Moose352 said:
Hmm, how did you end up with the formula for the area? Thanks again. I figured out that I was making a stupid mistake differentiating, and I managed to find the answer that way too. But your way is a lot nicer.
And halls, AOB i guess means the portion of the parabola.
Moose
:) I imagine the problem would get
very ugly if you didn't have that formula.
I can't remember the derivation, but the determinant of the cross product of two vectors gives the area of the parallelogram formed by those two vectors (of course, those vectors would be 2 of the 4 sides, but you should get the idea). The area of the triangle would just be half the area of that parallelogram. I'm at work right now, so I can't really try to figure out a derivation, but if you can't find one online I'll try to provide one (although I'm sure someone here will do that before I get a chance).
EDIT: Ignore most of the stuff above. I was a bit rusty with this stuff, so I looked it up on mathworld where their notation confused me, so what I wrote didn't make perfect sense. It's not the determinant of the cross product, but the magnitude of it which gives you the area of the parallelogram. If you have vectors \vec{u} = (u_x, u_y) and \vec{v} = (v_x, v_y) then the area of the parallelogram is:
A = |\vec{u} \times \vec{v}| = \det \left[\begin{array}{cc}u_x&u_y\\v_x&v_y\end{array}\right]
Now, how do we prove this?
Well, |\vec{u} \times \vec{v}| = |\vec{u}||\vec{v}|\sin \theta, where \theta is the angle between the vectors. Now, it's not hard to see that if the absolute value of the cross product is what's given on the right, that we have the area of the parallelogram. If |\vec{u}| represents the base of the parallelogram, we can see with some trigonometry that |\vec{v}|\sin \theta is the height/altitude of the parallelogram, and clearly the product of these two values is the area. Now, how do we know that the equation at the start of this paragraph is true? Well, I suppose it would be messy, but you'd just have to show that:
u_xv_y - v_xu_y = |\vec{u}||\vec{v}|\sin \theta
You can use the fact that:
\sin \theta = \sqrt{1 - \cos ^2 \theta} = \sqrt{1 - \left (\frac{\vec{u} \cdot \vec{v}}{|\vec{u}||\vec{v}|} \right )}