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College Trigonometry, 2011a

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11.8 Vectors 1019<br />

The remaining properties are proved similarly and are left as exercises.<br />

Our next example demonstrates how Theorem 11.19 allows us to do the same kind of algebraic<br />

manipulations with vectors as we do with variables – multiplication and division of vectors notwithstanding.<br />

If the pedantry seems familiar, it should. This is the same treatment we gave Example<br />

8.3.1 in Section 8.3. As in that example, we spell out the solution in excruciating detail to encourage<br />

the reader to think carefully about why each step is justified.<br />

Example 11.8.3. Solve 5⃗v − 2(⃗v + 〈1, −2〉) =⃗0 for⃗v.<br />

Solution.<br />

5⃗v − 2(⃗v + 〈1, −2〉) = ⃗0<br />

5⃗v +(−1) [2 (⃗v + 〈1, −2〉)] = ⃗0<br />

5⃗v +[(−1)(2)] (⃗v + 〈1, −2〉) = ⃗0<br />

5⃗v +(−2) (⃗v + 〈1, −2〉) = ⃗0<br />

5⃗v +[(−2)⃗v +(−2) 〈1, −2〉] = ⃗0<br />

5⃗v +[(−2)⃗v + 〈(−2)(1), (−2)(−2)〉] = ⃗0<br />

[5⃗v +(−2)⃗v]+〈−2, 4〉 = ⃗0<br />

(5 + (−2))⃗v + 〈−2, 4〉 = ⃗0<br />

3⃗v + 〈−2, 4〉 = ⃗0<br />

(3⃗v + 〈−2, 4〉)+(−〈−2, 4〉) = ⃗0+(−〈−2, 4〉)<br />

3⃗v +[〈−2, 4〉 +(−〈−2, 4〉)] = ⃗0+(−1) 〈−2, 4〉<br />

3⃗v + ⃗0 = ⃗0+〈(−1)(−2), (−1)(4)〉<br />

3⃗v = 〈2, −4〉<br />

[( 1<br />

3<br />

1<br />

3 (3⃗v) = 1 3<br />

(〈2, −4〉)<br />

) ] 〈(<br />

(3) ⃗v =<br />

1<br />

) (<br />

3 (2), 1<br />

〉<br />

3)<br />

(−4)<br />

1⃗v = 〈 2<br />

3 , − 4 〉<br />

3<br />

⃗v = 〈 2<br />

3 , − 4 〉<br />

3<br />

A vector whose initial point is (0, 0) is said to be in standard position. If⃗v = 〈v 1 ,v 2 〉 is plotted<br />

in standard position, then its terminal point is necessarily (v 1 ,v 2 ). (Once more, think about this<br />

before reading on.)<br />

y<br />

(v 1 ,v 2 )<br />

⃗v = 〈v 1 ,v 2 〉 in standard position.<br />

x

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