Solucionario de estática, décima edición, Beer - Johnston

1. SOLUTION
MANUAL

2. CHAPTER 2

4. PROBLEM 2.1
Two forces are applied at point B of beam AB. Determine
graphically the magnitude and direction of their resultant using
(a) the parallelogram law, (b) the triangle rule.
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3
SOLUTION
(a) Parallelogram law:
(b) Triangle rule:
We measure: R = 3.30 kN, α = 66.6° R = 3.30 kN 66.6° 

5. PROBLEM 2.2
The cable stays AB and AD help support pole AC. Knowing
that the tension is 120 lb in AB and 40 lb in AD, determine
graphically the magnitude and direction of the resultant of the
forces exerted by the stays at A using (a) the parallelogram
law, (b) the triangle rule.
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4
SOLUTION
We measure: 51.3
59.0
α
β
= °
= °
(a) Parallelogram law:
(b) Triangle rule:
We measure: R = 139.1 lb, γ = 67.0° R =139.1 lb 67.0° 


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5
PROBLEM 2.3
Two structural members B and C are bolted to bracket A. Knowing that both
members are in tension and that P = 10 kN and Q = 15 kN, determine
graphically the magnitude and direction of the resultant force exerted on the
bracket using (a) the parallelogram law, (b) the triangle rule.
SOLUTION
(a) Parallelogram law:
(b) Triangle rule:
We measure: R = 20.1 kN, α = 21.2° R = 20.1 kN 21.2° 

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6
PROBLEM 2.4
Two structural members B and C are bolted to bracket A. Knowing that
both members are in tension and that P = 6 kips and Q = 4 kips, determine
graphically the magnitude and direction of the resultant force exerted on
the bracket using (a) the parallelogram law, (b) the triangle rule.
SOLUTION
(a) Parallelogram law:
(b) Triangle rule:
We measure: R = 8.03 kips, α = 3.8° R = 8.03 kips 3.8° 

8. ° + + ° = °
R
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7
PROBLEM 2.5
A stake is being pulled out of the ground by means of two ropes as shown.
Knowing that α = 30°, determine by trigonometry (a) the magnitude of the
force P so that the resultant force exerted on the stake is vertical, (b) the
corresponding magnitude of the resultant.
SOLUTION
Using the triangle rule and the law of sines:
(a)
120 N
sin 30 sin 25
P =
° °
P = 101.4 N 
(b) 30 25 180
180 25 30
125
β
β
= °− °− °
= °
120 N
sin 30 sin125
=
° °
R = 196.6 N 

9. PROBLEM 2.6
A trolley that moves along a horizontal beam is acted upon by two
forces as shown. (a) Knowing that α = 25°, determine by trigonometry
the magnitude of the force P so that the resultant force exerted on the
trolley is vertical. (b) What is the corresponding magnitude of the
resultant?
° + + ° = °
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8
SOLUTION
Using the triangle rule and the law of sines:
(a)
1600 N
=
P sin 25° sin 75
°
P = 3660 N 
(b) 25 75 180
180 25 75
80
β
β
= °− °− °
= °
1600 N
=
R sin 25° sin80
°
R = 3730 N 

10. PROBLEM 2.7
A trolley that moves along a horizontal beam is acted upon by two forces
as shown. Determine by trigonometry the magnitude and direction of the
force P so that the resultant is a vertical force of 2500 N.
= °
= °
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9
SOLUTION
Using the law of cosines: 2 (1600 N)2 (2500 N)2 2(1600 N)(2500 N) cos 75°
2596 N
P
P
= + −
=
Using the law of sines:
sin sin 75
1600 N 2596 N
36.5
α
α
P is directed 90° − 36.5° or 53.5° below the horizontal. P = 2600 N 53.5° 

11. ° + ° + = °
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10
PROBLEM 2.8
A telephone cable is clamped at A to the pole AB. Knowing that the tension
in the left-hand portion of the cable is T1 = 800 lb, determine by
trigonometry (a) the required tension T2 in the right-hand portion if the
resultant R of the forces exerted by the cable at A is to be vertical, (b) the
corresponding magnitude of R.
SOLUTION
Using the triangle rule and the law of sines:
(a) 75 40 180
180 75 40
65
α
α
= °− °− °
= °
800 lb 2
sin 65 sin 75
T =
° °
2 T = 853 lb 
(b)
800 lb
sin 65 sin 40
R =
° °
R = 567 lb 

12. PROBLEM 2.9
A telephone cable is clamped at A to the pole AB. Knowing that the
tension in the right-hand portion of the cable is T2 = 1000 lb, determine
by trigonometry (a) the required tension T1 in the left-hand portion if
the resultant R of the forces exerted by the cable at A is to be vertical,
(b) the corresponding magnitude of R.
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11
SOLUTION
Using the triangle rule and the law of sines:
(a) 75 40 180
180 75 40
65
β
β
° + ° + = °
= °− °− °
= °
1000 lb =
T 1
sin 75° sin 65
°
1 T = 938 lb 
(b)
1000 lb
=
R sin 75° sin 40
°
R = 665 lb 

13. PROBLEM 2.10
Two forces are applied as shown to a hook support. Knowing that the
magnitude of P is 35 N, determine by trigonometry (a) the required angle
α if the resultant R of the two forces applied to the support is to be
horizontal, (b) the corresponding magnitude of R.
α
= °
=
α = 37.138° α = 37.1° 
+ + °= °
R =
° °
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12
SOLUTION
Using the triangle rule and law of sines:
(a)
sin sin 25
50 N 35 N
sin 0.60374
α
(b) 25 180
180 25 37.138
117.862
α β
β
= °− °− °
= °
35 N
sin117.862 sin 25
R = 73.2 N 

14. PROBLEM 2.11
A steel tank is to be positioned in an excavation. Knowing that
α = 20°, determine by trigonometry (a) the required magnitude
of the force P if the resultant R of the two forces applied at A is
to be vertical, (b) the corresponding magnitude of R.
+ °+ °= °
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13
SOLUTION
Using the triangle rule and the law of sines:
(a) 50 60 180
180 50 60
70
β
β
= °− °− °
= °
425 lb
sin 70 sin 60
P =
° °
P = 392 lb 
(b)
425 lb
sin 70 sin 50
R =
° °
R = 346 lb 

15. PROBLEM 2.12
A steel tank is to be positioned in an excavation. Knowing that
the magnitude of P is 500 lb, determine by trigonometry (a) the
required angle α if the resultant R of the two forces applied at A
is to be vertical, (b) the corresponding magnitude of R.
+ ° + °+ = °
α β
= °− + °− °
= °−
β α
β α
α
° − = °
90° −α = 47.402° α = 42.6° 
R =
° + ° °
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14
SOLUTION
Using the triangle rule and the law of sines:
(a) ( 30 ) 60 180
180 ( 30 ) 60
90
sin (90 ) sin 60
425 lb 500 lb
(b)
500 lb
sin (42.598 30 ) sin 60
R = 551 lb 

16. PROBLEM 2.13
A steel tank is to be positioned in an excavation. Determine by
trigonometry (a) the magnitude and direction of the smallest
force P for which the resultant R of the two forces applied at A
is vertical, (b) the corresponding magnitude of R.
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15
SOLUTION
The smallest force P will be perpendicular to R.
(a) P = (425 lb) cos30° P = 368 lb 
(b) R = (425 lb)sin 30° R = 213 lb 

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16
PROBLEM 2.14
For the hook support of Prob. 2.10, determine by trigonometry (a) the
magnitude and direction of the smallest force P for which the resultant R of
the two forces applied to the support is horizontal, (b) the corresponding
magnitude of R.
SOLUTION
The smallest force P will be perpendicular to R.
(a) P = (50 N)sin 25° P = 21.1 N 
(b) R = (50 N) cos 25° R = 45.3 N 

18. PROBLEM 2.15
Solve Problem 2.2 by trigonometry.
PROBLEM 2.2 The cable stays AB and AD help support pole
AC. Knowing that the tension is 120 lb in AB and 40 lb in AD,
determine graphically the magnitude and direction of the
resultant of the forces exerted by the stays at A using (a) the
parallelogram law, (b) the triangle rule.
=
= °
=
= °
α β ψ
+ + = °
° + ° + = °
γ = °
γ
φ α γ
φ
φ
= °
= °− +
= °− ° + °
= ° R = 139.1 lb 67.0° 
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17
SOLUTION
8
tan
10
38.66
6
tan
10
30.96
α
α
β
β
Using the triangle rule: 180
38.66 30.96 180
110.38
ψ
ψ
= °
Using the law of cosines: 2 (120 lb)2 (40 lb)2 2(120 lb)(40 lb) cos110.38
139.08 lb
R
R
= + − °
=
Using the law of sines:
sin sin110.38
40 lb 139.08 lb
15.64
(90 )
(90 38.66 ) 15.64
66.98

