  We investigate the quench dynamics of quasi-one and two dimensional dipolar
Bose-Einstein condensates (dBEC) of $^{164}$Dy atoms under the influence of a
fast rotating magnetic field. The magnetic field thus controls both the
magnitude and sign of the dipolar potential. We account for quantum
fluctuations, critical to formation of exotic quantum droplet and supersolid
phases in the extended Gross-Pitaevskii formalism, which includes the so-called
Lee-Huang-Yang (LHY) correction. An analytical variational ansatz allows us to
obtain the phase diagrams of the superfluid and droplet phases. The crossover
from the superfluid to the supersolid phase and to single and droplet arrays is
probed with particle number and dipolar interaction. The dipolar strength is
tuned by rotating the magnetic field with subsequent effects on phase
boundaries. Following interaction quenches across the aforementioned phases, we
monitor the dynamical formation of supersolid clusters or droplet lattices. We
include losses due to three-body recombination over the crossover regime, where
the three-body recombination rate coefficient scales with the fourth power of
the scattering length ($a_s$) or the dipole length ($a_{dd}$). For fixed values
of the dimensionless parameter, $\epsilon_{dd} = a_{dd}/a_s$, tuning the
dipolar anisotropy leads to an enhancement of the droplet lifetimes.
