chapter 51 scalar and vector products AWS

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CHAPTER 51 SCALAR AND VECTOR PRODUCTS EXERCISE 216 Page 591 1. Find the scalar product a • b when (i) a = i + 2j – k and b = 2i + 3j + k (ii) a = i – 3j + k and b = 2i + j + k

(a) a b = (1)(2) + (2)(3) + (–1)(1) = 7 (b) a b = (1)(2) + (–3)(1) + (1)(1) = 2 – 3 + 1 = 0

2. Given p = 2i – 3j, q = 4j – k and r = i + 2j – 3k, determine: (a) p • q

(b) p • r

(a) p q = (2)(0) + (–3)(4) + (0)(–1) = –12 (b) p r = (2)(1) + (–3)(2) + (0)(–3) = 2 – 6 = –4

3. Given q = 4j – k and r = i + 2j – 3k, determine: (a) q • r (b) r • q

(a) q r = (0)(1) + (4)(2) + (–1)(–3) = 0 + 8 + 3 = 11 (b) r q = (1)(0) + (2)(4) + (–3)(–1) = 0 + 8 + 3 = 11

4. Given p = 2i – 3j and r = i + 2j – 3k, determine: (a) p (b) r

(a) p =

( (2)

(b) r =

( (1)

)

2

+ (−3) 2 + (0) 2 = 13

2

+ (2) 2 + (−3) 2 = 14

)

5. Given p = 2i – 3j, q = 4j – k and r = i + 2j – 3k, determine: (a) p •(q + r)

(b) 2r •(q – 2p)

(a) p ⋅ ( q + r ) = (2i – 3j)(4j – k + i + 2j – 3k) = (2i – 3j)( i + 6j – 4k) = (2)(1) + (–3)(6) + (0)(–4) = 2 – 18 + 0 = –16 (b) 2r ⋅ (q – 2p) = (2i + 4j – 6k) ⋅ (4j – k – 2(2i – 3j)) = (2i + 4j – 6k) ⋅ (– 4i + 10j – k) 886

© 2014, John Bird

= (2)(–4) + (4)(10) + (–6)(–1) = – 8 + 40 + 6 = 38

6. Given p = 2i – 3j, q = 4j – k and r = i + 2j – 3k, determine: (a) p + r

( (2 + 1)

(a) p + r =

( (2)

(b) p + r =

2

2

(b) p + r

)

+ (−3 + 2) 2 + (0 − 3) 2 = 19

)

+ (−3) 2 + (0) 2 +

((1) + ( 2) + ( −3) ) = 2

2

2

13 + 14 = 7.347

7. Given p = 2i – 3j, q = 4j – k and r = i + 2j – 3k, find the angle between (a) p and q (b) q and r

(a) From equation (4), page 589, cos θ =

=

a + a2 2 + a32 b12 + b2 2 + b32 (2)(0) + (−3)(4) + (0)(−1) 2 + (−3) + 0 2

2

2

0 + 4 + (−1) 2

2

2

=

−12 = –0.8072 13 17

θ = cos −1 (−0.8072) = 143.82°

from which, (b) cos θ =

a1b1 + a2b2 + a3b3 2 1

(0)(1) + (4)(2) + (−1)(−3) = 0 + 42 + (−1) 2 12 + 22 + (−3) 2 2

11 = 0.713024 17 14

θ = cos −1 (0.713024) = 44.52°

from which,

8. Given p = 2i – 3j, q = 4j – k and r = i + 2j – 3k, determine the direction cosines of: (a) p

(b) q

(c) r

(a) For p, cos α =

2 = 2 2 + (−3) 2

0 −3 2 = 0.555, cos β = = –0.832 and cos γ = =0 13 13 13

(b) For q, cos α =

0 = 2 4 + (−1) 2

−1 4 0 = 0, cos β = = 0.970 and cos γ = = –0.243 17 17 17

1 = 2 2 1 + 2 + (−3) 2 −3 and cos γ = = –0.802 14

(c) For r, cos α =

2 1 = 0.267, cos β = = 0.535 14 14

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9. Determine the angle between the forces: F1 = 3i + 4j + 5k and F2 = i + j + k

cos θ =

(3)(1) + (4)(1) + (5)(1) = 32 + 42 + 52 12 + 12 + 12

from which,

12 = 0.979795... 50 3

θ = cos −1 (0.979795...) = 11.54°

10. Find the angle between the velocity vectors v 1 = 5i + 2j + 7k and v2 = 4i + j – k

cos θ =

(5)(4) + (2)(1) + (7)(−1) = 52 + 22 + 7 2 42 + 12 + (−1) 2

from which,

15 = 0.40032 78 18

θ = cos −1 (0.40032) = 66.40°

11. Calculate the work done by a force F = (–5i + j + 7k) N when its point of application moves from point (–2i – 6j + k) m to the point (i – j + 10k) m. Work done = F ⋅ d where d = (i – j + 10k) – (–2i – 6j + k) = 3i + 5j + 9k Hence, work done = (–5i + j + 7k) ⋅ (3i + 5j + 9k) = –15 + 5 + 63 = 53 N m