19. PROBLEM 2.16
Solve Problem 2.4 by trigonometry.
PROBLEM 2.4 Two structural members B and C are bolted to bracket A.
Knowing that both members are in tension and that P = 6 kips and Q = 4 kips,
determine graphically the magnitude and direction of the resultant force
exerted on the bracket using (a) the parallelogram law, (b) the triangle rule.
SOLUTION
Using the force triangle and the laws of cosines and sines:
We have: 180 (50 25 )
γ= °− °+ °
= °
(4 kips) (6 kips) 2(4 kips)(6 kips) cos105
64.423 kips
8.0264 kips
=
° + °
° + =
° + = °
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18
105
Then 2 2 2
2
R
R
= + − °
=
=
And
4 kips 8.0264 kips
sin(25 ) sin105
sin(25 ) 0.48137
25 28.775
3.775
α
α
α
α
= °
R = 8.03 kips 3.8° 

20. PROBLEM 2.17
For the stake of Prob. 2.5, knowing that the tension in one rope is 120 N,
determine by trigonometry the magnitude and direction of the force P so
that the resultant is a vertical force of 160 N.
PROBLEM 2.5 A stake is being pulled out of the ground by means of two
ropes as shown. Knowing that α = 30°, determine by trigonometry (a) the
magnitude of the force P so that the resultant force exerted on the stake is
vertical, (b) the corresponding magnitude of the resultant.
= °
=
= °
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19
SOLUTION
Using the laws of cosines and sines:
2 (120 N)2 (160 N)2 2(120 N)(160 N) cos25
72.096 N
P
P
= + − °
=
And
sin sin 25
120 N 72.096 N
sin 0.70343
44.703
α
α
α
P = 72.1 N 44.7° 

21. PROBLEM 2.18
For the hook support of Prob. 2.10, knowing that P = 75 N and α = 50°,
determine by trigonometry the magnitude and direction of the resultant of
the two forces applied to the support.
PROBLEM 2.10 Two forces are applied as shown to a hook support.
Knowing that the magnitude of P is 35 N, determine by trigonometry (a) the
required angle α if the resultant R of the two forces applied to the support is
to be horizontal, (b) the corresponding magnitude of R.
SOLUTION
Using the force triangle and the laws of cosines and sines:
We have 180 (50 25 )
β= °− °+ °
= °
(75 N) (50 N)
2(75 N)(50 N) cos105
10,066.1 N
100.330 N
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20
105
Then 2 2 2
2 2
R
R
R
= +
− °
=
=
and
sin sin105
75 N 100.330 N
sin 0.72206
46.225
γ
γ
γ
= °
=
= °
Hence: γ − 25° = 46.225° − 25° = 21.225° R =100.3 N 21.2° 

22. PROBLEM 2.19
Two forces P and Q are applied to the lid of a storage bin as shown.
Knowing that P = 48 N and Q = 60 N, determine by trigonometry the
magnitude and direction of the resultant of the two forces.
SOLUTION
Using the force triangle and the laws of cosines and sines:
We have 180 (20 10 )
γ= °− °+ °
= °
=
φ = ° −α − °
= °− °− °
= °
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21
150
Then 2 (48 N)2 (60 N)2
2(48 N)(60 N) cos150
104.366 N
R
R
= +
− °
=
and
48 N 104.366 N
sin sin150
sin 0.22996
13.2947
α
α
α
°
=
= °
Hence: 180 80
180 13.2947 80
86.705
R =104.4 N 86.7° 

23. PROBLEM 2.20
Two forces P and Q are applied to the lid of a storage bin as shown.
Knowing that P = 60 N and Q = 48 N, determine by trigonometry the
magnitude and direction of the resultant of the two forces.
SOLUTION
Using the force triangle and the laws of cosines and sines:
We have 180 (20 10 )
γ= °− °+ °
= °
=
φ = ° −α − °
= °− °− °
= °
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22
150
Then 2 (60 N)2 (48 N)2
2(60 N)(48 N)cos 150
104.366 N
R
R
= +
− °
=
and
60 N 104.366 N
sin sin150
sin 0.28745
16.7054
α
α
α
°
=
= °
Hence: 180 180
180 16.7054 80
83.295
R =104.4 N 83.3° 

24. PROBLEM 2.21
Determine the x and y components of each of the forces shown.
SOLUTION
80-N Force: (80 N) cos 40 x F = + ° 61.3 N x F = 
Fy = +(80 N) sin 40° 51.4 N Fy = 
120-N Force: (120 N) cos 70 x F = + ° 41.0 N x F = 
(120 N) sin 70 Fy = + ° 112.8 N Fy = 
150-N Force: (150 N) cos35 x F = − ° 122. 9 N x F = − 
(150 N) sin 35 Fy = + ° 86.0 N Fy = 
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23

25. PROBLEM 2.22
Determine the x and y components of each of the forces shown.
SOLUTION
40-lb Force: (40 lb) cos60 x F = + ° 20.0 lb x F = 
Fy = −(40 lb)sin 60° 34.6 lb Fy = − 
50-lb Force: (50 lb)sin 50 x F = − ° 38.3 lb x F = − 
(50 lb) cos50 Fy = − ° 32.1 lb Fy = − 
60-lb Force: (60 lb) cos25 x F = + ° 54.4 lb x F = 
(60 lb)sin 25 Fy = + ° 25.4 lb Fy = 
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24

26. PROBLEM 2.23
Determine the x and y components of each of the forces shown.
(600) (800)
1000 mm
(560) (900)
1060 mm
(480) (900)
1020 mm
1000 x F = + 640 N x F = + 
1000 Fy = + Fy = +480 N 
1060 x F = − 224 N x F = − 
1060 y F = − 360 N Fy = − 
1020 x F = + 192.0 N x F = + 
1020 y F = − 360 N Fy = − 
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25
SOLUTION
Compute the following distances:
2 2
2 2
2 2
OA
OB
OC
= +
=
= +
=
= +
=
800-N Force:
800
(800 N)
600
(800 N)
424-N Force:
560
(424 N)
900
(424 N)
408-N Force:
480
(408 N)
900
(408 N)

27. PROBLEM 2.24
Determine the x and y components of each of the forces shown.
(24 in.) (45 in.)
51.0 in.
(28 in.) (45 in.)
53.0 in.
(40 in.) (30 in.)
50.0 in.
51.0 in. Fx = − 48.0 lb x F = − 
51.0 in. Fy = + 90.0 lb Fy = + 
= + Fx 56.0 lb x F = + 
53.0 in. Fy = + 90.0 lb Fy = + 
50.0 in. Fx = − 160.0 lb x F = − 
50.0 in. Fy = − 120.0 lb Fy = − 
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26
SOLUTION
Compute the following distances:
2 2
2 2
2 2
OA
OB
OC
= +
=
= +
=
= +
=
102-lb Force:
24 in.
102 lb
45 in.
102 lb
106-lb Force:
28 in.
106 lb
53.0 in.
45 in.
106 lb
200-lb Force:
40 in.
200 lb
30 in.
200 lb

28. PROBLEM 2.25
The hydraulic cylinder BD exerts on member ABC a force P directed
along line BD. Knowing that P must have a 750-N component
perpendicular to member ABC, determine (a) the magnitude of the force
P, (b) its component parallel to ABC.
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27
SOLUTION
(a) 750 N = Psin 20°
P = 2192.9 N P = 2190 N 
(b) cos 20 ABC P = P °
= (2192.9 N) cos 20° 2060 N ABC P = 

29. PROBLEM 2.26
Cable AC exerts on beam AB a force P directed along line AC. Knowing that
P must have a 350-lb vertical component, determine (a) the magnitude of the
force P, (b) its horizontal component.
y P
= °
= 500 lb x P = 
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28
SOLUTION
(a)
cos 55
P =
°
350 lb
cos 55
610.21 lb
=
°
= P = 610 lb 
(b) sin 55 xP = P °
(610.21 lb)sin 55
499.85 lb

30. PROBLEM 2.27
Member BC exerts on member AC a force P directed along line BC. Knowing
that P must have a 325-N horizontal component, determine (a) the magnitude
of the force P, (b) its vertical component.
=    
=    
x P P
 
  =  
=    
y P P
 
  =  
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29
SOLUTION
(650 mm)2 (720 mm)2
970 mm
BC= +
=
(a)
650
970 Px P
 
or
970
650
970
325 N
650
485 N
 
=
P = 485 N 
(b)
720
970
720
485 N
970
360 N
 
=
970 N Py = 

31. PROBLEM 2.28
Member BD exerts on member ABC a force P directed along line BD.
Knowing that P must have a 240-lb vertical component, determine (a)
the magnitude of the force P, (b) its horizontal component.
y P
P or P = 373 lb 
= =
°
y
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30
SOLUTION
(a)
240 lb
sin 40 sin 40°
(b)
240 lb
tan 40 tan 40°
x
P
P= =
°
or 286 lb x P = 

32. PROBLEM 2.29
The guy wire BD exerts on the telephone pole AC a force P directed along
BD. Knowing that P must have a 720-N component perpendicular to the
pole AC, determine (a) the magnitude of the force P, (b) its component
along line AC.
P Px
Py = Px
=
=
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31
SOLUTION
(a)
37
12
37
(720 N)
12
2220 N
=
=
=
P = 2.22 kN 
(b)
35
12
35
(720 N)
12
2100 N
= 2.10 kN Py 

