PRO BLEM 2 - University of Massachusetts...
Transcript of PRO BLEM 2 - University of Massachusetts...
SOLUT
(a) P
(b) T
W
TION
arallelogram l
Triangle rule:
We measure:
PRO
Twomagn(b) th
law:
OBLEM 2.1
o forces are anitude and dirhe triangle rul
139R =
1
applied as shorection of theile.
1 kN, 47α =
own to a hooir resultant us
7.8°
ok. Determineing (a) the pa
1391 N=R
e graphically arallelogram la
N 47.8°
the aw,
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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: 20.1 kN,R = 21.2α = ° 20.1 kN=R 21.2°
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PROBLEM 2.7
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.
SOLUTION
Using the triangle rule and the law of sines:
(a) 75 40 180
180 75 40
65
ββ
° + ° + = °= ° − ° − °= °
11000 lbsin 75° sin 65
T=
° 1 938 lbT =
(b) 1000 lbsin 75° sin 40
R=
° 665 lbR =
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SOLUT
Using th
(a)
(b)
TION
he triangle rulee and the law
50β + °
4s
4s
P
Athmfom
of sines:
60 180
180
70
β° + ° = °
= °= °
425 lbsin 70 sin 6
P=
°
425 lbsin 70 sin 5
R=
°
PROBLEM
A steel tank is hat α = 20°, d
magnitude of forces applied magnitude of R
50 60− ° − °
0°
0°
2.11
to be positiondetermine by the force P iat A is to be v
R.
ned in an excavtrigonometry if the resultanvertical, (b) th
vation. Knowi(a) the requir
nt R of the the correspondi
392 lbP =
346 lbR =
ing red two ing
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SOLUT
Comput
800-N F
424-N F
408-N F
TION
te the followin
Force:
Force:
Force:
ng distances:
PROBL
Determin
2
(600)
1000 m
(560)
1060 m
(480)
1020 m
OA
OB
OC
=
=
=
=
=
=
(800 NxF = +
(800 NyF = +
(424 NxF = −
(424 NyF = −
(408 NxF = +
(408 NyF = −
LEM 2.22
ne the x and y
2 2
2 2
2 2
(800)
mm
(900)
mm
(900)
mm
+
+
+
800N)
1000
600N)
1000
560N)
1060
900N)
1060
480N)
1020
900N)
1020
components oof each of the
F
forces shown.
640 NxF = +
480 NyF = +
224 NxF = −
360 NyF = −
192.0 NxF = +
360 NyF = −
.
N
N
N
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SOLUT
Compon
TION
nents of the fo
F
2
5
5
orces were dete
Force x
29 lb
50 lb
51 lb
R
tan
PROBLE
Determine t
PROBLEMforces show
ermined in Pro
x Comp. (lb)
+21.0
–14.00
+24.0
31.0xR = +
(31.0 lb)
n
23.031.036.573
23.0 lbsin (36.57
x y
y
x
R R
RR
R
α
α
= +
=
=
=
= °
=
i j
i
R
38.601 lb=
EM 2.31
the resultant o
M 2.21 Determwn.
oblem 2.21:
y Comp
+20
+4
–4
2yR = +
(23.0 lb)
b73 )
+
°
i j
b
of the three for
mine the x and
p. (lb)
0.0
8.0
5.0
3.0
rces of Problem
d y componen
38.6=R
m 2.21.
nts of each of
6 lb 36.6°
the
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SOLUT
Determi
Cable fo
500-N F
200-N F
and
Further:
TION
ine force comp
orce AC:
Force:
Force:
ponents:
(365 N
(365 N
= −
= −
x
y
F
F
(500 N)
(500 N)
x
y
F
F
=
=
(200 N)
(200 N
x
y
F
F
=
= −
2
(400 N
474.37
= Σ = −
= Σ = −
= +
=
=
x x
y y
x
R FR F
R R R
255tan
40032.5
α
α
=
= °
PRKnoresu
960N) 24
14601100
N) 271460
= −
= −
24) 480 N
257
) 140 N25
=
=
4) 160 N
53
N) 120 N5
=
= −
2
2
240 N 480
275 N 140 N
N) ( 255 N
N
− +
− +
+ −
yR
°
ROBLEM 2.owing that theultant of the th
40 N
75 N
N
2
N 160 N 4
N 120 N
N)
+ =
− = −
36 tension in rop
hree forces exe
400 N
255 N−
pe AC is 365 Nerted at point C
474=R
N, determine C of post BC.
