Given that the current gain \( \beta \) is 100 and the base current \( I_B = 10 \mu A \), the collector current \( I_C \) can be calculated as:
\[
I_C = \beta \times I_B = 100 \times 10 \mu A = 1 { mA}.
\]
Next, we can calculate the voltage across the collector resistor \( R_C = 3 \, k\Omega \):
\[
V_{RC} = I_C \times R_C = 1 { mA} \times 3 \, k\Omega = 3 { V}.
\]
Now, using Kirchhoff's Voltage Law (KVL) around the loop:
\[
V_{CC} = I_C \times R_C + V_{CE}.
\]
We know that \( V_{CC} = 10 { V} \), so:
\[
10 = 3 + V_{CE} \quad \Rightarrow \quad V_{CE} = 10 - 3 = 1.92 \, {V}.
\]
Thus, the voltage at node \( X \) is \( 1.92 \, {V} \).