33. PROBLEM 2.30
The hydraulic cylinder BC exerts on member AB a force P directed along
line BC. Knowing that P must have a 600-N component perpendicular to
member AB, determine (a) the magnitude of the force P, (b) its component
along line AB.
° = °+ α
+ °+ °
= °− °− °− °
= °
P
x
P
P
x
α
P
P
y
=
x
=
= °
=
α
P P
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32
SOLUTION
180 45 90 30
180 45 90 30
15
α
(a) cos
cos
600 N
cos15
621.17 N
P
α
=
=
=
°
=
P = 621 N 
(b) tan
tan
(600 N) tan15
160.770 N
y x
α
160.8 N Py = 

34. PROBLEM 2.31
Determine the resultant of the three forces of Problem 2.23.
PROBLEM 2.23 Determine the x and y components of each of
the forces shown.
SOLUTION
Components of the forces were determined in Problem 2.23:
Force x Comp. (N) y Comp. (N)
800 lb +640 +480
424 lb –224 –360
408 lb +192 –360
Rx = +608 Ry = −240
R R i R
j
x y
(608 lb) ( 240 lb)
y
R
R
x
α
α
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33
tan
240
608
21.541
240 N
sin(21.541°)
653.65 N
R
= +
= +−
=
=
= °
=
=
i j
R = 654 N 21.5° 

35. PROBLEM 2.32
Determine the resultant of the three forces of Problem 2.21.
PROBLEM 2.21 Determine the x and y components of each of the
forces shown.
SOLUTION
Components of the forces were determined in Problem 2.21:
Force x Comp. (N) y Comp. (N)
80 N +61.3 +51.4
120 N +41.0 +112.8
150 N –122.9 +86.0
Rx = −20.6 Ry = +250.2
R R
x y
( 20.6 N) (250.2 N)
R
R
y
x
α
α
α
α
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34
tan
250.2 N
tan
20.6 N
tan 12.1456
85.293
250.2 N
sin85.293
R
= +
= − +
=
=
=
= °
=
°
R i j
i j
R = 251 N 85.3° 

36. PROBLEM 2.33
Determine the resultant of the three forces of Problem 2.22.
PROBLEM 2.22 Determine the x and y components of each of the
forces shown.
R R
x y
y
R
R
x
α
α
α
α
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35
SOLUTION
Force x Comp. (lb) y Comp. (lb)
40 lb +20.00 –34.64
50 lb –38.30 –32.14
60 lb +54.38 +25.36
Rx = +36.08 Ry = −41.42
( 36.08 lb) ( 41.42 lb)
tan
41.42 lb
tan
36.08 lb
tan 1.14800
48.942
41.42 lb
sin 48.942
R
= +
= + + −
=
=
=
= °
=
°
R i j
i j
R = 54.9 lb 48.9° 

37. PROBLEM 2.34
Determine the resultant of the three forces of Problem 2.24.
PROBLEM 2.24 Determine the x and y components of each of the
forces shown.
SOLUTION
Components of the forces were determined in Problem 2.24:
Force x Comp. (lb) y Comp. (lb)
102 lb −48.0 +90.0
106 lb +56.0 +90.0
200 lb −160.0 −120.0
Rx = −152.0 Ry = 60.0
= +
= − +
=
R R i R
j
x y
( 152 lb) (60.0 lb)
y
x
R
R
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36
tan
60.0 lb
tan
152.0 lb
tan 0.39474
21.541
α
α
α
α
=
=
= °
i j
60.0 lb
sin 21.541
R =
°
R = 163.4 lb 21.5° 

38. PROBLEM 2.35
Knowing that α = 35°, determine the resultant of the three forces
shown.
F
F
F
F
F
F
= +
= − + −
=
R R i R
j
x y
y
R
R
x
=
= °
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37
SOLUTION
100-N Force: (100 N) cos35 81.915 N
(100 N)sin 35 57.358 N
x
y
= + ° = +
= − ° = −
150-N Force: (150 N)cos65 63.393 N
(150 N) sin 65 135.946 N
x
y
= + ° = +
= − ° = −
200-N Force: (200 N)cos35 163.830 N
(200 N)sin 35 114.715 N
x
y
= − ° = −
= − ° = −
Force x Comp. (N) y Comp. (N)
100 N +81.915 −57.358
150 N +63.393 −135.946
200 N −163.830 −114.715
Rx = −18.522 Ry = −308.02
( 18.522 N) ( 308.02 N)
tan
308.02
18.522
86.559
α
α
i j
308.02 N
sin86.559
R = R = 309 N 86.6° 

39. PROBLEM 2.36
Knowing that the tension in rope AC is 365 N, determine the
resultant of the three forces exerted at point C of post BC.
= − = −
= − = −
F
F
F
F
F
F
= Σ = − + + =
= Σ = − + − = −
= +
= +−
=
240 N 480 N 160 N 400 N
275 N 140 N 120 N 255 N
R x F
x
R F
y y
R R R
x y
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38
SOLUTION
Determine force components:
Cable force AC:
960
(365 N) 240 N
1460
1100
(365 N) 275 N
1460
x
y
500-N Force:
24
(500 N) 480 N
25
7
(500 N) 140 N
25
x
y
= =
= =
200-N Force:
4
(200 N) 160 N
5
3
(200 N) 120 N
5
x
y
= =
= − = −
and
2 2
2 2
(400 N) ( 255 N)
474.37 N
Further:
255
tan
400
32.5
α
α
=
= °
R = 474 N 32.5° 

40. PROBLEM 2.37
Knowing that α = 40°, determine the resultant of the three forces
shown.
SOLUTION
60-lb Force: (60 lb)cos 20 56.382 lb
(60 lb)sin 20 20.521 lb
F
F
F
F
F
F
= Σ =
= Σ =
= +
=
200.305 lb
29.803 lb
R F
R F
R
x x
y y
α = −
= ° R = 203 lb 8.46° 
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39
x
y
= °=
= °=
80-lb Force: (80 lb) cos60 40.000 lb
(80 lb)sin60 69.282 lb
x
y
= °=
= °=
120-lb Force: (120 lb) cos30 103.923 lb
(120 lb)sin 30 60.000 lb
x
y
= °=
= − ° = −
and
2 2
(200.305 lb) (29.803 lb)
202.510 lb
Further:
29.803
tan
200.305
α =
1 29.803
tan
200.305
8.46

41. PROBLEM 2.38
Knowing that α = 75°, determine the resultant of the three forces
shown.
SOLUTION
60-lb Force: (60 lb) cos 20 56.382 lb
(60 lb) sin 20 20.521 lb
F
F
F
F
F
F
= Σ =
= Σ =
R F
R F
R= +
=
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40
x
y
= °=
= °=
80-lb Force: (80 lb) cos 95 6.9725 lb
(80 lb)sin 95 79.696 lb
x
y
= °= −
= °=
120-lb Force: (120 lb) cos 5 119.543 lb
(120 lb)sin 5 10.459 lb
x
y
= °=
= °=
Then 168.953 lb
110.676 lb
x x
y y
and (168.953 lb)2 (110.676 lb)2
201.976 lb
110.676
tan
168.953
tan 0.65507
33.228
α
α
α
=
=
= ° R = 202 lb 33.2° 

42. PROBLEM 2.39
For the collar of Problem 2.35, determine (a) the required value of
α if the resultant of the three forces shown is to be vertical, (b) the
corresponding magnitude of the resultant.
= Σ
= + + ° −
= − + + ° (1)
R F
x x
R
= Σ
= − − + ° −
= − − + ° (2)
R F
y y
α α
− + + ° =
α α α
− + ° − ° =
α α
=
29.904
=
=
= ° α = 21.7° 
Ry = − ° − °
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41
SOLUTION
(100 N) cos (150 N) cos ( 30 ) (200 N) cos
(100 N)cos (150 N) cos ( 30 )
x
α α α
α α
(100 N) sin (150 N)sin ( 30 ) (200 N)sin
(300 N) sin (150 N)sin ( 30 )
y
R
α α α
α α
(a) For R to be vertical, we must have 0. x R = We make 0 x R = in Eq. (1):
100cos 150cos ( 30 ) 0
100cos 150(cos cos 30 sin sin 30 ) 0
29.904cos 75sin
tan
75
0.39872
21.738
α
α
(b) Substituting for α in Eq. (2):
300sin 21.738 150sin 51.738
228.89 N
= −
| | 228.89 N R = Ry = R = 229 N 

43. PROBLEM 2.40
For the post of Prob. 2.36, determine (a) the required tension in
rope AC if the resultant of the three forces exerted at point C is
to be horizontal, (b) the corresponding magnitude of the
resultant.
= Σ = − + +
R F T
x x AC
= − + (1)
R T
x AC
= Σ = − + −
R F T
y y AC
= − + (2)
R T
y AC
73 AC − T + =
= − +
=
= =
R
R
R R R = 623 N 
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42
SOLUTION
960 24 4
(500 N) (200 N)
1460 25 5
48
640 N
73
1100 7 3
(500 N) (200 N)
1460 25 5
55
20 N
73
(a) For R to be horizontal, we must have Ry = 0.
Set 0 Ry = in Eq. (2):
55
20 N 0
26.545 N AC T = 26.5 N AC T = 
(b) Substituting for AC T into Eq. (1) gives
48
(26.545 N) 640 N
73
622.55 N
623 N
x
x
x

