I just finished a question that I thought was pretty cool so I thought I might give you guys a go.
Prove mathematically that if the speed of a moving particle moving along a curve is constant, the acceleration is perpendicular to the velocity.
The topic is vector calculus if you want a clue.


=\frac{d}{dt}(k^2))
Assuming

is defined in
\times x(t)+y(t)\times y(t)+z(t)\times z(t)\right]=x(t)\times \frac{dx}{dt}+\frac{dx}{dt}\times x(t)+y(t)\times \frac{dy}{dt}+\frac{dy}{dt}\times y(t) +z(t)\times \frac{dz}{dt}+\frac{dz}{dt}\times z(t))
(product rule)
=\left(\frac{dx}{dt},\frac{dy}{dt},\frac{dz}{dt}\right)\cdot \left(x(t),y(t),z(t)\right) + \left(x(t),y(t),z(t)\right) \cdot\left(\frac{dx}{dt},\frac{dy}{dt},\frac{dz}{dt}\right))
(this can be shown for n-dimensions)
=\frac{d\vec{v}}{dt}\cdot\vec{v}+\vec{v}\cdot \frac{d\vec{v}}{dt}})
(basically, the product rule)



, given that neither

nor

are
0hence, in general, where the magnitude of velocity is a constant, acceleration is perpendicular to the direction of motion
EDIT: and for dcc's sake, this holds true where velocity is defined and continuous (and in this case, its magnitude is also constant)