For a spherical shell, the electric field outside the shell at a distance \( r \) from the center is given by the formula:
\[
E = \frac{kQ}{r^2}
\]
where \( Q \) is the total charge on the shell, and \( k \) is Coulomb's constant.
At a distance \( 3R \) from the center, the electric field due to each shell is the same as if the entire charge were concentrated at the center of the shell. Therefore, the electric fields due to shells A, B, and C at a distance \( 3R \) are given by:
\[
E_A = \frac{k(6q)}{(3R)^2} = \frac{k(6q)}{9R^2}
\]
\[
E_B = \frac{k(-4q)}{(3R)^2} = \frac{k(-4q)}{9R^2}
\]
\[
E_C = \frac{k(14q)}{(3R)^2} = \frac{k(14q)}{9R^2}
\]
Thus, the magnitude of the electric fields is:
\[
|E_A| = \frac{6kq}{9R^2}, \quad |E_B| = \frac{4kq}{9R^2}, \quad |E_C| = \frac{14kq}{9R^2}
\]
The electric field due to shell C is the largest, followed by shell A, and then shell B.