44. PROBLEM 2.41
A hoist trolley is subjected to the three forces shown. Knowing that α = 40°,
determine (a) the required magnitude of the force P if the resultant of
the three forces is to be vertical, (b) the corresponding magnitude of
the resultant.
P
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43
SOLUTION
x R = (ΣFx = P + 200 lb)sin 40° − (400 lb) cos 40°
177.860 lb x R = P − (1)
Ry = (200 lb) cos 40 (400 lb) sin 40 ΣFy = ° + °
410.32 lb Ry = (2)
(a) For R to be vertical, we must have 0. x R =
Set 0 x R = in Eq. (1)
0 177.860 lb
177.860 lb
P
= −
= P = 177.9 lb 
(b) Since R is to be vertical:
= = 410 lb R Ry R = 410 lb 

45. PROBLEM 2.42
A hoist trolley is subjected to the three forces shown. Knowing
that P = 250 lb, determine (a) the required value of α if the
resultant of the three forces is to be vertical, (b) the corresponding
magnitude of the resultant.
α = α
+
α = α
+
α = α + α
+
α α α
(400 lb) cos (200 lb) sin 250 lb
2cos sin 1.25
4cos sin 2.5sin 1.5625
− = + +
4(1 sin ) sin 2.5sin 1.5625
= + −
α α
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44
SOLUTION
x R = 250 lb ΣFx = + (200 lb)sinα − (400 lb)cosα
250 lb (200 lb)sin (400 lb)cos x R = + α − α (1)
Ry = (200 lb) cos (400 lb)sin ΣFy = α + α
(a) For R to be vertical, we must have 0. x R =
Set 0 x R = in Eq. (1)
0 = 250 lb + (200 lb)sinα − (400 lb) cosα
2 2
2 2
2
0 5sin 2.5sin 2.4375
Using the quadratic formula to solve for the roots gives
sinα = 0.49162
or α = 29.447° α = 29.4° 
(b) Since R is to be vertical:
(200 lb) cos 29.447 (400 lb) sin 29.447 R = Ry = ° + ° R = 371 lb 

46. PROBLEM 2.43
Two cables are tied together at C and are loaded as shown.
Determine the tension (a) in cable AC, (b) in cable BC.
TAC TBC = =
° ° °
sin108.492 AC T= °
sin108.492 BC T= °
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45
SOLUTION
Free-Body Diagram
1100
tan
960
48.888
400
tan
960
22.620
α
α
β
β
=
= °
=
= °
Force Triangle
Law of sines:
15.696 kN
sin 22.620 sin 48.888 sin108.492
(a)
15.696 kN
(sin 22.620 )
°
6.37 kN AC T = 
(b)
15.696 kN
(sin 48.888 )
°
12.47 kN BC T = 

47. PROBLEM 2.44
Two cables are tied together at C and are loaded as shown. Determine
the tension (a) in cable AC, (b) in cable BC.
TAC TBC = =
° ° °
sin 94.979 AC T= °
sin 94.979 BC T= °
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46
SOLUTION
3
tan
2.25
53.130
1.4
tan
2.25
31.891
α
α
β
β
=
= °
=
= °
Free-Body Diagram
Law of sines: Force-Triangle
660 N
sin 31.891 sin 53.130 sin 94.979
(a)
660 N
(sin 31.891 )
°
350 N AC T = 
(b)
660 N
(sin 53.130 )
°
530 N BC T = 

48. PROBLEM 2.45
Knowing that α = 20°, determine the tension (a) in cable AC,
(b) in rope BC.
AC BC T T = =
° ° °
sin 65 TAC = °
sin 65 TBC = °
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47
SOLUTION
Free-Body Diagram Force Triangle
Law of sines:
1200 lb
sin 110 sin 5 sin 65
(a)
1200 lb
sin 110
°
1244 lb AC T = 
(b)
1200 lb
sin 5
°
115.4 lb BC T = 

49. PROBLEM 2.46
Knowing that α = 55° and that boom AC exerts on pin C a force directed
along line AC, determine (a) the magnitude of that force, (b) the tension in
cable BC.
AC BC F T = =
° ° °
sin 95 FAC = °
sin 95 TBC = °
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48
SOLUTION
Free-Body Diagram Force Triangle
Law of sines:
300 lb
sin 35 sin 50 sin 95
(a)
300 lb
sin 35
°
172.7 lb AC F = 
(b)
300 lb
sin 50
°
231 lb BC T = 

50. PROBLEM 2.47
Two cables are tied together at C and loaded as shown.
Determine the tension (a) in cable AC, (b) in cable BC.
TAC TBC = =
° ° °
sin 44.333 AC T= °
sin 44.333 BC T= °
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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49
SOLUTION
Free-Body Diagram
1.4
tan
4.8
16.2602
1.6
tan
3
28.073
α
α
β
β
=
= °
=
= °
Force Triangle
Law of sines:
1.98 kN
sin 61.927 sin 73.740 sin 44.333
(a)
1.98 kN
sin 61.927
°
2.50 kN AC T = 
(b)
1.98 kN
sin 73.740
°
2.72 kN BC T = 

51. PROBLEM 2.48
Two cables are tied together at C and are loaded as shown.
Knowing that P = 500 N and α = 60°, determine the tension in
(a) in cable AC, (b) in cable BC.
AC BC T T = =
° °
sin 70 AC T = °
sin 70 BC T = °
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50
SOLUTION
Free-Body Diagram Force Triangle
Law of sines:
500 N
sin 35 sin 75 sin 70°
(a)
500 N
sin 35
°
305 N AC T = 
(b)
500 N
sin 75
°
514 N BC T = 

52. PROBLEM 2.49
Two forces of magnitude TA = 8 kips and TB = 15 kips are
applied as shown to a welded connection. Knowing that the
connection is in equilibrium, determine the magnitudes of the
forces TC and TD.
T
T = 5.87 kips C T 
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51
SOLUTION
Free-Body Diagram
0 1 ΣFx = 5 kips − 8 kips − TD cos 40° = 0
9.1379 kips D T =
0 ΣFy = sin 40 0 D C T ° − T =
(9.1379 kips) sin 40 0
5.8737 kips
° − =
=
C
C
9.14 kips D T = 

53. PROBLEM 2.50
Two forces of magnitude TA = 6 kips and TC = 9 kips are
applied as shown to a welded connection. Knowing that the
connection is in equilibrium, determine the magnitudes of the
forces TB and TD.
° − =
− − °=
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52
SOLUTION
Free-Body Diagram
Σ Fx = 0 6 kips cos 40 0 B D T − − T ° = (1)
0 Σ Fy = sin 40 9 kips 0
9 kips
sin 40
14.0015 kips
D
D
D
T
T
T
=
°
=
Substituting for TD into Eq. (1) gives:
6 kips (14.0015 kips) cos40 0
16.7258 kips
B
B
T
T
=
16.73 kips B T = 
14.00 kips D T = 

54. PROBLEM 2.51
Two cables are tied together at C and loaded as shown. Knowing
that P = 360 N, determine the tension (a) in cable AC, (b) in
cable BC.
13 5 x AC ΣF = − T + = 312 N AC T = 
13 5 y BC ΣF = + T + − =
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53
SOLUTION
Free Body: C
(a)
12 4
0: (360 N) 0
(b)
5 3
0: (312 N) (360 N) 480 N 0
480 N 120 N 216 N BC T = − − 144 N BC T = 

55. PROBLEM 2.52
Two cables are tied together at C and loaded as shown.
Determine the range of values of P for which both cables
remain taut.
13 5 ΣFx = − TAC + P =
13 5 y AC BC ΣF = T + T + P − =
   + + − =   
  
15 BCT = − P (2)
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54
SOLUTION
Free Body: C
12 4
0: 0
13
15 ACT = P (1)
5 3
0: 480 N 0
Substitute for AC T from (1):
5 13 3
480 N 0
13 15 5 P TBC P
14
480 N
From (1), 0 AC T requires P0.
From (2), 0 BC T requires
14
480 N, 514.29 N
15
P P
Allowable range: 0 P514 N 

56. PROBLEM 2.53
A sailor is being rescued using a boatswain’s chair that is
suspended from a pulley that can roll freely on the support
cable ACB and is pulled at a constant speed by cable CD.
Knowing that α = 30° and β =10° and that the combined
weight of the boatswain’s chair and the sailor is 900 N,
determine the tension (a) in the support cable ACB, (b) in the
traction cable CD.
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55
SOLUTION
Free-Body Diagram
0: cos 10 cos 30 cos 30 0 x ACB ACB CD ΣF = T ° −T ° −T ° =
0.137158 CD ACB T = T (1)
0: sin 10 sin 30 sin 30 900 0 ΣFy = TACB ° + TACB ° + TCD ° − =
0.67365 0.5 900 ACB CD T + T = (2)
(a) Substitute (1) into (2): 0.67365 0.5(0.137158 ) 900 ACB ACB T + T =
1212.56 N ACB T = 1213 N ACB T = 
(b) From (1): 0.137158(1212.56 N) CD T = 166.3 N CD T = 

