5 dimensional analysis
TRANSCRIPT
-
7/29/2019 5 Dimensional Analysis
1/12
Chapter 5Dimensional Analysis
Page 1 of 12
5_001 A gas having a molecular weight of 86 is flowing at a rate of 1.38 kg/min through a tube having an actual i.d.of 1.20 in. At a cross section where the absolute pressure is 330 atm and the temperature is 340 F, the true
density is 1.2 times that predicted by the perfect-gas law, and the viscosity is 2.0 x 10-6
force-pound xseconds per square foot. Calculate the numerical value of the dimensionless Reynolds number.
Solution:
Reynolds number:
NRe
= DG/
F
= 2.0 x 10-6 Force-pound x seconds per square foot
= Fg
c
= (2.0 x 10-6)(32.2)
= 6.44 x 10-5 lb matter / sec-ftD = 1.2 in = 0.1 ft
G = 4w/D2
w = 1.38 kg/min = 0.050715 lb/sec
G = 4(0.050715)/[(0.1)2] = 6.457234
NRe
= (0.1)(6.457234)/6.44 x 10-5
NRe
= 10,027 . . . Ans.
5_002 It is desired to investigate the drag force on geometrically similar solid objects placed in a free stream offlowing fluid. In the general case, the force Fexerted on the body is thought to depend on the characteristiclength of the object x, the approach velocity V, the acceleration due to gravity g, and the following properties
of the fluid: the density , the viscosity , the surface tension , and the velocity Va
at which sound waves
are propagated in the liquid.
a. What is the numbern
of algebraically independent dimensionless groups which may be used to
correlate the variables?
b. Determine a set of these n
dimensionless groups, using the force Fin only one group.
c. Calculate the numerical value of each of these groups except the one in which the force Fappers,for the condition in which x= 7 inches, g= 32.2 ft/(sec)(sec), V= 11 ft/sec, and the fluid is water at 68 F
(assume Va = 4900 ft/sec).
Solution:
Variables -
aV,,,g,V,x,F, Then:
( ) 0V,,,g,V,x,F, a = Dimension of Factors: MLF
Dimensions Factors
F x V g Va
M 1 1L 1 1 1 -3 1 -1 1
-1 -2 -1 -1
F 1 1
a. nf= no. of physical factors of importance
nf= 8
ni= nd = number of dimension
ni= 4
-
7/29/2019 5 Dimensional Analysis
2/12
Chapter 5Dimensional Analysis
Page 2 of 12
n
= no. of independent dimensionless group
n
= nf- n
i= 8 - 4 = 4
b. Incompatible factors
( ) ( ) ( )L
M&,T
1,L
M,Lx 3 ==
==
FF
x
x
x
L
M
xLM
xL
23
33
=
===
==
=
Remaining factors:
aV,g,V,
xV;
x
x
x
LV
F
x;
x
F
L
F
gx;
x
x
x
Lg
xV;
x
x
x
LV
a42a
3
2
32
232
2
22
2
12
====
===
==
==
====
c. Values:x = 7 inches = 0.583333 ftg = 32.2 ft/(sec)(sec)V = 11 ft/secV
a= 4900 ft/sec
at 68 F
= 62.282 lb/cu ft
= 6.75 x 10-4 lb/(sec)(ft)
= 72.7 Dynes/cm2
= 0.67534 N/ft2
( )( )( )
( ) ( ) ( )
( )( )( )263,737
106.75
62.28249000.583333
xV
36,730106.75
32.20.58333362.282
gx
592,063106.75
62.282110.583333
xV
4
a4
4
32
2
32
2
41
=
==
=
==
=
=
=
5_003 Below are some data from an early article on the performance of a packed regenerator. In heating runs, thepacked spheres were initially at an elevated uniform temperature, and air at room temperature entered atconstant mass rate. In cooling runs, the spheres were initially at room temperature, and air at approximately
