical midpoint method on so(3). In this paper we introduce a new minimalvariable, second order, numerical integrator for isospectral flows intrinsically defined on quadratic Lie algebras and symmetric matrices. The algorithm is isospectral for general isospectral flows and Lie-Poisson preserving when the isospectral flow is Hamiltonian. The simplicity of the scheme, together with its structure-preserving properties, makes it a competitive alternative to those already present in literature. isospectral flow and Lie-Poisson integrator and symplectic Runge-Kutta methods and generalized rigid body and Brockett flow and Heisenberg spin chain and Point-vortex on the hyperbolic plane 1 In view of [11, Sec. I.8], there is no restriction in looking at real matrix Lie algebras, since the complex ones can be seen as real matrix Lie algebras of double dimension.