57. PROBLEM 2.54
A sailor is being rescued using a boatswain’s chair that is
suspended from a pulley that can roll freely on the support
cable ACB and is pulled at a constant speed by cable CD.
Knowing that α = 25° and β =15° and that the tension in
cable CD is 80 N, determine (a) the combined weight of the
boatswain’s chair and the sailor, (b) in tension in the support
cable ACB.
+ °− =
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56
SOLUTION
Free-Body Diagram
0: cos 15 cos 25 (80 N) cos 25 0 x ACB ACB ΣF = T ° −T ° − ° =
1216.15 N ACB T =
0: (1216.15 N) sin 15 (1216.15 N)sin 25 ΣFy = ° + °
(80 N) sin 25 0
862.54 N
W
W
=
(a) W = 863 N 
(b) 1216 N ACB T = 

58. PROBLEM 2.55
Two forces P and Q are applied as shown to an aircraft
connection. Knowing that the connection is in equilibrium and
that P = 500 lb and Q = 650 lb, determine the magnitudes of
the forces exerted on the rods A and B.
= − + °
− °
+ − ° + ° =
R j i
j
i i j
= + °
B A F = F ° − °
= °− °
= 419.55 lb 420 lb B F = 
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57
SOLUTION
Free-Body Diagram
Resolving the forces into x- and y-directions:
0 A B R = P +Q + F + F =
Substituting components: (500 lb) [(650 lb) cos50 ]
[(650 lb) sin 50 ]
( cos50) ( sin50) 0 B A A F F F
In the y-direction (one unknown force):
500 lb (650 lb)sin 50 sin 50 0 A − − ° + F ° =
Thus,
500 lb (650 lb) sin 50
sin 50 A F
°
=1302.70 lb 1303 lb A F = 
In the x-direction: (650 lb)cos50 cos50 0 B A ° + F − F ° =
Thus, cos50 (650 lb) cos50
(1302.70 lb) cos50 (650 lb) cos50

59. PROBLEM 2.56
Two forces P and Q are applied as shown to an aircraft
connection. Knowing that the connection is in equilibrium
and that the magnitudes of the forces exerted on rods A and B
are 750 A F = lb and 400 B F = lb, determine the magnitudes of
P and Q.
= −P + Q ° −Q °
− °
+ °+
R j i j
i
j i
Q
= ° −
P = −Q ° + °
= − °+ °
= P = 477 lb; Q =127.7 lb 
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58
SOLUTION
Free-Body Diagram
Resolving the forces into x- and y-directions:
R = P +Q + FA + FB = 0
Substituting components: cos 50 sin 50
[(750 lb)cos 50 ]
[(750 lb)sin 50 ] (400 lb)
In the x-direction (one unknown force):
Q cos 50° −[(750 lb) cos 50°] + 400 lb = 0
(750 lb) cos 50 400 lb
cos 50
127.710 lb
°
=
In the y-direction: −P −Q sin 50° + (750 lb) sin 50° = 0
sin 50 (750 lb) sin 50
(127.710 lb)sin 50 (750 lb)sin 50
476.70 lb

60. PROBLEM 2.57
Two cables tied together at C are loaded as shown. Knowing that
the maximum allowable tension in each cable is 800 N, determine
(a) the magnitude of the largest force P that can be applied at C,
(b) the corresponding value of α.
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59
SOLUTION
Free-Body Diagram: C Force Triangle
Force triangle is isosceles with
2 180 85
47.5
β
β
= °− °
= °
(a) P = 2(800 N)cos 47.5° = 1081 N
Since P0, the solution is correct. P =1081 N 
(b) α =180° − 50° − 47.5° = 82.5° α = 82.5° 

61. PROBLEM 2.58
Two cables tied together at C are loaded as shown. Knowing that
the maximum allowable tension is 1200 N in cable AC and 600 N
in cable BC, determine (a) the magnitude of the largest force P
that can be applied at C, (b) the corresponding value of α.
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60
SOLUTION
Free-Body Diagram Force Triangle
(a) Law of cosines: 2 (1200 N)2 (600 N)2 2(1200 N)(600 N) cos 85
1294.02 N
P
P
= + − °
=
Since P1200 N, the solution is correct.
P =1294 N 
(b) Law of sines:
sin sin 85
1200 N 1294.02 N
67.5
180 50 67.5
β
β
α
= °
= °
= ° − ° − ° α = 62.5° 

62. PROBLEM 2.59
For the situation described in Figure P2.45, determine (a) the
value of α for which the tension in rope BC is as small as
possible, (b) the corresponding value of the tension.
PROBLEM 2.45 Knowing that α = 20°, determine the tension
(a) in cable AC, (b) in rope BC.
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61
SOLUTION
Free-Body Diagram Force Triangle
To be smallest, BC T must be perpendicular to the direction of . AC T
(a) Thus, α = 5° α = 5.00° 
(b) (1200 lb)sin 5 BC T = ° 104.6 lb BC T = 

63. PROBLEM 2.60
For the structure and loading of Problem 2.46, determine (a) the value of α for
which the tension in cable BC is as small as possible, (b) the corresponding
value of the tension.
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62
SOLUTION
BC T must be perpendicular to AC F to be as small as possible.
Free-Body Diagram: C Force Triangle is a right triangle
To be a minimum, BC T must be perpendicular to . AC F
(a) We observe: α = 90° − 30° α = 60.0° 
(b) (300 lb)sin 50 BC T = °
or 229.81 lb BC T = 230 lb BC T = 

64. PROBLEM 2.61
For the cables of Problem 2.48, it is known that the maximum
allowable tension is 600 N in cable AC and 750 N in cable BC.
Determine (a) the maximum force P that can be applied at C,
(b) the corresponding value of α.
β = ° + °
β = 46.0° ∴ α = 46.0° + 25° α = 71.0° 
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63
SOLUTION
Free-Body Diagram Force Triangle
(a) Law of cosines P2 = (600)2 + (750)2 − 2(600)(750) cos (25° + 45°)
P = 784.02 N P = 784 N 
(b) Law of sines
sin sin (25 45 )
600 N 784.02 N

65. PROBLEM 2.62
A movable bin and its contents have a combined weight of 2.8 kN.
Determine the shortest chain sling ACB that can be used to lift the
loaded bin if the tension in the chain is not to exceed 5 kN.
α = h
=
AC
=
=
= °
h
° = ∴ h =
= AC = +
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64
SOLUTION
Free-Body Diagram
tan
0.6 m
(1)
Isosceles Force Triangle
Law of sines:
1
2
1
2
(2.8 kN)
sin
5 kN
(2.8 kN)
sin
5 kN
16.2602
AC
T
T
α
α
α
From Eq. (1): tan16.2602 0.175000 m
0.6 m
Half length of chain (0.6 m)2 (0.175 m)2
0.625 m
=
Total length: = 2× 0.625 m 1.250 m 

66. PROBLEM 2.63
Collar A is connected as shown to a 50-lb load and can slide on
a frictionless horizontal rod. Determine the magnitude of the
force P required to maintain the equilibrium of the collar when
(a) x = 4.5 in., (b) x =15 in.
SOLUTION
(a) Free Body: Collar A Force Triangle
P = P = 10.98 lb 
P = P = 30.0 lb 
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65
50 lb
4.5 20.5
(b) Free Body: Collar A Force Triangle
50 lb
15 25


67. PROBLEM 2.64
Collar A is connected as shown to a 50-lb load and can slide on a
frictionless horizontal rod. Determine the distance x for which the
collar is in equilibrium when P = 48 lb.
x =
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66
SOLUTION
Free Body: Collar A Force Triangle
2 (50)2 (48)2 196
14.00 lb
N
N
= − =
=
Similar Triangles
48 lb
20 in. 14 lb
x = 68.6 in. 

