Let the charge on sphere A and B be \( Q_A \) and \( Q_B \), respectively. The formula for the charge distribution when two spheres are connected by a conducting wire is given by:
\[
\frac{Q_A}{r_A} = \frac{Q_B}{r_B}
\]
where \( r_A \) and \( r_B \) are the radii of the spheres, and \( Q_A \) and \( Q_B \) are the charges on the spheres. Given the radius values for the spheres:
\[
r_A = 8 \, \text{cm}, \quad r_B = 10 \, \text{cm}
\]
We can substitute these values into the charge distribution equation:
\[
\frac{90}{8} = \frac{Q_B}{10}
\]
Solving for \( Q_B \):
\[
Q_B = \frac{90 \times 10}{8} = 112.5 \, \mu C
\]
The charge on sphere B after they are connected will be \( 112.5 \, \mu C \), and the charge on sphere A will be \( 90 \, \mu C \). The total charge after redistribution remains the same. Therefore, the charge transferred from sphere A to sphere B is:
\[
\Delta Q = Q_B - 90 = 112.5 - 102.5 = 10 \, \mu C
\]
Thus, the charge flowing from sphere A to sphere B is \( 10 \, \mu C \).