We theoretically propose how to observe topological effects in a generic
classical system of coupled harmonic oscillators, such as classical pendula or
lumped-element electric circuits, whose oscillation frequency is modulated fast
in time. Making use of Floquet theory in the high frequency limit, we identify
a regime in which the system is accurately described by a Harper-Hofstadter
model where the synthetic magnetic field can be externally tuned via the phase
of the frequency-modulation of the different oscillators. We illustrate how the
topologically-protected chiral edge states, as well as the Hofstadter butterfly
of bulk bands, can be observed in the driven-dissipative steady state under a
monochromatic drive. In analogy with the integer quantum Hall effect, we show
how the topological Chern numbers of the bands can be extracted from the mean
transverse shift of the steady-state oscillation amplitude distribution.
Finally we discuss the regime where the analogy with the Harper-Hofstadter
model breaks down.Comment: 15 pages, 9 figure