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© 2014, John Bird

EXERCISE 217 Page 594

1. Given p = 3i + 2k, q = i – 2j + 3k and r = –4i + 3j – k determine: (a) p × q

(b) q × p

i j k 0 2 3 2 3 0 (a) p × q = 3 0 2 = i –j +k = 4i – 7j – 6k 1 3 1 −2 −2 3 1 −2 3 i j k −2 3 1 3 1 −2 (b) q × p = 1 −2 3 = i –j +k = –4i + 7j + 6k 0 2 3 2 3 0 3 0 2

2. Given p = 3i + 2k, q = i – 2j + 3k and r = –4i + 3j – k determine: (a) p × r

(b) r × q

( p ⋅ p )( r ⋅ r ) − ( p ⋅ r )

(a) p × r =

where p ⋅ p = (3)(3) + (2)(2) = 13,

2

r ⋅ r = (–4)(–4) + (3)(3) + (–1)(–1) = 26 and Hence,

p×r =

(b) r × q = =

2 (13)(26) − (−14)  =

( r ⋅ r )( q ⋅ q ) − ( r ⋅ q )

2

p ⋅ r = (3)(–4) + (0)(3) + (2)(–1) = –14 (338 − 196) =

142 = 11.92

where r ⋅ r = (–4)(–4) + (3)(3) + (–1)(–1) = 26, q ⋅ q = (1)(1) +(–2)(–2) + (3)(3) = 14

and Hence,

r×q =

2 (26)(14) − (−13)  =

r ⋅ q = (–4)(1) + (3)(–2) + (–1)(3) = –13 (364 − 169) =

195 = 13.96

3. Given p = 3i + 2k, q = i – 2j + 3k and r = –4i + 3j – k determine: (a) 2p × 3r

(b) (p + r) × q

(a) 2p = 2(3i + 2k) = 6i + 4k

and 3r = 3(– 4i + 3j – k) = – 12i + 9j – 3k

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© 2014, John Bird

i j k 0 Hence, 2p × 3r = 6 0 4 =i 9 − 12 9 −3

4 6 –j −3 − 12

4 6 0 +k = – 36i – 30j + 54k −3 − 12 9

(b) p + r = 3i + 2k + (– 4i + 3j – k) = – i + 3j + k i Hence, (p + r) × q = − 1

j 3

1 −2

k 1 =i 3

−1 1 3 1 −1 –j +k −2 3 1 3 1

3 = 11i + 4j – k −2

4. Given p = 3i + 2k, q = i – 2j + 3k and r = –4i + 3j – k determine: (a) p × (r × q)

(b) (3p × 2r) × q

i j k (a) r × q = − 4 3 −1 = 7i + 11j + 5k 1 −2 3

Hence,

i j k p × (r × q) = 3 0 2 = (–22)i – (1)j + (33)k = –22i – j + 33k 7 11 5

(b) 3p × 2r =

i 9

j 0

k 6

= (–36)i – (–18 + 48)j + (54)k = –36i – 30j + 54k

− 8 6 −2 i j k (3p × 2r) × q = − 36 −30 54 = (–90 + 108)i – (–108 – 54)j + (72 + 30)k 1

−2

3

= 18i + 162j + 102k

5. For vectors p = 4i – j + 2k and q = –2i + 3j – 2k determine (i) p • q

(ii) p × q

(iii) p × q

(iv) q × p and (v) the angle between the vectors

(i)

p • q = (4)(– 2) + (–1)(3) +(2)(–2) = –15

(ii)

i j k p × q = 4 −1 2 = i ( 2 − 6 ) – j(– 8 + 4) + k(12 – 2) = −4i + 4 j + 10k − 2 3 −2

(iii) p ⋅ p = (4)(4) + (–1)(–1) + ( 2 )( 2 ) = 21 890

© 2014, John Bird

q ⋅ q = (–2)(–2) + (3)(3) + (–2)(–2) = 17 p ⋅ q = (4)(–2) + (–1)(3) + ( 2 )( −2 ) = –15 p×q =

= ( 357 − 225 )

2 ( 21)(17 ) − ( −15=  )  

i

132 = 11.49

k (iv) q × p = − 2 3 −2 = i ( 6 − 2 ) – j(– 4 + 8) + k(2 – 12) = 4i − 4 j − 10k 4 −1 2