-
7/29/2019 5 Dimensional Analysis
3/12
Chapter 5Dimensional Analysis
Page 3 of 12
200 F entered at constant mass rate. In the data given below the relation between the temperature ofentering air (t
1), the temperature of exit air (t
2), and initial uniform temperature (t
0) of the bed of spheres is
given by the dimensionless term y= (t2
- t0)/(t
1- t
0). The heat capacity of the vertical cylindrical column was
small compared with that of the spheres used for packing, and the column was well insulated.Correlate all the values ofygiven below, plotted as ordinates against some suitable abscissa:
Material Steel Steel Steel Steel Lead Glass
Bed depth, inches ..... 5.125 10.25 5.125 2.56 9.55 9.71
Bed diam, in .............. 4 8 4 2 8 8
Particle diam, in ......... 0.125 0.25 0.125 0.0625 0.233 0.237
Sp ht .......................... 0.111 0.111 0.111 0.111 0.0347 0.168
Sp gr ......................... 7.83 7.83 7.83 7.83 11.34 2.6
k, Btu/(hr)(ft)(deg F) .. 26 26 26 26 19.5 0.4
Air superficial mass
vel., lb/(sec)(sq ft) ... .. 0.15 0.15 0.3 0.3 0.3 0.3
y , , , , , ,
sec sec sec sec sec sec
0.1 300 600 140 . . . 113 127
0.2 360 680 160 . . . 133 149
0.3 380 740 190 . . . 147 166
0.4 410 810 205 100 162 182
0.5 450 890 220 . . . 176 199
0.6 480 970 240 . . . 191 215
0.7 510 1050 250 . . . 206 232
0.8 570 1140 300 140 222 250
0.9 650 1300 330 170 248 280
The quantity is the elapsed time at which the indicated ywas measured.
Solution:
L - ftD
t- ft
Dp
- ft
cp
- Btu/lb-ft
- lb/cu ftk - Btu/sec-fr-deg FG
o- lb/sec-sq ft
- time, sec
MLTFH System:
Hoppt Kq,,Gk,,,c,D,DL,y = p
Hnm
oife
pc
pb
ta KGkcDDLy =
( ) ( ) ( ) ( )p
2
2n
m
2
if
3
ecba
H
ML
L
M
LT
H
L
M
MT
HLLL1
=
-
7/29/2019 5 Dimensional Analysis
4/12
Chapter 5Dimensional Analysis
Page 4 of 12
(1) L: a + b + c - 3f - i - 2m + 2p = 0
(2) L: e + i - p = 0
(3) M: -e + f + m + p = 0
(4) T: -e - i = 0
(5) : -i - m + n - 2p = 0
(4) i = -e(5) e + i - p = 0
e - e - p = 0p = 0
(3) -e + f + m + p = 0-e + m + n = 0e = m - n
Equating:e = f + m = m - n
(1) a + b + c - 3f - i - 2m + 2p = 0a + b + c - 3f + e -2m = 0a + b + c - 3f + e - 2(e - f) = 0a + b + c - 3f + e - 2e + 2f = 0a + b + c -f -e = 0
a + b + c = f + ef = a + b + c -e
Then:
p = 0a = ab = bc = ce = ef = a + b + c -ei = -em = e -f = 2e - a - b -c
n = -f = e - a - b -c
Then:cbaecba2e
oeecbae
pc
pb
ta GkcDDLy
++=
e2
op
c
o
pb
o
t
a
o rk
Gc
G
D
G
D
G
Ly
=
Note: Strouhal Numbers:
G
LN
oLSl, =
GDN
o
tDSl, t
=
G
DN
o
pDSl, p
=
Ratio of Peclet Number to Strouhal Number:
-
7/29/2019 5 Dimensional Analysis
5/12
Chapter 5Dimensional Analysis
Page 5 of 12
k
Gc
N
N2
op
Sl
Pe =
Steel # 1:
L = 5.125 in = 0.4271 ftD
t= 4 in = 0.3333 ft
Dp
= 0.125 in = 0.01042 ft
cp
= 0.111 Btu/lb-F
= 7.83 x 62.4 = 488.6 lb/cu ft
k = 26 Btu/hr-ft-deg F = 7.2222 x 10-3
Btu/sec-ft-deg FG
o= 0.15 lb/sec-sq ft
( )( )
1391.2
0.15
488.60.4271
G
LN
oLSl, ===