4 N 32.5°
the
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SOLUT
60-lb Fo
80-lb Fo
120-lb F
and
Further:
TION
orce:
orce:
Force:
(60 l
(60 lx
y
FF
=
=
(80 l
(80 lx
y
FF
=
=
(120
(12x
y
FF
=
= −
(20
202.
x x
y y
R FR F
R
= Σ
= Σ
=
=
29.tan
200α =
tan
8.46
α −=
= °
PROKnowiforces
lb)cos 20 5
lb)sin 20 20
° =
° =
lb)cos60 4
lb)sin 60 69
° =
° =
0 lb)cos30 1
20 lb)sin 30
° =
° =
2
200.305 lb
29.803 lb
00.305 lb) (
.510 lb
=
=
+
803.305
1 29.803200.305
°
BLEM 2.37ing that α =shown.
6.382 lb
0.521 lb
0.000 lb
9.282 lb
103.923 lb
60.000 lb= −
2(29.803 lb)
7 40°, determiine the result
203=R
ant of the th
3 lb 8.46°
hree
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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.
SOLUTION
Free-Body Diagram Force Triangle
Law of sines:
400 lbsin 60 sin 40 sin80
AC BCT T= =
° ° °
(a) 400 lb
(sin 60 )sin80ACT = °
° 352 lbACT =
(b) 400 lb
(sin 40 )sin80BCT = °
° 261 lbBCT =
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SOLUT
Law of s
(a)
(b)
TION
Free
sines:
e-Body Diagra
sin
PKAC
am
n 110 sin 5AC BCT T
=°
1200sin 6ACT =
1200sin 6BCT =
PROBLEM 2Knowing that α
C, (b) in rope
1200 lb5 sin 65
=° °
0 lbsin 110
65°
°
lbsin 5
65°
°
2.48 20 ,α = ° dete
BC.
Force Triang
rmine the ten
gle
T
T
sion (a) in ca
1244 lbACT =
115.4 lbBCT =
ble
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SOLUT
xFΣ
For P =
yFΣ
Solvin
TION
0 CAT= −
200N= we ha
0=
0.8
ng equations (
PRO
Two KnowBC.
sin30 CBT+D
ve,
0.5 CAT−
coCAT
86603 0.8CAT +
1) and (2) sim
BLEM 2.49
cables are wing that P =
Free-B
sin30 cosP−D
0.5 21A CBT+ +
os30 coCBT° −
86603 21CBT −
multaneously g
9
tied togeth= 300 N, de
Body Diagram
s 45 200N° − =
12.13 200− =
s30 sin 4P−D
12.13 0= (2)
ives,
her at C anetermine the
m
0=
0 (1)
5 0=D
)
nd are loadtension in c
T
T
ded as showcables AC a
134.6 NCAT =
110.4 NCBT =
wn. and
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SOLUT
Free-Bo (a)
(b)
(c)
(d )
(e)
TION
ody Diagram of Pulley
FΣ
FΣ
FΣ
FΣ
FΣ
0: 2yF T= −
0: 2yF T= −
0: 3yF T= −
0: 3yF T= −
0: 4yF T= −
PR
A 6andfor (Se
(600 lb) 0
12
T
− =
=
(600 lb) 0
12
T
− =
=
(600 lb) 0
1(
3T
− =
=
(600 lb) 0
1(
3T
− =
=
(600 lb) 0
14
T
− =
=
ROBLEM 2
600-lb crate id-pulley arrang
each arrangeee the hint for
(600 lb)
(600 lb)
(600 lb)
(600 lb)
(600 lb)
.67
is supported bgements as sh
ement the tensProblem 2.66
by several rophown. Determsion in the ro.)
300 lbT =
300 lbT =
200 lbT =
200 lbT =
150.0 lbT =
pe-ine pe.
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