experimental methods for engineers - solution manual testbank … · 2018-09-20 · instructor’s...
TRANSCRIPT
Instructor’s Solutions Manual
to accompany
Experimental Methods for
Engineers
Eighth Edition J. P. Holman
Professor of Mechanical Engineering
Southern Methodist University
Boston Burr Ridge, IL Dubuque, IA Madison, WI New York San Francisco St. Louis
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Chapter 2 2-3
x0 = 1
1
Amplitude ratio = Fk0 ìïïïïïíîï éêëê1 - ( ww1n )2
ùúúûú+ éêêë2(cac )( ww1n
)úùúûïïïïþüýïï ê
=
amplitude ratio 0.99 (Use Figure. 2-5)
F t( ) = F0 sin wt x t1 ;( ) = x0 sin(wt1 - )
time lag = txmax - tFmax
F t( ) = F0 = max (when sin wt1 = 1) \ wt1 = sin- 11 = ; tFmax
2
1
=
w1 2
æ1 öæ öæ tFmax = çççè40 øè
øè÷÷÷÷ççç
π2
÷÷÷÷ççç2
1π
öø
÷÷÷÷=
0.00625sec
x t( ) = x0 = max (whensin(wt1 - ) = 1 \ (wt1 - ) = sin- 11 =
1 æçççèπ2 + ÷÷÷÷öø
txmax = w1
2(ccc )(ww1n ) = tan- 1 2 = tan- 1
2 1 -
= 33.7° (Use Figure 2-6)
1 é æçççè180 öø÷÷÷÷ùúúû= 0.054 sec
txmax = 40 2êêë + 33.7
\ time lag = 0.54 - 0.000625 time lag = 0.0478sec
2-4
1 x0
=
SM: Experimental Methods for Engineers Chapter 2
2
F0
ìï 2 2 ïü
k
w1 = 0.306. which
gives
wn
wn = (100)(2 ) = 628 rad/sec
w1 = (0.306)(628) w1 = 192.1
rad/sec = 30.6 Hz
ïïîíïï éêëê1 - ( ww1n ) úúúûù + éêëê2(ccc
)( ww1n ) úúûúùïïïïïïþý k ïï ê ê
4
For xF00 = 1.00 + 0.01 = 1.01we have æççççè
ww1n öø÷÷÷÷÷ k w1 ® imaginary.
4
For xF00 = 1.00 - 0.01 = 0.99 we haveæççççè
ww1n öø÷÷÷÷÷ -
2
0.04
æèçççç ww1n ö÷÷÷÷÷ + 1 -
çççèæ1.011 øö÷÷÷÷2 = 0 and
ø
2
0.04 ø æèçççç ww1n ö÷÷÷÷÷ + 1 -
ççæèç0.991÷÷÷÷öø2 = 0
12 2
SM: Experimental Methods for Engineers Chapter 2
3
2-5
T - T¥ = e- ( RC1 )t
T - T
At t = 3sec,T = 200°F
T - T¥ = 0.435. At t
= T0 - T¥
T - T¥ =
0.1304 T0 - T¥
1 - 0.632 =
0.328 RC » 3.4
sec
2-6
P = EAB2
R
EAB = Eæççç
R
ö÷÷÷÷÷ çè R +
Ri ø
2
5sec, T = 270°F
P = RRi
0 ¥
1
1
i i
R
R R R +
ö æ ÷ ç ÷ ç ÷ ç ÷ ç ÷ ç ÷ ÷ ç ÷ ø è
SM: Experimental Methods for Engineers Chapter 2
4
2-7
®inch Readability
®inch Least count
2-8
t = RC = time constant t =
(106ohms)(10- 5f) = 10 sec
t = 10 sec
2-9
% error = éê(R + Ri) - R ùú´ 100 êêë
(R + Ri) úúû
=´ 100
ç
% error = 20%
2-10
E2
P = AB ; EAB = E +RRi
R R
E = 100 v
R = 20,000 ohms
Ri = 5000 ohms
P = E2 æç R ÷÷ö2 = 104
é 2 ´ 104 ù
ú= 0.32 Watts ê
Maximum power occurs when = 0 ® R = Ri dR
P =
max E2 æçççè2PR øö÷÷÷÷2 = 2.010´ 4104 = 5000
Watts
R
When R = 1000 ohms and Ri = 5000 ohms:
104 éê 103 ùú2 = 10 volts2 = 0.278 Watts
P = 3 ê6 ´ 103 úúû 36 ohm
10 êë
\ R = 5000 ohms
SM: Experimental Methods for Engineers Chapter 2
5
R Rèçç + Ri ÷÷ø
2(10)4
êêë2.5´ 104
úúû dP
mx + kx = 0
® wn = k
x + k x = 0 where wn2 = k
m m m
From the static deflection: k = mg where = deflection = 0.5 cm
k g g 980 seccm2
= ® wn = =
m 0.5 cm wn =
44.3 rad/sec
2-12
= 0.25 inch; g = 386 in/sec2
wn = g = 986 secin.2 = 39.4 rad/sec
0.25 in.
