I can understand the height analogy for voltage but what would be a
similar analogy for current which also explains the above question?
I'll try a different approach.
Assume you have a resistor of resistance $1\, \Omega$ connected across an ideal cell that maintains $1\, \mathrm{V}$ across its terminals.
The voltage across the resistor is thus $1\, \mathrm{V}$ and so, the current through the resistor is, by Ohm's law, $1\, \mathrm{A}$.
Now, replace the $1\,\mathrm{V}$ cell with a $3\,\mathrm{V}$ cell.
The voltage across the resistor is thus $3\, \mathrm{V}$ and so, the current through the resistor is, by Ohm's law, $3\, \mathrm{A}$.
Assuming you have no problem with the above, take the next step and replace the $3\,\mathrm{V}$ cell with a $3\,\mathrm{V}$ battery consisting of three $1\,\mathrm{V}$ cells in series.
Since the voltage across the resistor is still $3\, \mathrm{V}$, the current through the resistor is still $3\, \mathrm{A}$.
So you see, the current increases when you place cells in series for the same reason the current increases when you use a cell with a larger voltage - the larger voltage across the same resistance produces a larger current.