Ejercicios De Trabajo Virtual
Chapter 10, Solution 1.
Link ABC: Assume δθ clockwise Then, for point C
δ xC = (125 mm ) δθ
and for point D
δ xD = δ xC = (125 mm ) δθ
and for point E
δ xE =
Link DEFG: Thus
250 mm 2 δ xD = δ xD 3 375 mm
δ xD = ( 375 mm ) δφ
(125 mm ) δθ = ( 375 mm ) δφ
δφ = δθ
1 3
Then
δ G = 100 2 mm δφ = 3 δ yG = δ G cos 45° =
(
)
100
2 mm δθ
100 100 2 mm δθ cos 45° = mm δθ 3 3
Virtual Work:
Assume P acts downward at G
δ U = 0:
( 9000 N ⋅ mm ) δθ − (180 N )(δ xE
mm ) + P (δ yG mm ) = 0
2 100 δθ = 0 9000 δθ − 180 × 125 δθ + P 3 3
or
P = 180.0 N
Vector Mechanics for Engineers: Statics and Dynamics, 8/e,Ferdinand P. Beer, E. Russell Johnston, Jr., Elliot R. Eisenberg, William E. Clausen, David Mazurek, Phillip J. Cornwell © 2007 The McGraw-Hill Companies.
COSMOS: Complete Online Solutions Manual Organization System
Chapter 10, Solution 2.
Have
FA = 20 lb at A
FD = 30 lb at D
Link ABC:
δ y A = (16 in.) δθ
Link BF:
δ yF = δ yB
δ yB = (10 in.) δθ
Link DEFG: or
δ yF =( 6 in.) δφ = (10 in.) δθ δφ = δθ δ yG = (12 in.) δφ = ( 20 in.) δθ
d ED = 5 3
( 5.5 in.)2 + ( 4.8 in.)2
5
= 7.3 in.
δ D = ( 7.3 in.) δφ = × 7.3 in. δθ 3 δ xD =
Virtual Work: 4.8 4.8 5 δD = × 7.3 in. δθ = ( 8 in.) δθ 7.3 7.3 3
Assume P acts upward at G
δ U = 0:
or or
FAδ y A + FDδ xD + Pδ yG = 0
( 20 lb ) (16 in.) δθ + ( 30 lb ) (8 in.) δθ + P( 20 in.) δθ = 0
P = − 28.0 lb
P = 28.0 lb
Vector Mechanics for Engineers: Statics and Dynamics, 8/e, Ferdinand P. Beer, E. Russell Johnston, Jr., Elliot R. Eisenberg, William E. Clausen, David Mazurek, Phillip J. Cornwell © 2007 The McGraw-Hill Companies.
COSMOS: Complete Online Solutions Manual Organization System
Chapter 10, Solution 3.
Link ABC: Assume δθ clockwiseThen, for point C
δ xC = (125 mm ) δθ
and for point D
δ xD = δ xC = (125 mm ) δθ
and for point E
δ xE =
Link DEFG: Thus or Virtual Work:
250 mm 2 δ xD = δ xD 3 375 mm
δ xD = ( 375 mm ) δφ
(125 mm ) δθ = ( 375 mm ) δφ
δφ = δθ
Assume M acts clockwise on link DEFG
1 3
δ U = 0:
( 9000 N ⋅ mm ) δθ − (180 N )(δ xE
mm ) + M δφ = 0
2 1 9000 δθ − 180 ⋅125 δθ + M δθ = 0 3 3
or
M = 18000 N ⋅ mm
or
M = 18.00 N ⋅ m
Vector Mechanics for Engineers: Statics and Dynamics, 8/e, Ferdinand P. Beer, E. Russell Johnston, Jr., Elliot R. Eisenberg, William E. Clausen, David Mazurek, Phillip J. Cornwell © 2007 The McGraw-Hill Companies.
COSMOS: Complete Online Solutions Manual Organization System
Chapter 10, Solution 4.
HaveFA = 20 lb at A FD = 30 lb
at D
Link ABC:
δ y A = (16 in.) δθ δ yB = (10 in.) δθ δ yF = ( 6 in.) δφ = (10 in.) δθ
or
Link BF:
δ yF = δ yB
Link DEFG:
δφ = δθ
5 3
d ED =
( 5.5 in.)2 + ( 4.8 in.)2
5 3
= 7.3 in.
δ D = ( 7.3 in.) δφ = × 7.3 in. δθ
δ xD =
Virtual Work: 4.8 4.8 5 δD = × 7.3 in. δθ = ( 8 in.) δθ 7.3 7.3 3 on DEFG 5 δθ =0 3 M = 28.0 lb ⋅ ft
Assume M acts
δ U = 0:
or or
FAδ y A + FDδ xD + M δφ = 0
( 20 lb ) (16 in.) δθ + ( 30 lb ) (8 in.) δθ + M
M = − 336.0 lb ⋅ in.
Vector Mechanics for Engineers: Statics and Dynamics, 8/e, Ferdinand P. Beer, E. Russell Johnston, Jr., Elliot R. Eisenberg, William E. Clausen, David Mazurek, Phillip J. Cornwell © 2007 The McGraw-Hill Companies.COSMOS: Complete Online Solutions Manual Organization System
Chapter 10, Solution 5.
Assume δθ
δ x A = 10 δθ in.
δ yC = 4 δθ in.
δ yD = δ yC = 4 δθ in.
δφ =
δ yD
6
=
2 δθ 3 2
δ xG = 15 δφ = 15 δθ = 10 δθ in. 3
Virtual Work: Assume that force P is applied at A.
δ U = 0:
δ U = − Pδ x A + 30 δ yC + 60 δ yD + 240 δφ + 80 δ xG = 0
2 − P...
Regístrate para leer el documento completo.