2-14
wn = 39.4 rad/sec = 6.27 Hz
w x0 for c = 0
w wn F0 cc
k
20 3.19 0.108
40 6.38 0.025
2-11
SM: Experimental Methods for Engineers Chapter 2
6
60 9.57 0.011
2-15
dV V - c
= - cV = e
d V0
dV
At = 0, V = 10 liters, = - 6
d
c = 0.6 hr- 1
2-16
(1 lbf/in )(4.448 N/lbf)(144 in /ft )(3.28 ft /2 2 2 2 2 m )2
= 6890 N/m2
1 kgf = 9.806 N
1 lbf/in2 = (6890)(9.806) = 67570 kgf/m2 = 6.757 kp/cm2
2-17
(mi/gal)(5280 ft/mi)çççèæ 2311 gal/in3÷÷÷÷öø(1728 in /ft3 3)
´ (35.313 ft /m33)æ
çççè10001
m /l3 ø÷÷÷
÷ö´ (3.2808´ 10- 3 km/ft)
= 4.576 km/l
2-18
æ lbm ft ö
2-19
æ 1 Btu ö æ5 ö
(kJ/kg·°C)çççè1.055 kJ
ø÷÷÷÷(0.454 kg/lbm) èççç9 °C/ F° ø
÷÷÷÷= 0.2391 Btu/lbm· F°
(kJ/kg·°C)çççæ4.1821 kcalkJ ø÷÷÷÷
öæççèçç1000
1
kgg ÷÷
÷÷öø= 2.391´ 10
- 4 kcal/g- C° è
(lbf-s/ft2) 32.17çççè lbf s2 ø÷
÷÷÷=
32.17 lbm/sft · ´
= 47.92 kg/ms·
(0.454 kg/lbm)(3.2808 ft/m)
SM: Experimental Methods for Engineers Chapter 2
7
2-20
3)æ
çççè4541
lbm/gö æ
ø (g/m )(0.02832 m /ft3 3
è÷÷÷÷´ ççç32.17
1 slug/lbm
öø
÷÷÷÷
= 1.939 ´ 10- 6 slug/ft3
2-21
sec/hö÷÷÷÷´ J/Btu° )ççæ 1(Btu/h-ft- F)(1055
(107
erg/J)æ
èççç9
5° °F/ Cöø
÷÷÷÷
çè3600 ø
æçççè12 ´
12.54 ft/cmø
ö÷÷÷÷= 5.275 ´ 10
6 erg/s·ft· C° ´
= 1.731´ 105 erg/s·cm· C°
2-22 2
/s2 )æ
çççè2.541´ 12 cm
ft ö÷÷÷÷ø = 1.076 ft /2 s (cm
2-23
(W/m3) 3.413ççèçæçW·hBtu ø÷÷÷÷öèæççç3.28081 mft ö÷÷÷ø÷3 =
0.09664 Btu/h·ft3
2-24
(dyn s/cm· 2)(10
- 5 N/dyn)(0.2248 lbf/N) ´ (2.54 ´ 12
cm/ft)2çç
æ32.17
lbm ft2
ö÷÷÷
= 0.0672 lbm/s ft· ´ 3600 s/h
lhm
= 241.8
h ft·
çè lbf s ø÷
2-25
W 3.413 Btu/W h·
´
c
m3
SM: Experimental Methods for Engineers Chapter 2
8
( 2.541 )2 cmin22 ´ 1441
inft22
W Btu/hr-ft2
´ =
cm2
2-26
R = 1545lbm molft-lbf·· R ´ 0.30480.454mftkg´
4.4485 ΚlbfN =
lbm ´ 9 R
2-27
cms 3æçççè öø÷÷÷÷3 cmin33 ´ 2311
gal in2
´
cm3
´ =
gal/min s
2-28
R = K
J
8305 kg mol · K
2-29
= 105, T0 = 30 C, T¥ = 100 C
Rise time 90 = 2.303 = 23.03s
0.01 = e- t
t
= 4.605
t(99 ) = 46.05 sec
2-30
A = 20 C = 0.01Hz = 0.0628 rad/s
= tan- 1
T
= tan-
1[(0.0628)(
10)]
= - 32.14 deg
= -
0.561rad
t =
=
= 8.93sec
