At least when $X$ and $Y$ are separable and metrizable, one can relate the support of a measure and the pullback of the support of the pushforward. We'll use the following (see Parthasarathy's Probability Measures on Metric Spaces, pp.27-28, Thm.2.1):
Theorem: Let $X$ be a separable metrizable space. Then for any Borel probability measure $\mu$ on $X$, its support $\text{supp}(\mu)$ is defined by any one of the following statements:
- $\text{supp}(\mu)=\bigcap\{F\subseteq X \,|\, F\text{ is closed and } \mu(X\setminus F)=0\}$.
- $\text{supp}(\mu)= \{x\in X\,|\, \forall U\in\text{Nbhd}(x):\mu(U)>0\}$.
- $\mu(\text{supp}(\mu))=1$ and for any closed subset $F\subseteq X$ with $\mu(F)=1$, $\text{supp}(\mu)\subseteq F$.
Next let $X,Y$ be separable and metrizable, $f:X\to Y$ be Borel measurable. Let $\mu$ be a Borel probability measure on $X$ and denote by $f_\ast(\mu)$ the pushforward of $\mu$ by $f$. $f^{-1}(\text{supp}(f_\ast(\mu)))$ is Borel measurable and has $\mu$-measure $1$; consequently we have
$$\text{supp}(\mu)\subseteq \overline{f^{-1}\left(\text{supp}(f_\ast(\mu))\right)}$$
(so that $f^{-1}\left(\text{supp}(f_\ast(\mu))\right)$ is dense in $\text{supp}(\mu)$, similar to the linked discussion). Interpreted differently, we also have that all three of the sets
$$\text{supp}(\mu),\quad f^{-1}\left(\text{supp}(f_\ast(\mu))\right),\quad \overline{f^{-1}\left(\text{supp}(f_\ast(\mu))\right)}$$
represent the same element of the measure algebra of $X$ w/r/t $\mu$ (see my answer at Why do we write $P\ll Q$ and why is $P$ called absolutely continuous w.r.t. $Q$?).