Conic Sections
I don't understand when Spivak says (see the picture)
we can make things a lot simpler for ourselves if we rotate everything so that this intersection line points straight out from the plane of the paper, while the first axis is in the usual position that we are familiar with. The plane $P$ is thus viewed “straight on,” ...
Can someone please clarify it? How does he exactly rotate things to get that view?