68. PROBLEM 2.65
Three forces are applied to a bracket as shown. The directions of the two 150-N
forces may vary, but the angle between these forces is always 50°. Determine the
range of values of α for which the magnitude of the resultant of the forces acting at A
is less than 600 N.
SOLUTION
Combine the two 150-N forces into a resultant force Q:
Q= °
=
° + = − °
° + = °− °
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67
2(150 N) cos25
271.89 N
Equivalent loading at A:
Using the law of cosines:
(600 N)2 (500 N)2 (271.89 N)2 2(500 N)(271.89 N) cos(55 )
cos(55 ) 0.132685
α
α
= + + ° +
° + =
Two values for α : 55 82.375
27.4
α
α
° + =
= °
or 55 82.375
55 360 82.375
222.6
α
α
α
= °
For R 600 lb: 27.4° α 222.6 

69. PROBLEM 2.66
A 200-kg crate is to be supported by the rope-and-pulley arrangement shown.
Determine the magnitude and direction of the force P that must be exerted on the free
end of the rope to maintain equilibrium. (Hint: The tension in the rope is the same on
each side of a simple pulley. This can be proved by the methods of Ch. 4.)
xF P P α
α
α
 
Σ =   + ° − =
 
Σ =   + − ° − =
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SOLUTION
Free-Body Diagram: Pulley A
5
0: 2 cos 0
281
cos 0.59655
53.377
 
Σ = −   + =
 
=
= ± °
For α = +53.377°:
16
0: 2 sin 53.377 1962 N 0
281 yF P P
 
P = 724 N 53.4° 
For α = −53.377°:
16
0: 2 sin( 53.377 ) 1962 N 0
281 yF P P
 
P =1773 53.4° 

70. Σ = − =
Σ = − =
Σ = − =
Σ = − =
Σ = − =
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69
PROBLEM 2.67
A 600-lb crate is supported by several rope-and-pulley
arrangements as shown. Determine for each
arrangement the tension in the rope. (See the hint
for Problem 2.66.)
SOLUTION
Free-Body Diagram of Pulley
(a) 0: 2 (600 lb) 0
1
(600 lb)
2
Fy T
T
=
T = 300 lb 
(b) 0: 2 (600 lb) 0
1
(600 lb)
2
Fy T
T
=
T = 300 lb 
(c) 0: 3 (600 lb) 0
1
(600 lb)
3
Fy T
T
=
T = 200 lb 
(d) 0: 3 (600 lb) 0
1
(600 lb)
3
Fy T
T
=
T = 200 lb 
(e) 0: 4 (600 lb) 0
1
(600 lb)
4
Fy T
T
=
 T =150.0 lb 

71. Σ = − =
Σ = − =
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PROBLEM 2.68
Solve Parts b and d of Problem 2.67, assuming that
the free end of the rope is attached to the crate.
PROBLEM 2.67 A 600-lb crate is supported by
several rope-and-pulley arrangements as shown.
Determine for each arrangement the tension in the
rope. (See the hint for Problem 2.66.)
SOLUTION
Free-Body Diagram of Pulley and Crate
(b) 0: 3 (600 lb) 0
1
(600 lb)
3
Fy T
T
=
T = 200 lb 
(d) 0: 4 (600 lb) 0
1
(600 lb)
4
Fy T
T
=
T =150.0 lb 


72. PROBLEM 2.69
A load Q is applied to the pulley C, which can roll on the
cable ACB. The pulley is held in the position shown by a
second cable CAD, which passes over the pulley A and
supports a load P. Knowing that P = 750 N, determine
(a) the tension in cable ACB, (b) the magnitude of load Q.
Σ = °+ ° + °− =
Fy TACB Q
° + ° + ° − =
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71
SOLUTION
Free-Body Diagram: Pulley C

(a) 0: (cos 25 cos55 ) (750 N)cos55° 0 x ACB ΣF = T ° − ° − =
Hence: 1292.88 N ACB T =
1293 N ACB T = 
(b) 0: (sin 25 sin55 ) (750 N)sin 55 0
(1292.88 N)(sin 25 sin 55 ) (750 N) sin 55 Q
0
or Q = 2219.8 N Q = 2220 N 

73. PROBLEM 2.70
An 1800-N load Q is applied to the pulley C, which can roll
on the cable ACB. The pulley is held in the position shown
by a second cable CAD, which passes over the pulley A and
supports a load P. Determine (a) the tension in cable ACB,
(b) the magnitude of load P.
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72
SOLUTION
Free-Body Diagram: Pulley C
0: ΣFx = TACB (cos 25° − cos55°) − Pcos55° = 0
or 0.58010 ACB P = T (1)
0: (sin 25 sin 55 ) sin 55 1800 N 0 ΣFy = TACB ° + ° + P ° − =
or 1.24177 0.81915 1800 N ACB T + P = (2)
(a) Substitute Equation (1) into Equation (2):
1.24177 0.81915(0.58010 ) 1800 N ACB ACB T + T =
Hence: 1048.37 N ACB T =
1048 N ACB T = 
(b) Using (1), P = 0.58010(1048.37 N) = 608.16 N
P = 608 N 

74. PROBLEM 2.71
Determine (a) the x, y, and z components of the 900-N force, (b) the
angles θx, θy, and θz that the force forms with the coordinate axes.
F F
F
Fx = Fh °
=
= −130.091 N, x F 130.1N x F = − 
F F
F
= °
= °
= +
F F
z h
F 357 N z F = + 
θ = = − 98.3 x θ = ° 
θ = = + 66.6 z θ
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73
SOLUTION
cos 65
(900 N) cos 65
380.36 N
h
h
= °
= °
=
(a) sin 20
(380.36 N)sin 20°
sin 65
(900 N) sin 65°
815.68 N,
y
y
= °
=
= + 816 N y F = + 
cos 20
(380.36 N)cos 20
357.42 N
z
(b)
130.091 N
cos
900 N
x
x
F
F
815.68 N
cos
900 N
y
y
F
F
θ = = + 25.0 y θ = ° 
357.42 N
cos
900 N
z
z
F
F
= ° 

75. PROBLEM 2.72
Determine (a) the x, y, and z components of the 750-N force, (b) the
angles θx, θy, and θz that the force forms with the coordinate axes.
F F
F
= °
=
x h F F
F F
F
F F
z h
F
θ = = + 58.7 x θ = ° 
θ = = + 76.0 z θ
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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74
SOLUTION
sin 35
(750 N)sin 35
430.18 N
h
h
= °
= °
=
(a) cos 25
(430.18 N) cos 25°
= +389.88 N, x F 390 N x F = + 

cos35
(750 N) cos 35°
614.36 N,
y
y
= °
=
= + 614 N Fy = + 
sin 25
(430.18 N)sin 25
181.802 N
z
= °
= °
= +
181.8 N z F = + 
(b)
389.88 N
cos
750 N
x
x
F
F
614.36 N
cos
750 N
y
y
F
F
θ = = + 35.0 y θ = ° 
181.802 N
cos
750 N
z
z
F
F
= ° 

76. PROBLEM 2.73
A gun is aimed at a point A located 35° east of north. Knowing that the barrel of the gun forms an angle of 40°
with the horizontal and that the maximum recoil force is 400 N, determine (a) the x, y, and z components of
that force, (b) the values of the angles θx, θy, and θz defining the direction of the recoil force. (Assume that the
x, y, and z axes are directed, respectively, east, up, and south.)
∴ FH = °
x H F = −F °
= − °
yF = −F °
= − °
= − 257 N Fy = − 
z H F = +F °
= + °
= + 251N z F = + 
θ = = − 116.1 x θ = ° 
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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75
SOLUTION
Recoil force F = 400 N
(400 N)cos40
306.42 N
=
(a) sin 35
(306.42 N)sin 35
= −175.755 N 175.8 N x F = − 
sin 40
(400 N)sin 40
257.12 N
cos35
(306.42 N)cos35
251.00 N
(b)
175.755 N
cos
400 N
x
x
F
F
257.12 N
cos
400 N
y
y
F
F
θ = = − 130.0 y θ = ° 
251.00 N
cos
400 N
z
z
F
F
θ = = 51.1 z θ
= °

77. PROBLEM 2.74
Solve Problem 2.73, assuming that point A is located 15° north of west and that the barrel of the gun forms an
angle of 25° with the horizontal.
PROBLEM 2.73 A gun is aimed at a point A located 35° east of north. Knowing that the barrel of the gun
forms an angle of 40° with the horizontal and that the maximum recoil force is 400 N, determine (a) the x, y,
and z components of that force, (b) the values of the angles θx, θy, and θz defining the direction of the recoil
force. (Assume that the x, y, and z axes are directed, respectively, east, up, and south.)
H ∴ F = °
x H F = +F °
= + °
= +350.17 N 350 N x F = + 
yF = −F °
= − °
= − 169.0 N Fy = − 
z H F = +F °
= + °
= + 93.8 N z F = + 
θ = = + 28.9 x θ = ° 
θ = = + 76.4 z θ
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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76
SOLUTION
Recoil force F = 400 N
(400 N)cos25
362.52 N
=
(a) cos15
(362.52 N) cos15
sin 25
(400 N)sin 25
169.047 N
sin15
(362.52 N)sin15
93.827 N
(b)
350.17 N
cos
400 N
x
x
F
F
169.047 N
cos
400 N
y
y
F
F
θ = = − 115.0 y θ = ° 
93.827 N
cos
400 N
z
z
F
F
= °

78. PROBLEM 2.75
Cable AB is 65 ft long, and the tension in that cable is 3900 lb.
Determine (a) the x, y, and z components of the force exerted
by the cable on the anchor B, (b) the angles , x θ , y θ and z θ
defining the direction of that force.
θ
θ
Fx = −F θ y °
= − ° °
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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77
SOLUTION

