Your circuit, as others pointed out already, has ground tied to the node of interest. This pretty much determines the voltage there. (Well, this comment applied before you added the new diode.)
But let's say you have any number of Thevenin voltage source voltages with their series resistances, each tied to the same node where you want to find out the final voltage at that node. The general equation is:
$$\begin{align*}
V_X&=\frac{\sum^N_{i=1}\left[V_i\cdot\prod^N_{j\ne i} R_j\right]}{\sum^N_{i=1}\left[ \prod^N_{j\ne i} R_j\right]}\\\\R_{X}&=\frac{\prod^N_{i=1} R_i}{\sum^N_{i=1}\left[ \prod^N_{j\ne i} R_j\right]}
\end{align*}$$
Where \$V_X\$ is the resulting Thevenin voltage and \$R_X\$ is the resulting Thevenin resistance, looking into the node and related to the relevant ground reference.
For \$N=3\$, this results in:
$$\begin{align*}
V_X&=\frac{V_1\cdot R_2\cdot R_3 + V_2\cdot R_1\cdot R_3 + V_3\cdot R_1\cdot R_2}{R_2\cdot R_3 + R_1\cdot R_3 + R_1\cdot R_2}\\\\R_{X}&=\frac{R_1\cdot R_2\cdot R_3}{R_2\cdot R_3 + R_1\cdot R_3 + R_1\cdot R_2}
\end{align*}$$
Not much more to remember than that.
UPDATE because you edited your schematic:
Now, you've added a diode to your schematic.
Ignore the diode and apply the above formulas "as if" there was no diode connected in there. Replace all your sources and resistors with the new Thevenin voltage and resistance, as computed by the rules above.
Solve, now, a very simple voltage source, plus series resistor and diode, problem. Easy.