( )( )
1085.7
0.15
488.60.3333
G
DN
o
tDSl, t
===
( )( )
33.9414
0.15
488.60.01042
G
DN
o
pDSl, p
===
( )( )
( )( )107.07754
107.2222488.6
0.150.111
k
Gc
N
N 43
22op
Sl
Pe
=
==
Table No. 1
X1N LSl, = X2N
tDSl,=
X3N
pDSl,=
X4NN
Sl
Pe =
y X1 X2 X3 X4
0.1 300 4.637333 3.619000 0.113138 0.212326
0.2 360 3.864444 3.015833 0.094282 0.254791
0.3 380 3.661053 2.857105 0.089319 0.268947
0.4 410 3.393171 2.648049 0.082784 0.290179
0.5 450 3.091556 2.412667 0.075425 0.318489
0.6 480 2.898333 2.261875 0.070711 0.339722
0.7 510 2.727843 2.128824 0.066552 0.360955
0.8 570 2.440702 1.904737 0.059546 0.403420
0.9 650 2.140308 1.670308 0.052218 0.460040
Steel # 2:
L = 10.25 in = 0.8542 ftD
t= 8 in = 0.6667 ft
Dp
= 0.25 in = 0.02083 ft
cp
= 0.111 Btu/lb-F
= 7.83 x 62.4 = 488.6 lb/cu ft
k = 26 Btu/hr-ft-deg F = 7.2222 x 10-3
Btu/sec-ft-deg F
-
7/29/2019 5 Dimensional Analysis
6/12
Chapter 5Dimensional Analysis
Page 6 of 12
Go
= 0.15 lb/sec-sq ft
( )( )
2782.4
0.15
488.60.8542
G
LN
oLSl, ===
( )( )
2171.7
0.15
488.60.6667
G
DN
o
tDSl, t
===
( )( )
67.8503
0.15
488.60.02083
G
DN
o
pDSl, p
===
( )( )
( )( )107.07754
107.2222488.6
0.150.111
k
Gc
N
N 43
22op
Sl
Pe
=
==
Table No. 1
X1N LSl, = X2N
tDSl,=
X3N
pDSl,=
X4NN
Sl
Pe =
y X1 X2 X3 X4
0.1 600 4.637333 3.619500 0.113084 0.424652
0.2 680 4.091765 3.193676 0.099780 0.481273
0.3 740 3.760000 2.934730 0.091690 0.523738
0.4 810 3.435062 2.681111 0.083766 0.573281
0.5 890 3.126292 2.440112 0.076236 0.629901
0.6 970 2.868454 2.238866 0.069949 0.686521
0.7 1050 2.649905 2.068286 0.064619 0.743142
0.8 1140 2.440702 1.905000 0.059518 0.806840
0.9 1300 2.140308 1.670538 0.052193 0.920080
Steel # 3:
L = 5.125 in = 0.4271 ftD
t= 4 in = 0.3333 ft
Dp
= 0.125 in = 0.01042 ft
cp
= 0.111 Btu/lb-F
= 7.83 x 62.4 = 488.6 lb/cu ft
k = 26 Btu/hr-ft-deg F = 7.2222 x 10-3
Btu/sec-ft-deg FG
o= 0.30 lb/sec-sq ft
( )( )
695.6
0.30
488.60.4217
G
LN
o
LSl, ===
( )( )
542.8
0.30
488.60.3333
G
DN
o
tDSl, t
===
( )( )
16.97
0.30
488.60.01042
G
DN
o
pDSl, p
===
( )( )
( )( )102.83102
107.2222488.6
0.300.111
k
Gc
N
N3
22op
Sl
Pe 3
=
==
-
7/29/2019 5 Dimensional Analysis
7/12
Chapter 5Dimensional Analysis
Page 7 of 12
Table No. 1
X1N LSl, = X2N
tDSl,=
X3N
pDSl,=
X4NN
Sl
Pe =
y X1 X2 X3 X4
0.1 140 4.968571 3.877143 0.121214 0.396343
0.2 160 4.347500 3.392500 0.106063 0.452963
0.3 190 3.661053 2.856842 0.089316 0.537894
0.4 205 3.393171 2.647805 0.082780 0.580359
0.5 220 3.161818 2.467273 0.077136 0.622824
0.6 240 2.898333 2.261667 0.070708 0.679445
0.7 250 2.782400 2.171200 0.067880 0.707755
0.8 300 2.318667 1.809333 0.056567 0.849306
0.9 330 2.107879 1.644848 0.051424 0.934237
Steel # 4:
L = 2.56 in = 0.2134 ftD
t= 2 in = 0.1667 ft
Dp
= 0.0625 in = 0.00521 ft
cp
= 0.111 Btu/lb-F
= 7.83 x 62.4 = 488.6 lb/cu ft
k = 26 Btu/hr-ft-deg F = 7.2222 x 10-3
Btu/sec-ft-deg FG
o= 0.30 lb/sec-sq ft
( )( )
347.6
0.30
488.60.2134
G
LN
o
LSl, ===
( )( )
271.5
0.30
488.60.1667
G
DN
o
tDSl, t
===
( )( )
8.485
0.30
