If coordinate axes are the angle bisectors of the pair of lines
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Let's consider an easier case, when the given lines have the form y=mxy=mx and y=nxy=nx (with m≠nm≠n, of course).
The points on the angle bisectors satisfy the conditions that their distance from the two lines is the same. So you have, for such a point (x,y)(x,y),
|y−mx|1+m2−−−−−−√=|y−nx|1+n2−−−−−√|y−mx|1+m2=|y−nx|1+n2
By squaring, we get
(y−mx)2(1+n2)=(y−nx)2(1+m2)(y−mx)2(1+n2)=(y−nx)2(1+m2)
and expanding
(y−mx)2−(y−nx)2=m2(y−nx)2−n2(y−mx)2.(y−mx)2−(y−nx)2=m2(y−nx)2−n2(y−mx)2.
The left hand side becomes
(y−mx+y−nx)(y−mx−y+nx)=−(m−n)(2y−(m+n)x)x(y−mx+y−nx)(y−mx−y+nx)=−(m−n)(2y−(m+n)x)x
and the right hand side is
(my−mnx+ny−mnx)(my−mnx−ny+mnx)=(m−n)((m+n)y−2mnx)y(my−mnx+ny−mnx)(my−mnx−ny+mnx)=(m−n)((m+n)y−2mnx)y
Since m≠nm≠n, we can factor out m−nm−non both sides, getting
−2xy+(m+n)x2=(m+n)y2−2mnxy−2xy+(m+n)x2=(m+n)y2−2mnxy
that can be written
(m+n)x2−2(1−mn)xy−(m+n)y2=0(m+n)x2−2(1−mn)xy−(m+n)y2=0
If you consider the equation by2+2hxy+ax2=0by2+2hxy+ax2=0 in the unknown yy, you can see that mm and nn are the roots of it (when b≠0b≠0). Thus m+n=−2h/bm+n=−2h/b and mn=a/bmn=a/b, so you can rewrite the above equation in the form
−2hbx2−2(1−ab)xy−−2hby2=0−2hbx2−2(1−ab)xy−−2hby2=0
which is
hx2−(a−b)xy−hy2=0hx2−(a−b)xy−hy2=0
Note that it can't be both h=0h=0 and a=b≠0a=b≠0, because in this case the original equations would be x2+y2=0x2+y2=0(the isotropic lines, if you consider the complex plane).
The points on the angle bisectors satisfy the conditions that their distance from the two lines is the same. So you have, for such a point (x,y)(x,y),
|y−mx|1+m2−−−−−−√=|y−nx|1+n2−−−−−√|y−mx|1+m2=|y−nx|1+n2
By squaring, we get
(y−mx)2(1+n2)=(y−nx)2(1+m2)(y−mx)2(1+n2)=(y−nx)2(1+m2)
and expanding
(y−mx)2−(y−nx)2=m2(y−nx)2−n2(y−mx)2.(y−mx)2−(y−nx)2=m2(y−nx)2−n2(y−mx)2.
The left hand side becomes
(y−mx+y−nx)(y−mx−y+nx)=−(m−n)(2y−(m+n)x)x(y−mx+y−nx)(y−mx−y+nx)=−(m−n)(2y−(m+n)x)x
and the right hand side is
(my−mnx+ny−mnx)(my−mnx−ny+mnx)=(m−n)((m+n)y−2mnx)y(my−mnx+ny−mnx)(my−mnx−ny+mnx)=(m−n)((m+n)y−2mnx)y
Since m≠nm≠n, we can factor out m−nm−non both sides, getting
−2xy+(m+n)x2=(m+n)y2−2mnxy−2xy+(m+n)x2=(m+n)y2−2mnxy
that can be written
(m+n)x2−2(1−mn)xy−(m+n)y2=0(m+n)x2−2(1−mn)xy−(m+n)y2=0
If you consider the equation by2+2hxy+ax2=0by2+2hxy+ax2=0 in the unknown yy, you can see that mm and nn are the roots of it (when b≠0b≠0). Thus m+n=−2h/bm+n=−2h/b and mn=a/bmn=a/b, so you can rewrite the above equation in the form
−2hbx2−2(1−ab)xy−−2hby2=0−2hbx2−2(1−ab)xy−−2hby2=0
which is
hx2−(a−b)xy−hy2=0hx2−(a−b)xy−hy2=0
Note that it can't be both h=0h=0 and a=b≠0a=b≠0, because in this case the original equations would be x2+y2=0x2+y2=0(the isotropic lines, if you consider the complex plane).
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