From triangle AOB:
56 ft
cos
65 ft
0.86154
30.51
y
y
=
=
= °
(a) sin cos 20
(3900 lb)sin 30.51 cos 20
1861 lb x F = − 
cos (3900 lb)(0.86154) Fy = +F θ y = 3360 lb Fy = + 
(3900 lb)sin 30.51° sin 20° z F = + 677 lb z F = + 
(b)
1861 lb
cos 0.4771
3900 lb
x
x
F
F
θ = =− =− 118.5 x θ = ° 
From above: 30.51 y θ = ° 30.5 y θ = ° 
677 lb
cos 0.1736
3900 lb
z
z
F
F
θ = =+ =+ 80.0 z θ
= ° 

79. PROBLEM 2.76
Cable AC is 70 ft long, and the tension in that cable is 5250 lb.
Determine (a) the x, y, and z components of the force exerted by
the cable on the anchor C, (b) the angles θx, θy, and θz defining the
direction of that force.
θ
θ
=
= °
=
= °
=
θ = = − 117.4 x θ = ° 
θ = = − 112.7 z θ
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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78
SOLUTION

In triangle AOB: 70 ft
56 ft
5250 lb
AC
OA
F
=
=
=
56 ft
cos
70 ft
36.870
sin
(5250 lb) sin 36.870
3150.0 lb
y
y
FH F θ
y
(a) sin 50 (3150.0 lb)sin 50 2413.04 lb x H F = −F ° = − ° = − 2413 lb x F = − 
cos (5250 lb) cos36.870 4200.0 lb Fy = +F θ y = + ° = + 4200 lb Fy = + 
cos50 3150cos50 2024.8 lb z H F = −F ° = − ° = − 2025 lb z F = − 
(b)
2413.04 lb
cos
5250 lb
x
x
F
F
From above:
36.870 y θ = ° 36.9 y θ = ° 
2024.8 lb
5250 lb
z
z
F
F
= ° 

80. PROBLEM 2.77
The end of the coaxial cable AE is attached to the pole AB, which is
strengthened by the guy wires AC and AD. Knowing that the tension
in wire AC is 120 lb, determine (a) the components of the force
exerted by this wire on the pole, (b) the angles θx, θy, and θz that the
force forms with the coordinate axes.
SOLUTION
(a) (120 lb) cos 60 cos 20 x F= ° °
56.382 lb x F = 56.4 lb x F = + 
(120 lb)sin 60
103.923 lb
F
F
F
F
θ = = − 99.8 z θ
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79
y
y
= − °
= − Fy = −103.9 lb 
(120 lb) cos 60 sin 20
20.521 lb
z
z
= − ° °
= − 20.5 lb z F = − 
(b)
56.382 lb
cos
120 lb
x
x
F
F
θ = = 62.0 x θ = ° 
103.923 lb
cos
120 lb
y
y
F
F
θ = = − 150.0 y θ = ° 
20.52 lb
cos
120 lb
z
z
F
F
= ° 

81. PROBLEM 2.78
The end of the coaxial cable AE is attached to the pole AB, which is
strengthened by the guy wires AC and AD. Knowing that the tension
in wire AD is 85 lb, determine (a) the components of the force
exerted by this wire on the pole, (b) the angles θx, θy, and θz that the
force forms with the coordinate axes.
SOLUTION
(a) (85 lb)sin 36 sin 48 x F= ° °
= 37.129 lb 37.1 lb x F = 
F = − (85 lb)cos 36
°
y = − 68.766 lb
Fy = − 68.8 lb 
F= (85 lb)sin 36 ° cos 48
°
z = 33.431 lb
F = 33.4 lb 
z PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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80
(b)
37.129 lb
cos
85 lb
x
x
F
F
θ = = 64.1 x θ = ° 
68.766 lb
cos
85 lb
y
y
F
F
θ = = − 144.0 y θ = ° 
33.431 lb
cos
85 lb
z
z
F
F
θ = = 66.8 z θ
= ° 

82. = + −
= + +
= + + −
=
F i j k
(690 N) (300 N) (580 N)
x y z F F F F
θ = = − 127.6 z θ
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81
PROBLEM 2.79
Determine the magnitude and direction of the force F = (690 lb)i + (300 lb)j – (580 lb)k.
SOLUTION
2 2 2
2 2 2
(690 N) (300 N) ( 580 N)
950 N
F = 950 N 
690 N
cos
950 N
x
x
F
F
θ = = 43.4 x θ = ° 
300 N
cos
950 N
y
y
F
F
θ = = 71.6 y θ = ° 
580 N
cos
950 N
z
z
F
F
= ° 

83. = − +
= + +
= +− +
F (650 N) i (320 N) j (760 N)
k
F Fx Fy Fz
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82
PROBLEM 2.80
Determine the magnitude and direction of the force F = (650 N)i − (320 N)j + (760 N)k.
SOLUTION
2 2 2
2 2 2
(650 N) ( 320 N) (760 N)
F =1050 N 
650 N
cos
1050 N
x
x
F
F
θ = = 51.8 x θ = ° 
320 N
cos
1050 N
y
y
F
F
θ = = − 107.7 y θ = ° 
760 N
cos
1050 N
z
z
F
F
θ = = 43.6 z θ
= ° 

84. θ + θ + θ
=
cos cos cos 1
x y z
° + + ° =
= θ
=
F = 416.09 lb
y y F F
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83
PROBLEM 2.81
A force acts at the origin of a coordinate system in a direction defined by the angles θx = 75° and θz = 130°.
Knowing that the y component of the force is +300 lb, determine (a) the angle θy, (b) the other components
and the magnitude of the force.
SOLUTION
2 2 2
2 2 2
cos (75 ) cos cos (130 ) 1
cos 0.72100
y
y
θ
θ
= ±
(a) Since Fy 0, we choose cos 0.72100 y θ 43.9 y ∴ θ = ° 
(b) cos
300 lb F
(0.72100)
F = 416 lb 
cos 416.09 lbcos75 x x F = F θ = ° 107.7 lb x F = + 
cos 416.09 lbcos130 z z F = F θ = ° 267 lb z F = − 

85. θ + θ + θ
=
θ
+ °+ °=
cos cos cos 1
x y z
cos cos 55 cos 45 1
θ
= θ
x x F F
− = −
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84
PROBLEM 2.82
A force acts at the origin of a coordinate system in a direction defined by the angles θy = 55° and θz = 45°.
Knowing that the x component of the force is −500 N, determine (a) the angle θx, (b) the other components
and the magnitude of the force.
SOLUTION
2 2 2
2 2 2
cos 0.41353
x
x
= ±
(a) Since Fy 0, we choose cos 0.41353 x θ 114.4 x ∴ θ = ° 
(b) cos
500 N F
( 0.41353)
F =1209.10 N
F =1209.1N 
cos 1209.10 Ncos55 Fy = F θ y = ° 694 N Fy = + 
cos 1209.10 Ncos45 z z F = F θ = ° 855 N z F = + 

86. PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited
distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual,
you are using it without permission.
85
PROBLEM 2.83
A force F of magnitude 230 N acts at the origin of a coordinate system. Knowing that θx = 32.5°, Fy = −60 N,
and Fz 0, determine (a) the components Fx and Fz, (b) the angles θy and θz.
SOLUTION
(a) We have
Fx = F cosθ x = (230 N) cos32.5° 194.0 N x F = − 
Then: 193.980 N x F =
2 2 2 2
F = Fx + Fy + Fz
So: (230 N)2 (193.980 N)2 ( 60 N)2 2 z = + − + F
Hence: (230 N)2 (193.980 N)2 ( 60 N)2 z F = + − − − 108.0 N z F = 
(b) 108.036 N z F =
60 N
cos 0.26087
230 N
y
y
F
F
θ = = − = − 105.1 y θ = ° 
108.036 N
cos 0.46972
230 N
z
z
F
F
θ = = = 62.0 z θ
= ° 

87. PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited
distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual,
you are using it without permission.
86
PROBLEM 2.84
A force F of magnitude 210 N acts at the origin of a coordinate system. Knowing that Fx = 80 N, θz = 151.2°,
and Fy 0, determine (a) the components Fy and Fz, (b) the angles θx and θy.
SOLUTION
(a) Fz = F cosθ z = (210 N)cos151.2°
= −184.024 N 184.0 N z F = − 
Then: 2 2 2 2
F = Fx + Fy + Fz
So: (210 N)2 (80 N)2 ( )2 (184.024 N)2 = + Fy +
Hence: (210 N)2 (80 N)2 (184.024 N)2 y F = − − −
= −61.929 N 62.0 lb Fy = − 
(b)
80 N
cos 0.38095
210 N
x
x
F
F
θ = = = 67.6 x θ = ° 
61.929 N
cos 0.29490
210 N
y
y
F
F
θ = = =− 107.2 y θ = ° 

88. PROBLEM 2.85
In order to move a wrecked truck, two cables are attached at A
and pulled by winches B and C as shown. Knowing that the
tension in cable AB is 2 kips, determine the components of the
force exerted at A by the cable.