488.60.00521
G
DN
o
pDSl, p
===
( )( )
( )( )102.83102
107.2222488.6
0.300.111
k
Gc
N
N3
22op
Sl
Pe 3
=
==
Table No. 1
X1N LSl, = X2N
tDSl,=
X3N
pDSl,=
X4N
N
Sl
Pe =
y X1 X2 X3 X4
0.4 100 3.476000 2.715000 0.084850 0.283102
0.8 140 2.482857 1.939286 0.060607 0.396343
0.9 170 2.044706 1.597059 0.049912 0.481273
-
7/29/2019 5 Dimensional Analysis
8/12
Chapter 5Dimensional Analysis
Page 8 of 12
Lead:
L = 9.55 in = 0.7958 ftD
t= 8 in = 0.6667 ft
Dp
= 0.233 in = 0.01942 ft
cp = 0.0347 Btu/lb-F = 11.34 x 62.4 = 707.6 lb/cu ft
k = 19.5 Btu/hr-ft-deg F = 5.4167 x 10-3
Btu/sec-ft-deg FG
o= 0.30 lb/sec-sq ft
( )( )
1877
0.30
707.60.7958
G
LN
oLSl, ===
( )( )
1572.5
0.30
707.60.6667
G
DN
o
tDSl, t
===
( )( )
45.81
0.30
707.60.01942
G
DN
o
pDSl, p
===
( )( )
( )( )108.14797
105.4167707.6
0.300.0347
k
Gc
N
N3
22op
Sl
Pe 4
=
==
Table No. 1
X1N LSl, = X2N
tDSl,=
X3N
pDSl,=
X4N
N
Sl
Pe =
y X1 X2 X3 X4
0.1 113 16.610619 13.915929 0.405398 0.0920720.2 133 14.112782 11.823308 0.344436 0.108368
0.3 147 12.768707 10.697279 0.311633 0.119775
0.4 162 11.586420 9.706790 0.282778 0.131997
0.5 176 10.664773 8.934659 0.260284 0.143404
0.6 191 9.827225 8.232984 0.239843 0.155626
0.7 206 9.111650 7.633495 0.222379 0.167848
0.8 222 8.454955 7.083333 0.206351 0.180885
0.9 248 7.568548 6.340726 0.184718 0.202070 Glass:
L = 9.71 in = 0.8092 ftD
t= 8 in = 0.6667 ft
Dp
= 0.237 in = 0.01975 ft
cp
= 0.168 Btu/lb-F
= 2.60 x 62.4 = 162.24 lb/cu ft
k = 0.4 Btu/hr-ft-deg F = 1.1111 x 10-4
Btu/sec-ft-deg FG
o= 0.30 lb/sec-sq ft
( )( )
437.6
0.30
162.240.8092
G
LN
oLSl, ===
-
7/29/2019 5 Dimensional Analysis
9/12
Chapter 5Dimensional Analysis
Page 9 of 12
( )( )
360.6
0.30
162.240.6667
G
DN
o
tDSl, t
===
( )( )
10.68
0.30
162.240.01975
G
DN
o
pDSl, p
===
( )( )
( )( ) 0.838766101.1111162.240.300.168
k
Gc
N
N4
22op
Sl
Pe
===
Table No. 1
X1N LSl, = X2N
tDSl,=
X3N
pDSl,=
X4N
N
Sl
Pe =
y X1 X2 X3 X4
0.1 127 3.445669 2.839370 0.084094 106.523282
0.2 149 2.936913 2.420134 0.071678 124.976134
0.3 166 2.636145 2.172289 0.064337 139.235156
0.4 182 2.404396 1.981319 0.058681 152.655412
0.5 199 2.198995 1.812060 0.053668 166.914434
0.6 215 2.035349 1.677209 0.049674 180.334690
0.7 232 1.886207 1.554310 0.046034 194.593712
0.8 250 1.750400 1.442400 0.042720 209.691500
0.9 280 1.562857 1.287857 0.038143 234.854480
By curve fitting:
e2
op
c
o
pb
o
t
a
o rk
Gc
G
D
G
D
G
Ly
=
= 0.003593a = -29.130232b = 30.947910c = -3.944493e = -0.394509
Therefore:-0.394509
2op
-3.944493
o
p30.947910
o
t
-29.130232
o rk
Gc
G
D
G
D
G
L0.003593y
=
5_004 Two metals, A and B, are being considered for use in constructing tuning forks which are to produce
vibrations of a given frequency. What would be the ratio of the costs of the metal required for the two tuningforks, expressed as a function of the frequency, the physical properties of the metals, and the cost per unitmass of each metal (assumed independent of the quantity purchased)? The tuning forks are to begeometrically similar.
