The equation can't be nomogrammed, at least not in its current form. I found Kellog's two necessary criteria for nomogramability; $F$ fails the second test. Informally, there are just too many independent terms. Technically, a certain wronksian determinant fails to vanish.
First, we choose one of the variables to isolate—here, $b$—and we rewrite $$F(a,b,c) = \left(1\right)b^2 + (-2c)\,b^1 + [(c^2+kc)−ka]\, 1 = 0.$$ In other words, we have written:
$$F(a,b,c) = J_1(a,c)f_1(b) + J_2(a,c) f_2(b) + J_3(a,c)f_3(b)$$
where the $J_i$ are linearly independent of each other (note they each contain a $c$ term of different degree) and the $f_i$ are linearly independent of each other (note they each contain a $b$ term of different degree.)
Kellogg's second criterion is that, if we look at the non-isolated variables $a$ and $c$, the following wronskian determinants must vanish:
$$\det \begin{bmatrix}J_1 & J_2 & J_3 \\ \partial_aJ_1 & \partial_aJ_2 & \partial_aJ_3 \\ \partial_{aa}J_1 & \partial_{aa}J_2 & \partial_{aa}J_3\end{bmatrix} = 0$$
$$\det \begin{bmatrix}J_1 & J_2 & J_3 \\ \partial_cJ_1 & \partial_cJ_2 & \partial_cJ_3 \\ \partial_{cc}J_1 & \partial_{cc}J_2 & \partial_{cc}J_3\end{bmatrix} = 0.$$
Unfortunately, for the second wronksian, we get:
$$\det \begin{bmatrix}J_1 & J_2 & J_3 \\ \partial_cJ_1 & \partial_cJ_2 & \partial_cJ_3 \\ \partial_{cc}J_1 & \partial_{cc}J_2 & \partial_{cc}J_3\end{bmatrix} = \det \begin{bmatrix}1 & -2c & (c^2+kc)-ka \\ 0 & -2 & 2c + k \\ 0 & 0 & 2\end{bmatrix} = -4 \neq 0.$$
(All but one term in the determinant vanishes; the one on the main diagonal.)