(v)

cos θ =

j

(4)(−2) + (−1)(3) + ( 2 ) (−2) (4) 2 + (−1) 2 + ( 2 )

6. For vectors a = –7i + 4j +

(i)

(−2) 2 + (3) 2 + (−2) 2

=

−15 = −0.793884... 21 17

θ = cos −1 (−0.793884...) = 142.55°

from which,

(i) a • b

2

(ii) a × b

1 k and b = 6i – 5j – k find 2

(iii) a × b

(iv) b × a and (v) the angle between the vectors

1 1 a ⋅ b = (–7)(6) + (4)(–5) + ( )(–1) = –62 2 2

i (ii) a × b = − 7

6

j

k

5 1 1  = i  −4 +  – j(7 – 3) + k(35 – 24) = −1 i − 4 j + 11k 2 2 2  −5 −1 4

 1  1  (iii) a ⋅ a = (–7)(–7) + (4)(4) +     = 65.25  2  2  b ⋅ b = (6)(6) + (–5)(–5) + (–1)(–1) = 62

1 a ⋅ b = (–7)(6) + (4)(–5) +   ( −1) = –62.5 2 a×b =

2 ( 65.25 )( 62 ) − ( −62.5  = )  

i

(iv) b × a =

j

= ( 4045.5 − 3906.25 )

139.25 = 11.80

k

1  5  −5 −1 = i  − + 4  – j(3 – 7) + k(24 – 35) = 1 i + 4 j − 11k 2  2  1 −7 4 2

6

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© 2014, John Bird

cos θ =

(v)

1 (−7)(6) + (4)(−5) +   (−1) 2 1 (−7) 2 + (4) 2 +   2

2

=

(6) 2 + (−5) 2 + (−1) 2

−62.5 = −0.9826388 65.25 62

θ = cos −1 (−0.9826388) = 169.31°

from which,

7. Forces of (i + 3j), (– 2i – j), (i – 2j) newtons act at three points having position vectors of (2i + 5j), 4j and (–i + j) metres, respectively. Calculate the magnitude of the moment.

Magnitude of the moments = the sum of the magnitudes of the three forces When position vector, r = 2i + 5j and F = i + 3j Magnitude of M, M = r × F = where

( r ⋅ r )( F ⋅ F ) − ( r ⋅ F )

2

r ⋅ r = (2)(2) + (5)(5) +(0)(0) = 29 F ⋅ F = (1)(1) + (3)(3) +(0)(0) = 10 r ⋅ F = (2)(1) + (5)(3) + (0)(0) = 17

i.e.

M =

( 29 )(10 ) − (17 )

2

=1Nm

When position vector, r = 4j and F = –2i – j Magnitude of M, M = r × F = where

( r ⋅ r )( F ⋅ F ) − ( r ⋅ F )

2

r ⋅ r = (0)(0) + (4)(4) +(0)(0) = 16 F ⋅ F = (– 2)(–2) + (–1)(–1) +(0)(0) = 5 r ⋅ F = (0)(–2) + (4)(–1) + (0)(0) = –4

i.e.

M =

(16 )( 5) − ( −4 )

2

=8Nm

When position vector, r = –i + j and F = –i – 2j Magnitude of M, M = r × F = where

( r ⋅ r )( F ⋅ F ) − ( r ⋅ F )

2

r ⋅ r = (1)(1) + (1)(1) + (0)(0) = 2 F ⋅ F = (–1)(–1) + (–2)(–2) + (0)(0) = 5 892

© 2014, John Bird

r ⋅ F = (1)(–1) + (1)(–2) + (0)(0) = –3 i.e.

M =

( 2 )( 5) − ( −3)

2

=1Nm

Hence, magnitude of the moment = 1 + 8 + 1 = 10 N m

8. A force of (2i – j + k) newtons acts on a line through point P having coordinates (0, 3, 1) metres. Determine the moment vector and its magnitude about point Q having coordinates (4, 0, –1) metres.

Position vector, r = (0i + 3j + k) – (4i + 0j – k) = –4i + 3j + 2k

Moment, M = r × F

i j k where M = − 4 3 2 = (3 + 2)i – (–4 – 4)j + (4 – 6)k 2 −1 1 = (5i + 8j – 2k) N m

Magnitude of M, M = r × F = where

( r ⋅ r )( F ⋅ F ) − ( r ⋅ F )

2

r ⋅ r = (–4)(–4) + (3)(3) + (2)(2) = 29 F ⋅ F = (2)(2) + (–1)(–1) +(1)(1) = 6 r ⋅ F = (–4)(2) + (3)(–1) +(2)(1) = –9

i.e.

