Let the temperature of the contact surface be \( T \).
The heat current through plate A is equal to the heat current through plate B in the steady state:
\[
K_A A \frac{(T_A - T)}{L} = K_B A \frac{(T - T_B)}{L},
\]
where \( K_A \) and \( K_B \) are the thermal conductivities, \( T_A = 100^\circ \text{C} \), \( T_B = 0^\circ \text{C} \), and \( L \) is the thickness.
Substitute the given values:
\[
84 \cdot (100 - T) = 126 \cdot (T - 0).
\]
Simplify:
\[
8400 - 84T = 126T.
\]
Rearrange:
\[
8400 = 210T.
\]
Solve for \( T \):
\[
T = \frac{8400}{210} = 40^\circ \text{C}.
\]
Thus, the temperature of the contact surface is \( \boxed{40^\circ \text{C}} \).