Note that the potential of galvanic/electrolytic cell electrodes is relative to each other. They can be both positive or both negative wrt the potential of the standard hydrogen electrode (SHE), taken conventionally as 0.00 V potential reference. And the SHE has potential $\pu{+4.44 \pm 0.02 V}$ wrt the potential of a free electron.
Therefore, the "positive" electrode, contact or potential means being more positive than the "negative" one.
The electrolytic cell can be considered as a power source with the open circuit voltage $U_\text{cell}$ and internal resistance $R_\text{cell}$. The external source similarly is the combination of a voltage source $U_\text{src}$ with the internal resistance $R_\text{src}$.
Case 1 - The "Positive" contact of the voltage source is connected to the "positive" contact of the electrolytic cell. The source has higher voltage than the cell.
The current flows to the more positive electrode contact, electrons flow from it and this more positive electrode is the anode. The current $$I = \frac{U_\text{src} - U_\text{cell} }{ R_\text{src} + R_\text{cell}}$$
The voltage on the contacts is then
$$U_\text{cont} = \frac{ U_\text{src} R_\text{cell} + U_\text{cell} R_\text{src} } { R_\text{src} + R_\text{cell}} $$
The contact with the more positive potential is then obviously at the more positive contacts of both the source and the cell.
Case 2 - The "Positive" contact of the voltage source is connected to the "positive" contact of the electrolytic cell. The source has lower voltage than the cell.
The formulas above still stand, but there is the opposite direction of the current. The measured voltage on contacts is lower than the voltage of the cell at the open circuit, but higher than the voltage of the source at the open circuit. The cell works in the galvanic mode instead and the positive electrode is the cathode now.
Case 3 - The "Positive" contact of the voltage source is connected to the "negative" contact of the electrolytic cell.
In this case, we have two power sources, connected in a series, the cell working in the galvanic mode.
The current $$I = \frac{U_\text{src} + U_\text{cell} }{ R_\text{src} + R_\text{cell}}$$
The potential of the nominally "positive" electrode of the cell wrt to its nominally "negative" is:
$$U_\text{cont} = \frac{ U_\text{cell} R_\text{src} - U_\text{src} R_\text{cell}} { R_\text{src} + R_\text{cell}} ,$$
and can be both positive and negative. As in the case 2, the cell works in the galvanic mode and the nominally "positive" electrode is the cathode now.
Note that this mode may lead to very high currents and potentially to damage or destruction of the source or the cell.