If $|z|^2+\bar{A}z^2+A(\bar{z})^2+B\bar{z}+\bar{B}z+c=0$ represents a pair of intersecting lines with angle of intersection $'\theta'$ then find the value of |A|.
I tried using general equation of straight line in complex form as $a\bar{z}+\bar{a}z+b=0$ where b is real,where slope of line is $\frac{-a}{\bar{a}}$ and multiplying two such lines and then compairing coefficient.I found that c is real and used $$\tan(\theta)=\big|\left(\frac{\text{slope}_1-\text{slope}_2}{1+\text{slope}_1*\text{slope}_2}\right)\big|$$
one thought was also that the use of $|z_1+z_2|^2=(z_1+z_2)(\bar{z_1}+\bar{z_2})=|z_1|^2+|z_2|^2+\bf{z_1\bar{z_2}+z_2\bar{z_1}}$
But this is becoming very long and I think this is also not much effective and there should be some good way, is there a better way out ?
If the given equation defines two intersecting lines then we can translate them such that they intersect at the origin. (Replace $z$ in the equation by $z+p+iq$, and determine $p$ and $q$ such that there are no linear terms in $z$, $\bar z$ appearing. The constant term will then automatically be zero, or we would not have two lines.)
The new equation is $$z\bar z+\bar A z^2+A\bar z^2=0,\qquad A=a\, e^{i\alpha}\ne0\ .\tag{1}$$ The map $$T:\quad{\mathbb C}\to{\mathbb C}, \qquad z\mapsto w=e^{-i\alpha/2}\, z$$ is a rotation. It moves the two lines into the $w$-plane without changing the angle of the intersection. The equation there is obtained from $(1)$ by letting $z:=e^{i\alpha/2}\,w$, hence is $$w\bar w+a(w^2+\bar w^2)=0\ .$$ With $w=u+iv$ this means $(u^2+v^2)+2a(u^2-v^2)=0$, or $$v=\pm\sqrt{{2a+1\over2a-1}}\>u\ .$$ These are two lines symmetric to the $u$-axis. It follows that $$\tau:=\tan{\theta\over2}=\sqrt{{2a+1\over2a-1}}\ ,$$ so that $$\cos\theta={1-\tau^2\over1+\tau^2}=-{1\over2a}\ .$$ This implies $$|A|=a=-{1\over2\cos\theta}={1\over2\cos\theta'}\ ,$$ where $\theta'$ is the angle $<{\pi\over2}$ between the two lines.