Solution:
-
7/29/2019 5 Dimensional Analysis
10/12
Chapter 5Dimensional Analysis
Page 10 of 12
Let R = ratio of the cost of the metals.f = frequency, HzU
1, U
2= cost per unit mass.
Other properties:
1,
2= densities of material
V1, V
2= sound velocities
( )212121 U,U,V,V,,f,R = h
2g
1e
2d
1c
2b
1a UUVVfR =
hgedc
3
b
3
a
M
1
M
1
L
L
L
M
L
M
11
=
(1) : -a - d - e = 0
(2) M: b + c - g - h = 0
(3) L: -3b - 3c + d + e = 0
(1) d + e = -a(2) -3b - 3c - a =
b + c = -a / 3(3) b + c - g - h = 0
g + h = -a / 3
Then:
ga2
g1
da2
d1
ba2
b1
a 31
31
UUVVfR
=
g
2
1
d
2
1
b
2
1
a
222U
U
V
V
UVr
fR
31
31
=
g
2
1
d
2
1
b
2
13a
23
22
3
U
U
V
V
UVr
fR
=
Therefore:
=
2
1
2
1
2
1
23
22
3
U
U
V
V
UVr
fR ,,,
-
7/29/2019 5 Dimensional Analysis
11/12
Chapter 5Dimensional Analysis
Page 11 of 12
5_005 It is agreed to assume that the thermal conductivities of gases and vapors depend on the following factors:
cp, specific heat at constant pressure; c
v, specific heat at constant volume; , viscosity; T, absolute
temperature; = /(p)T, coefficient of compressibility; b = /(T)
p, coefficient of thermal expansion.
List all conclusions which may be drawn from dimensional consideration. If one additional physical variablewere to be included, what should it be?
Solution:
unitsc
p- Btu/lb-R
cv
- Btu/lb-R
- sq ft / lb
- 1/R
additional variable is the viscositym - Btu/sec-ft-R
MLTF system
Hvp K,,,,c,ck = f
Hedcb
va
p1 Kcck = f
2edc
2ba
H
ML
L
M
T
1
M
L
MT
H
MT
H
LT
H
=
(1) H: a + b - f = 1
(2) : -e - f = -1e + f = 1
(3) L: 2c - e + 2f = -1
(4) T: -a - b - d = -1
a + b + d = 1(5) M: -a - b - c + e + f = 0
(1) and (4)-f = df = -d
(5) -a - b - c + e + f = 0a + b + c - e - f = 0a + b + c -1 = 0a + b + c = 1
(2) e = 1 - fe = 1 + de = 1 + c
but c = 1 - a - b
Then:a = ab = bc = 1 - a - bd = 1 - a - be = 1 + c = 2 - a - bf = a + b -1
-
7/29/2019 5 Dimensional Analysis
12/12
Chapter 5Dimensional Analysis
Page 12 of 12
-1baH
b-a-2b-a-1b-a-1bv
ap1 Kcck
+=
=
H
b
Hv
a
Hp1
K
Kc
Kck
KH
= Jgc
= (778)(32.2) = 25,000 (lb matter)(ft)2 / (Btu)(sec)2
Final results.
=
Kc
Kc
K
k Hv
Hp
H
,
- end -