We study a hybrid impulsive reaction-advection-diffusion model given by a reaction-advection-diffusion equation composed with a discrete-time map in space dimension n ∈ N. The reaction-advection-diffusion equation takes the form ut(m)=div(A∇u(m)-qu(m))+f(u(m))for (x,t) ∈ Rn×(0,1], for some function f, a drift q and a diffusion matrix A. When the discrete-time map is local in space we use Nm(x) to denote the density of population at a point x at the beginning of reproductive season in the mth year and when the map is nonlocal we use um(x). The local discrete-time map is {u(m)(x,0)=g(Nm(x))for x ∈ Rn,Nm+1(x):=u(m)(x,1)for x ∈ Rn, for some function g. The nonlocal discrete time map is {u(m)(x,0)=um(x)for x ∈ Rn,um+1(x) := g(∫RnK(x-y)u(m)(y,1)dy) for x ∈ Rn, when K is a nonnegative normalized kernel. Here, we analyze the above model from a variety of perspectives so as to understand the phenomenon of propagation. We provide explicit formulas for the spreading speed of propagation in any direction e \in Rn. Due to the structure of the model, we apply a simultaneous analysis of the differential equation and the recurrence relation to establish the existence of traveling wave solutions. The remarkable point is that the roots of spreading speed formulas, as a function of drift, are exactly the values that yield blow-up for the critical domain dimensions, just as with the classical Fisher's equation with advection. We provide applications of our main results to impulsive reaction-advection-diffusion models describing periodically reproducing populations subject to climate change, insect populations in a stream environment with yearly reproduction, and grass growing logistically in the savannah with asymmetric seed dispersal and impacted by periodic fires. [ABSTRACT FROM AUTHOR]