M =

( 29 )( 6 ) − ( −9 )

2

= 9.64 N m

9. A sphere is rotating with angular velocity ω about the z-axis of a system, the axis coinciding with the axis of the sphere. Determine the velocity vector and its magnitude at position (–5i + 2j – 7k) m, when the angular velocity is (i + 2j) rad/s.

Velocity vector, v = ω × r = (i + 2j ) × (–5i + 2j – 7k) =

i

j

k

1

2

0

− 5 2 −7

= (–14 – 0)i – (– 7 – 0)j + (2 + 10)k = –14i + 7j + 12k

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© 2014, John Bird

Magnitude of v, v =

(ω ⋅ ω )( r ⋅ r ) − ( r ⋅ ω )

2

where ω ⋅ ω = (1)(1) + (2)(2) + (0)(0) = 5 r ⋅ r = (– 5)(–5) + (2)(2) + (–7)(–7) = 78 r ⋅ ω = (–5)(1) + (2)(2) + (–7)(0) = –1 Hence,

v =

( 5)( 78) − ( −1)

2

= 19.72 m/s

10. Calculate the velocity vector and its magnitude for a particle rotating about the z-axis at an angular velocity of (3i – j + 2k) rad/s when the position vector of the particle is at (i – 5j + 4k) m.

i j k Velocity vector, v = ω × r = (3i – j + 2k) × (i – 5j + 4k) = 3 1 2 1 −5 4

= (–4 + 10)i – (12 – 2)j + (–15 + 1)k = 6i – 10j – 14k Magnitude of v, v =

(ω ⋅ ω )( r ⋅ r ) − ( r ⋅ ω )

2

where ω ⋅ ω = (3)(3) + (–1)(–1) + (2)(2) = 14 r ⋅ r = (1)(1) + (–5)(–5) + (4)(4) = 42 r ⋅ ω = (1)(3) + (–5)(–1) + (4)(2) = 16 Hence,

v =

(14 )( 42 ) − (16 )

2

= 18.22 m/s

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© 2014, John Bird

EXERCISE 218 Page 596

1. Find the vector equation of the line through the point with position vector 5i – 2j + 3k which is parallel to the vector 2i + 7j – 4k. Determine the point on the line corresponding to λ = 2 in the resulting equation. Vector equation of the line, r = a + λb = (5i – 2j + 3k) + λ(2i + 7j – 4k) i.e.

r = (5 + 2λ)i + (7λ – 2)j + (3 – 4λ)k

When λ = 2,

r = 9i + 12j – 5k

2. Express the vector equation of the line in Problem 1 in standard Cartesian form.

The vector equation of a straight line in standard Cartesian form is:

x − a1 y − a2 z − a3 = = = λ b1 b2 b3 Since a = 5i – 2j + 3k,

a1 = 5, a2 = −2 and a3 = 3

and

b1 = 2, b2 = 7 and b3 = −4

b = 2i + 7j – 4k,

then the Cartesian equations are:

3. Express in vector form:

3x − 1 5 y + 1 4 − z = = 4 2 3

i.e.

i.e.

x −5 y + 2 z −3 = = = λ 2 7 −4

or

x −5 y + 2 3− z = = = λ 2 7 4

3x − 1 5 y + 1 4 − z = = 3 4 2

i.e.

1 1   3 x −  5 y +  3 5  −1( z − 4 )   = = 4 2 3

1  1  x−  y+  3  5 = = 4 2 3 5

( z − 4) −3

1 1 a1 = , a2 = − and a3 = 4 3 5 895

© 2014, John Bird

and

b1 =

4 2 , b2 = and b3 = −3 3 5

Hence, in vector form the equation is: r = ( a1 + λb1 ) i + ( a2 + λb2 ) j + ( a3 + λb3 ) k

1 4  =  + λi + 3 3  or

r=

 1 2   − + λ  j + ( 4 − 3λ ) k  5 5 

1 1 (1 + 4λ ) i + ( 2λ − 1) j + ( 4 − 3λ ) k 3 5

4. Express in vector form: 2x + 1 =

2 x + 1 1 − 4 y 3z − 1 = = 1 5 4

i.e.

3z − 1 1− 4 y = 4 5

1 1 1 z− x+ y− 3 2 = 4 = 1 5 4 − 2 4 3

i.e.

1 1 1 and a3 = a1 = − , a2 = 2 4 3

and

1 5 4 b1 = , b2 = − and b3 = 2 4 3

Hence, in vector form the equation is: r = ( a1 + λb1 ) i + ( a2 + λb2 ) j + ( a3 + λb3 ) k

1 5   1 1  1 4  = − + λi +  − λj +  + λk 4 4   2 2  3 3  or

r=

1 1 1 ( λ − 1) i + (1 − 5λ ) j + (1 + 4λ ) k 2 4 3

896

© 2014, John Bird