A famous example is the Ehrenfest process, introduced in 1911 by the physicists Paul Ehrenfest and Tatyana Ehrenfest-Afanaseva as a toy model to explain the macroscopic irreversibility of some microscopically reversible dynamics. The process is defined as follows.
Start with a hypercube $K=\{0,1\}^I$ of dimension $n$, thus $I$ can be any set of size $n$. The simple random walk $(X_t)_{t\geqslant0}$ on the graph with vertex set $K$ and the usual edge set is a Markov chain, such that, for every $t\geqslant0$, all the coordinates of $X_{t+1}$ are those of $X_t$ except one, and the exception is chosen randomly uniformly in $I$.
Now, let $S_t$ count the number of ones amongst the coordinates of $X_t$. The surprising fact is that $(S_t)_{t\geqslant0}$ is also a Markov chain (and more precisely, a birth-and-death chain). This new chain is defined on the set $L=\{0,1,\ldots,n\}$ and has transition probabilities, for every $i$ in $L$,
$$
Q(i,i-1)=i/n=1-Q(i,i+1).
$$
The funny thing is that $S_t=u(X_t)$ for the non injective function $u:K\to L$ one can imagine, and that, as said above, $(S_t)_{t\geqslant0}$ is still a Markov chain although, in general, such a non injective lumping of a Markov chain does not produce a Markov chain but rather what is called a hidden Markov chain.
A sufficient condition on any lumping to produce a Markov chain, which the Markov process $(X_t)_{t\geqslant0}$ on $K$ and the Ehrenfest function $u$ from $K$ to $L$ happen to satisfy, is well known. Call $q$ the transition matrix of $(X_t)_{t\geqslant0}$. Then, the sufficient condition is that the sum
$$
\sigma(x,s)=\sum\limits_{y:u(y)=s}q(x,y)
$$
depends on $u(x)$ and $s$ only, but not on $x$. In other words, one asks that $\sigma(x,s)=\sigma(x',s)$ as soon as $u(x)=u(x')$. Then $(S_t)_{t\geqslant0}$ is a Markov chain whose transition matrix $Q$ is defined by $Q(r,s)=\sigma(x,s)$ for any $r$ and $s$ and any $x$ such that $u(x)=r$.