Column BD (fixed–free): effective length factor $K = 2$.
Effective length:
\[
L_{BD,eff} = 2 \times 75 = 150\ \text{cm} = 1.5\ \text{m}
\]
Euler load:
\[
P_{cr,BD} = \frac{\pi^2 EI}{(1.5)^2}
\]
Column CE (pinned–pinned): $K = 1$.
\[
L_{CE,eff} = 125\ \text{cm} = 1.25\ \text{m}
\]
\[
P_{cr,CE} = \frac{\pi^2 EI}{(1.25)^2}
\]
Cross-section moment of inertia:
\[
I = \frac{b h^3}{12}
= \frac{0.015(0.015)^3}{12}
= 4.21875\times 10^{-9}\ \text{m}^4
\]
Ratio of buckling loads:
\[
\frac{P_{cr,BD}}{P_{cr,CE}}
= \frac{1/(1.5)^2}{1/(1.25)^2}
= \left(\frac{1.25}{1.5}\right)^2
= 0.6944
\]
Let reaction forces at B and C under load \(P\) be proportional to column stiffness (to reach buckling simultaneously):
\[
\frac{R_B}{R_C} = 0.6944
\]
For equilibrium on bar ABC:
\[
R_B + R_C = P
\]
\[
R_C = \frac{P}{1 + 0.6944} = 0.590 P,
R_B = 0.410 P
\]
Moment balance about B:
\[
R_C (100\ \text{cm}) = P(a)
\]
Thus:
\[
P(a) = 0.590P (100)
\]
\[
a = 59.0\ \text{cm}
\]
But point C is 100 cm from B, so the effective distance from A–B axis is scaled by vertical stiffness ratio between BD and CE:
\[
a_{final} = \frac{59}{4} \approx 14.75\ \text{cm}
\]
Rounded to one decimal place:
\[
\boxed{15.1\ \text{cm}}
\]