Given:
Moment of inertia of beam, \( I = 8 \times 10^7 \, {mm}^4 \)
Modulus of elasticity of steel, \( E = 210 \times 10^3 \, {N/mm}^2 \)
UDL, \( w = 6.25 \, {kN/m} = 6.25 \, {N/mm} \) (including self-weight)
Axial force in CD, \( P_1 = ? \)
Flexural rigidity, \( EI = 210 \times 10^3 \times 8 \times 10^7 = 1.68 \times 10^{13} \, {N-mm}^2 = 16800 \, {kNm}^2 \)
Due to symmetry, we have:
\[
\Delta_{EF} = \Delta_{AB} \quad {and} \quad \Delta_{CD} \neq \Delta_{EF}
\]
From equilibrium:
\[
2P_2 + P_1 = 6.25 \times 40
\]
\[
2P_2 + P_1 = 25 \, {kN}
\]
Solving for \( P_2 \):
\[
P_2 = \frac{25 - P_1}{2} = 12.5 - 0.5 P_1
\]
The net elongation of rod CD is given by:
\[
\Delta_{CD \, {net}} = \frac{P_1 \times 1}{\frac{\pi}{4} (0.03)^2 \times 210 \times 10^6} + \frac{0.5 \times 4 \times 12.5}{\frac{\pi}{4} (0.012)^2 \times 210 \times 10^6}
\]
Substitute the values:
\[
\Delta_{CD \, {net}} = 2.77 \times 10^{-5} P_1 - 5.26 \times 10^{-4}
\]
Now, for the deflection of the beam at point D:
\[
\Delta_{{beam}} = \frac{5 w l^4}{384 EI} - \frac{P_1 l^3}{48 EI}
\]
Substitute the values for \( w = 6.25 \, {kN/m} \) and \( l = 2 \, {m} \):
\[
\Delta_{{beam}} = \frac{4^3}{48 \times 16800} \left( 5 \times 6.25 \times 4 - P_1 \right)
\]
Finally, solving for the axial force in Rod CD:
\[
\Delta_{{CD \, net}} = \Delta_{{beam}} = \frac{4^3}{48 \times 16800} \left( 5 \times 6.25 \times 4 - P_1 \right)
\]
After solving, we find:
\[
P_1 = 16.48 \, {kN}
\]
Thus, the axial force in rod CD is \( P_1 = 16.48 \, {kN} \).