Step 1: Treat segment BC as a cantilever loaded at its free end B.
Cut the beam at B. Everything that segment AB does to segment BC can be replaced by the force $P$ and the moment it creates at B, transferred from A:
\[ M_B = P \times L_1 = 30 \times 100 = 3000 \text{ N-mm} \]
So segment BC (length $L_2$, stiffness $EI_2$, fixed at C) is a cantilever carrying an end force $P$ and an end moment $M_B$ at its tip B.
Step 2: Find the deflection and slope this produces at B.
Using standard cantilever tip formulas,
\[ \delta_B = \frac{PL_2^3}{3EI_2} + \frac{M_B L_2^2}{2EI_2}, \qquad \theta_B = \frac{PL_2^2}{2EI_2} + \frac{M_B L_2}{EI_2} \]
With $E=200{,}000$ N/mm$^2$, $I_2=700$ mm$^4$, $L_2=100$ mm:
\[ \delta_B = \frac{30(100)^3}{3(200000)(700)} + \frac{3000(100)^2}{2(200000)(700)} = 0.0714 + 0.1071 = 0.1786 \text{ mm} \]
\[ \theta_B = \frac{30(100)^2}{2(200000)(700)} + \frac{3000(100)}{(200000)(700)} = 0.001071 + 0.002143 = 0.003214 \text{ rad} \]
Step 3: Add the contribution of segment AB, treating B as its (moving) support.
Segment AB is itself a cantilever of length $L_1$, stiffness $EI_1$, carrying $P$ at its own free tip A. Its own bending adds a deflection of A relative to B,
\[ \delta_{AB} = \frac{PL_1^3}{3EI_1} = \frac{30(100)^3}{3(200000)(100)} = 0.5 \text{ mm} \]
Also, because B itself rotates by $\theta_B$, the rigid segment AB tips over by that same angle, carrying point A sideways by an extra
\[ \theta_B \times L_1 = 0.003214 \times 100 = 0.3214 \text{ mm} \]
Step 4: Add up every contribution at A.
\[ \delta_A = \delta_B + \theta_B L_1 + \delta_{AB} = 0.1786 + 0.3214 + 0.5 \]
Final Answer:
\[ \boxed{\delta_A = 1.0 \text{ mm}} \]