00:01
Any vector u can be decomposed into a horizontal piece and a vertical piece.
00:09
When the length of our vector equals 1, we know that this vertical piece is sine theta, and the horizontal piece is cosine theta.
00:22
So if v vector v has magnitude 1, this identity holds, well, when our vector is u not equal to 1, then this is equal to u, then this is equal to u times v.
00:50
So this piece here will be u times sine of theta, and this horizontal piece will be u times cosine theta.
01:04
So we can write any vector u as the sum of the horizontal component, u, cosine, theta, times v1, where v1 is just the horizontal component or horizontal factor 1 -0...