06.09.2021 Views

College Trigonometry, 2011a

College Trigonometry, 2011a

College Trigonometry, 2011a

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

1038 Applications of <strong>Trigonometry</strong><br />

and Q(1,m 1 + b 1 ). We let ⃗v 1 = −→ PQ = 〈1 − 0, (m1 + b 1 ) − b 1 〉 = 〈1,m 1 〉, and note that since ⃗v 1 is<br />

determined by two points on L 1 , it may be viewed as lying on L 1 . Hence it has the same direction<br />

as L 1 . Similarly, we get the vector ⃗v 2 = 〈1,m 2 〉 which has the same direction as the line L 2 . Hence,<br />

L 1 and L 2 are perpendicular if and only if ⃗v 1 ⊥ ⃗v 2 . According to Theorem 11.25, ⃗v 1 ⊥ ⃗v 2 if and<br />

only if ⃗v 1 · ⃗v 2 = 0. Notice that ⃗v 1 · ⃗v 2 = 〈1,m 1 〉·〈1,m 2 〉 =1+m 1 m 2 . Hence, ⃗v 1 · ⃗v 2 = 0 if and only<br />

if 1 + m 1 m 2 = 0, which is true if and only if m 1 m 2 = −1, as required.<br />

While Theorem 11.25 certainly gives us some insight into what the dot product means geometrically,<br />

there is more to the story of the dot product. Consider the two nonzero vectors ⃗v and ⃗w drawn<br />

with a common initial point O below. For the moment, assume that the angle between ⃗v and ⃗w,<br />

which we’ll denote θ, is acute. We wish to develop a formula for the vector ⃗p, indicated below,<br />

which is called the orthogonal projection of ⃗v onto ⃗w. The vector ⃗p is obtained geometrically<br />

as follows: drop a perpendicular from the terminal point T of ⃗v to the vector ⃗w and call the point<br />

of intersection R. The vector ⃗p is then defined as ⃗p = −→ OR. Like any vector, ⃗p is determined by its<br />

magnitude ‖⃗p‖ and its direction ˆp accordingtotheformula⃗p = ‖⃗p‖ˆp. Since we want ˆp to have the<br />

same direction as ⃗w, wehaveˆp = ŵ. To determine ‖⃗p‖, we make use of Theorem 10.4 as applied<br />

to the right triangle △ORT. We find cos(θ) = ‖⃗p‖<br />

‖⃗v‖<br />

,or‖⃗p‖ = ‖⃗v‖ cos(θ). To get things in terms of<br />

‖⃗v‖‖ ⃗w‖ cos(θ) ⃗v· ⃗w<br />

just ⃗v and ⃗w, we use Theorem 11.23 to get ‖⃗p‖ = ‖⃗v‖ cos(θ) =<br />

‖ ⃗w‖<br />

=<br />

‖ ⃗w‖<br />

. Using Theorem<br />

( )<br />

⃗v· ⃗w<br />

11.22, werewrite<br />

‖ ⃗w‖ = ⃗v · 1<br />

‖ ⃗w‖ ⃗w = ⃗v · ŵ. Hence, ‖⃗p‖ = ⃗v · ŵ, and since ˆp = ŵ, wenowhavea<br />

formula for ⃗p completely in terms of ⃗v and ⃗w, namely ⃗p = ‖⃗p‖ˆp =(⃗v · ŵ)ŵ.<br />

⃗v<br />

⃗v<br />

T<br />

T<br />

⃗w<br />

⃗w<br />

‖⃗v‖<br />

O<br />

θ<br />

O<br />

θ<br />

⃗p = −→ OR<br />

R<br />

O<br />

θ<br />

‖⃗p‖<br />

R<br />

Now suppose that the angle θ between ⃗v and ⃗w is obtuse, and consider the diagram below. In this<br />

case, we see that ˆp = −ŵ and using the triangle △ORT, we find ‖⃗p‖ = ‖⃗v‖ cos(θ ′ ). Since θ+θ ′ = π,<br />

it follows that cos(θ ′ )=− cos(θ), which means ‖⃗p‖ = ‖⃗v‖ cos(θ ′ )=−‖⃗v‖ cos(θ). Rewriting this<br />

last equation in terms of ⃗v and ⃗w as before, we get ‖⃗p‖ = −(⃗v · ŵ). Putting this together with<br />

ˆp = −ŵ, weget⃗p = ‖⃗p‖ˆp = −(⃗v · ŵ)(−ŵ) =(⃗v · ŵ)ŵ in this case as well.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!