0.0628
2-31
c
n = 10,000 Hz
= 0.3, 0.4
c
c
c
For= 0.3,
resonance
at = 0.9,
= 9000
Hz cc
n c
For= 0.4,
resonance at =
0.8, = 8000 Hz
cc
2-32
n
c
= 0.2 and 0.4 for
n c
c
At 2000 Hz
= 0.3
SM: Experimental Methods for Engineers Chapter 2
9
xF00 = = 1.034 k
= tan- 1 éêêë(2)(0.3)(0.2)1 - 0.22 ùúúû=
7.13deg At 4000 Hz
xF00 = = 1.145
k
= tan- 1
éêêë(2)(0.3)(0.4)
1 - 0.42 ùúúû=
15.9deg
2-33 xF00 = 0.4 21 == 1050
Hz Hz
k
From Fig. 2-6,
c
For = 1.0 cc
10
n = 33 Hz
0.3
2-34
= - 50 = - tan- 1
= 1.1918
= (2)(1.1918) = 2.3835
At amp response=
0.643
At amp response = 0.387
2-35
= 3 Hz = 18.85 rad/s = 0.5 sec
( ) = - tan - 1[(18.85)(0.5)] = - 8.39
1/2 = 0.1055
21 2 / 1
[1 2.384] +
0.3 n
>
<
21 2 / 1
[1 1.1918] +
SM: Experimental Methods for Engineers Chapter 2
10
2-36
T0 = 35 C T¥ = 110 C (8 secT ) = 75 C
= e- t/
t
= 0.7621
= 810.7621 = 10.497 sec 90 rise
time = 2.303 = 24.174 sec
2-38 static sens = 1.0
V/kgf
output = (10)(1.0) = 10.0 V
2-39 rise time =
0.003 ms e- t/ = e- Rc1
t = 0.1
1 = 7.86 ´ 105
RC
RC = 1.303 ´ 10- 6
R in ohm, C in farads
2-42
= 0.1sec
T t( ) = 17 C
T0 = 100 C T¥ = 15
C
= e- t/0.1
t
= 3.75
0.1
t = 0.375 sec
2-43
= 0.9
= 0.4843 to 4.84 rad/s
( ) = - tan- 1
(0.4843) = - 25.84 = 0.451 rad
0.451
Dt = = 0.093 sec
4.84
SM: Experimental Methods for Engineers Chapter 2
11
2-44
=
500
Hz
= 1500 Hz = 1
3
0.98 = ( ) 2 ( )( ) 2üïïï1/2
ìïïïíïîïï êéë1 - 13 2 úûùú +
ëêêé(2) ccc 13 úûùú ýïïþï ê
c
= 0.619 cc
2-45
t = 1´ 10- 6
sec = 90% rise time
1
- (1 10´ - 6)
24 (24)(3600)
t = 2 hr = 3600sec = ( )
( ) = 0.2618 rad = - tan( )
0.1 = e RC
RC = 4.34 ´ 10- 7
R in ohm, C in farads
2-46
t = 2 hr
1
cyc/hr 2 9.27 10- 5
rad/sec
= = = ´
1
n n
SM: Experimental Methods for Engineers Chapter 2
12
= 0.2679
0.2679
= = 3685sec = 1.024 hr
7.27 ´
Amp. response = = 0.966
2-47 m = 1.3 kg k = 100
N/m
k æ100 ö1/2
n = m = çççè1.3 ø÷÷÷÷= 8.77 rad/s
cc = 2 mk = 2[(1.3)(100)]1/2 = 72.11 c
= 1.0
cc
From Figure 2-8, n t = 3.6 for 90
3.6
t = = 0.41sec
8.77
2-48
c
= 0.1
cc From Figure 2-9, nt = 3.1.