= = − + +
i j k λ
AB
AB
T
= = − + +
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87
SOLUTION
Cable AB:
( 46.765 ft) (45 ft) (36 ft)
74.216 ft
46.765 45 36
74.216
AB
AB AB AB
i j k
T λ
( ) 1.260 kips AB x T = − 
( ) 1.213 kips TAB y = + 
( ) 0.970 kips AB z T = + 

89. PROBLEM 2.86
In order to move a wrecked truck, two cables are attached at A
and pulled by winches B and C as shown. Knowing that the
tension in cable AC is 1.5 kips, determine the components of
the force exerted at A by the cable.

= = − + + −
i j k λ
AC
AC
T
= = − + −
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
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88
SOLUTION
Cable AB:
( 46.765 ft) (55.8 ft) ( 45 ft)
85.590 ft
46.765 55.8 45
(1.5 kips)
85.590
AC
AC AC AC
i j k
T λ
( ) 0.820 kips AC x T = − 
( ) 0.978 kips TAC y = + 
( ) = −0.789 kips AC z T 

90. PROBLEM 2.87
Knowing that the tension in cable AB is 1425 N, determine the
components of the force exerted on the plate at B.
= − + +
= + +
=
=
=
i j k
(900 mm) (600 mm) (360 mm)
(900 mm) (600 mm) (360 mm)
1140 mm
BA
BA
T λ
BA BA BA
BA
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89
SOLUTION
2 2 2
1425 N
[ (900 mm) (600 mm) (360 mm) ]
1140 mm
(1125 N) (750 N) (450 N)
BA
T
BA
T
BA
= − + +
= − + +
T i j k
i j k


( ) TBA x = −1125 N, (TBA )y = 750 N, (TBA )z = 450 N 

91. PROBLEM 2.88
Knowing that the tension in cable AC is 2130 N, determine the
components of the force exerted on the plate at C.
= − + −
= + +
=
=
=
i j k
(900 mm) (600 mm) (920 mm)
(900 mm) (600 mm) (920 mm)
1420 mm
CA
CA
T λ
CA CA CA
CA
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90
SOLUTION
2 2 2
2130 N
[ (900 mm) (600 mm) (920 mm) ]
1420 mm
(1350 N) (900 N) (1380 N)
CA
T
CA
T
CA
= − + −
= − + −
T i j k
i j k


( TCA )x = −1350 N, (TCA )y = 900 N, (TCA )z = −1380 N 

92. PROBLEM 2.89
A frame ABC is supported in part by cable DBE that passes
through a frictionless ring at B. Knowing that the tension in the
cable is 385 N, determine the components of the force exerted by
the cable on the support at D.
= − +
= + +
=
=
=
i j k
(480 mm) (510 mm) (320 mm)
(480 mm) (510 mm ) (320 mm)
770 mm
DB
F λ
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91
SOLUTION
2 2 2
385 N
[(480 mm) (510 mm) (320 mm) ]
770 mm
(240 N) (255 N) (160 N)
DB
DB
F
DB
F
DB
= − +
= − +
i j k
i j k


Fx = +240 N, Fy = −255 N, Fz = +160.0 N 

93. PROBLEM 2.90
For the frame and cable of Problem 2.89, determine the components
of the force exerted by the cable on the support at E.
PROBLEM 2.89 A frame ABC is supported in part by cable DBE
that passes through a frictionless ring at B. Knowing that the tension
in the cable is 385 N, determine the components of the force exerted
by the cable on the support at D.
= − +
= + +
=
=
=
i j k
(270 mm) (400 mm) (600 mm)
(270 mm) (400 mm) (600 mm)
770 mm
EB

F λ

PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited
distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual,
you are using it without permission.
92
SOLUTION
2 2 2
385 N
[(270 mm) (400 mm) (600 mm) ]
770 mm
(135 N) (200 N) (300 N)
EB
EB
F
EB
F
EB
= − +
= − +
i j k
F i j k
Fx = +135.0 N, Fy = −200 N, Fz = +300 N 

94. PROBLEM 2.91
Find the magnitude and direction of the resultant of the two forces
shown knowing that P = 600 N and Q = 450 N.
= ° ° + ° + ° °
= + +
= ° ° + ° − ° °
= + −
= +
= + +
=
P i j k
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited
distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual,
you are using it without permission.
93
SOLUTION
(600 N)[sin 40 sin 25 cos 40 sin 40 cos 25 ]
(162.992 N) (459.63 N) (349.54 N)
(450 N)[cos55 cos30 sin 55 cos55 sin 30 ]
(223.53 N) (368.62 N) (129.055 N)
(386.52 N) (828.25 N) (220.49 N)
R (3
i j k
Q i j k
i j k
R P Q
i j k
86.52 N)2 (828.25 N)2 (220.49 N)2
940.22 N
+ +
= R = 940 N 
386.52 N
cos
940.22 N
x
x
R
R
θ = = 65.7 x θ = ° 
828.25 N
cos
940.22 N
y
y
R
R
θ = = 28.2 y θ = ° 
220.49 N
cos
940.22 N
z
z
R
R
θ = = 76.4 z θ
= ° 

95. PROBLEM 2.92
Find the magnitude and direction of the resultant of the two forces
shown knowing that P = 450 N and Q = 600 N.
= ° ° + ° + ° °
= + +
= ° ° + ° − ° °
= + −
= +
= + +
=
P i j k
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited
distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual,
you are using it without permission.
94
SOLUTION
(450 N)[sin 40 sin 25 cos40 sin 40 cos 25 ]
(122.244 N) (344.72 N) (262.154 N)
(600 N)[cos55 cos30 sin 55 cos55 sin 30 ]
(298.04 N) (491.49 N) (172.073 N)
(420.28 N) (836.21N) (90.081N)
R (
i j k
Q i j k
i j k
R P Q
i j k
420.28 N)2 + (836.21N)2 +
(90.081N)2
940.21N
= R = 940 N 
420.28
cos
940.21
x
x
R
R
θ = = 63.4 x θ = ° 
836.21
cos
940.21
y
y
R
R
θ = = 27.2 y θ = ° 
90.081
cos
940.21
z
z
R
R
θ = = 84.5 z θ
= ° 

96. PROBLEM 2.93
Knowing that the tension is 425 lb in cable AB and 510 lb in
cable AC, determine the magnitude and direction of the resultant
of the forces exerted at A by the two cables.
= (40 in.) i − (45 in.) j +
(60 in.)
k
= (40 in.) + (45 in.) + (60 in.) =
85 in.
= (100 in.) − (45 in.) +
(60 in.)
= (100 in.) + (45 in.) + (60 in.) =
125 in.
= = = − +

AB
AB
AC
AC
i j k
AB
T T

T i j k

912.92 lb x θ = = 48.2 x θ = ° 
912.92 lb y θ = =− 116.6 y θ = ° 
912.92 lb z θ
= = 53.4 z θ
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited
distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual,
you are using it without permission.
95
SOLUTION
2 2 2
2 2 2
(40 in.) (45 in.) (60 in.)
(425 lb)
AB AB AB AB
AB
85 in. i j k
T λ

(200 lb) (225 lb) (300 lb)
(100 in.) (45 in.) (60 in.)
(510 lb)
125 in.
(408 lb) (183.6 lb) (244.8 lb)
(608) (408.6 lb) (544.8 lb)
AB
AC AC AC AC
AC
AB AC
AC
T T
AC
 
 
 
= − +
 − +  = = =  
 
= − +
= + = − +
i j k
T λ
T i j k
R T T i j k
Then: R = 912.92 lb R = 913 lb 
and
608 lb
cos 0.66599
408.6 lb
cos 0.44757
544.8 lb
cos 0.59677
= ° 

97. PROBLEM 2.94
Knowing that the tension is 510 lb in cable AB and 425 lb in cable
AC, determine the magnitude and direction of the resultant of the
forces exerted at A by the two cables.
= (40 in.) i − (45 in.) j +
(60 in.)
k
= (40 in.) + (45 in.) + (60 in.) =
85 in.
= (100 in.) − (45 in.) +
(60 in.)
= (100 in.) + (45 in.) + (60 in.) =
125 in.
= = = − +

AB
AB
AC
AC
i j k
AB
T T

T i j k

912.92 lb x θ = = 50.6 x θ = ° 
912.92 lb y θ = − = − 117.6 y θ = ° 
912.92 lb z θ
= = 51.8 z θ
PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed,
reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited
distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual,
you are using it without permission.
96
SOLUTION
2 2 2
2 2 2
(40 in.) (45 in.) (60 in.)
(510 lb)
AB AB AB AB
AB
85 in. i j k
T λ

(240 lb) (270 lb) (360 lb)
(100 in.) (45 in.) (60 in.)
(425 lb)
125 in.
(340 lb) (153 lb) (204 lb)
(580 lb) (423 lb) (564 lb)
AB
AC AC AC AC
AC
AB AC
AC
T T
AC
 
 
 
= − +
 − +  = = =  
 
= − +
= + = − +
i j k
T λ
T i j k
R T T i j k
Then: R = 912.92 lb R = 913 lb 
and
580 lb
cos 0.63532
423 lb
cos 0.46335
564 lb
cos 0.61780
= ° 