3.1
t = = 0.353 sec
8.77
2-49
x t( ) c
= 0.9 = 1.5
x0 cc
From Figure 2-9 nt = 6.2,
2-50
t = 1sec, nt = 8.77 c 5.7
c = 5.7 = = cc
72.11
x
From Figure 2-9, » 1.8.
x0
2-51
Rise time = 10- 12 s
c x
6.2
t = = 0.71sec.
8.77
SM: Experimental Methods for Engineers Chapter 2
13
0.79
2-53
T0 = 20°C T¥ = 125°C e- t/ =
0.1
= 34.54 sec
= exp
T t20( )-- 125125 æçççè- t
öø÷÷÷÷=
T t( ) =
20.15°C
2-54
t = 0.05 sec
e- ( )
kg 2
1 = 0.02088 lbf sec/ft× m
s×
2-55
English units
= lbm/ft ,3 u = ft/sec x =
ft, = lbm/s-ft
SI units
= kg/m ,3 u = m/s
x = m, = kg/m-s
2-56
SI system
g = m/s ,2 = 1 / °C, = kg/m
3
T = °C, x = m, = kg/m-s
At = 1.0 cc and x0 nt 3.6, n = 3.7 ´ 10 rad/s = 0.9,
12
f = 5.7 ´ 1011 Hz = 570 GHz
2-52
m = 1000 lbm = 2203 kg
1000 lbf
÷÷÷÷ö1/2 = 7.29
rad/s
1.5 12
0
lbf/ft 8000 N/m 117,000
117,000
2203
0.9 1.0 At 3.6
3.6 0.495 s
7.29
n
n c
k
k
m
c x t
c x
t
= = =
æ ç = = ç ç ø è
= = »
= =
SM: Experimental Methods for Engineers Chapter 2
14
( 5 9
English system
g = ft/s ,2 = 1/ F,° = lbm/ft
3
T = °F, x = ft, = lbm/ft-s
2-57
W-cm 0.01 m/cm
´
in - F2 ° (2.54 cm/in.) (0.01 m/cm
2)2 °C/ F° )
W-cm in - F2
´ W/m-
C°
2-58
T0 = 45, T¥ = 100 rise time = 0.2 s T(0.1s) = ?
0.2 = 2.303 , = 0.0868 s
(T - 100)/(45 - 100) = exp( 0.1/0.0868)- = 0.316 T =
82.6ºC
2-59
m = 6000/4 = 1500 lbm = 3303 kg
k = 1500/(1/12) = 18,000 lb/ft = 263,250 N/m
n = (263250/3303)1/2 = 8.93 rad/s
For critically damped system:
0.9 = 1 - (1 + nt)exp( - nt)
Solution is nt = 3.8901
t = (3.8901)(8.93) = 0.435s
2-60
= 400 Hz, n = 1200 Hz / n = 400/1200 = 1/3
0.98 = 1/{[1 - (1/3) ]2 2 + [(2)(c c/ c)(1/3)] }2 1/2 c c/ c = 0.619
2-61
Insert function in Equations (2-38) and (2-39), manipulate algebra and the indicated result will be given.
2-62
t = 1.5 h, = 1/24 cyc/h = 2 /(24)(3600) = 7.27 ´ 10- 5
rad/sec
(1.5)(3600) = 5400 s = ( )/
( ) = (5400)(0.0000727) = 0.3926 = - tan- 1
( )
= 0.414
SM: Experimental Methods for Engineers Chapter 2
15
= 0.414/7.27 ´ 10- 5 = 5695 s = 1.58 h
2-63
T0 = 45 T¥ = 100 T(6s) = 70
(70 - 45)/(100 - 45) = exp( 6/ )-
= 7.61s
For 90% rise time exp(- /7.61) = 0.1
Rise time = 17.52 s
2-64
Insert function in Equations (2-38) and (2-39), manipulate algebra to give the indicated result.
2-65
= 8 s, T0 = 40, T¥ = 100
Rise time = 2.303 = 18.424 s
T(99%) = 99 C
(99 - 100)/(40 - 100) = exp(- t/8) t =
32.75 s
2-66
= 5 Hz, = 0.6 s
= (2π)(5) = 31.4 rad/s
( ) = - tan- 1( ) = - 8.7°
1/[1 + ( ) ]2 1/2 = 0.053
2-67
A = 15, = 0.01 Hz = 0.0628 rad/s
( ) = - tan- 1 = -
tan- 1(0.0628)(8) = - 26.7°
Attenuation = 1/[1 + ( ) ]2 1/2 = 0.894
SM: Experimental Methods for Engineers Chapter 2
13