natec 2016 - 大阪大学kato/fils/hara.pdf · suction pipe high frequency inverter sunken wreck...
TRANSCRIPT
11
Recovery of Heavy Fuel Oil from Sunken Ships
by High Frequency Induction Heating Method
Shoichi Hara, Osamu Miyata, Masao OnoNational Maritime Research InstituteHiroyasu KifuneTokyo University of Science and TechnologySukekazu ShimonishiNippon Salvage Co., Ltd
NATEC 2016
22
Contents of presentation
(1) Introduction
(2) Outline of experiment
(3) Experimental results
(4) Discussions
(5) Numerical calculation
(6) Conclusion
33
Necessity of recovering oil remained in the ship tank
●When the ship sinks loaded with the cargo oil or fuel oil due to marine disaster, the oil recovery is required because of the risk reduction of oil discharge and marine environment protection,
●The operation of the oil recovery from sunken vessels is extremely difficult in winter or in deep water, because the fluidity of oil in the tank is quite low.
44
Principle of technique (High Frequency Induction Heating Method)
alternate current →magnetic flux change→eddy current→Joule heat generation
coil metal
power
power
coil
IH electromagnetic cooker Induction heating principle
55
Heavy fuel oil recovery system
Heating system ①Direct heating unit: heating unit inside the hull
②Side hull heating unit: heating of heavy fuel oil
outside the hull by heat transfer
Assuming the case of impossibility of direct heating inside the hull, the target is to develop the system for providing the heat from outside of the hull. Schematic idea
IH unit
IH unit
suction pipe
high frequency inverter
sunken wreck
IH unit
IH unit
suction pipe
high frequency inverter
sunken wreck
①
②
6
Characteristics of heavy fuel oil recovery system
Advantage
●The induction heating recovery system needs no large-scale facilities such as boilers.
●The power can sufficiently be supplied from auxiliary generator on the salvaging vessel.
7
ρl(kg/m3)
y = -0.0008x + 0.9920.95
0.955
0.96
0.965
0.97
0.975
0.98
0 10 20 30 40 50 60
T(℃)
log(ν)
log(ν) = -0.0327T + 3.9211
0
1
2
3
4
5
0 10 20 30 40 50 60
T(℃)
Outline of experiment
Experimental parameter
●H
●L
●φd
●with/without heat
Physical property of
heavy fuel oil
Logarithmic kinematic viscosity
density
L
h
water
heavy oil
work coil
gravity tank
reservoir tank
Φd
heavy oil tank
circulating water channel
water
water
HL
h
water
heavy oil
work coil
gravity tank
reservoir tank
Φd
heavy oil tank
circulating water channel
water
water
H
(cSt)
schematic idea of the experimental arrangement
tank size:06x0.6x0.6m
88
Outline of experiment
schematic idea of the experimental arrangement
Gravity tank
Reservoir tank
Water
Heavy fuel oil
Work coil
Heavy oil tank
WaterLoad cell
W
Gravity tank
Reservoir tank
Water
Heavy fuel oil
Work coil
Heavy oil tank
WaterLoad cell
W
99
Measurement by thermo couples
unit:mm
central section
600mm
300 mm
heated area
Oil outletx
yz
Water inlet :thermo sensor
12345
6
7
89
1011
12
13141516
17
600mm
300 mm
heated area
Oil outletx
yz
Water inlet :thermo sensor
12345
6
7
89
1011
12
13141516
17
No x y z1 5 5 3002 5 10 3003 5 50 3004 5 100 3005 5 300 3006 5 500 3007 5 595 3008 300 5 3009 300 10 300
10 300 50 30011 300 100 30012 300 300 30013 450 5 30014 450 10 30015 450 50 30016 450 100 30017 450 300 30018 595 5 30019 595 10 30020 595 50 30021 595 100 30022 595 300 30023 595 500 30024 595 595 30025 450 5 526 450 10 527 450 50 528 450 100 529 450 300 5
30-3741-48
horizontal pipeheated pipe
1010
Experimental conditions
Exp.No.P ipe length
L(m )
PipediameterdΦ (mm)
Waterpressure
head h(m)
Heat time(min)
Mat size(m)
Watertemperature
(℃ )
Atmospheretemperature
(℃ )
O iltemperature
(℃ )
Electric powerbefore oil
recovery (W)
Heating position during oilrecovery
Electric powerduring oil
recovery (W)
Recoveryrate
(kg/s)
1 4 25 4 - - 28.2 - - - - - 0.0577
2 4 25 4 - - 24.8 - - - - - 0.0539
3 2 25 4 - - 28.0 - - - - - 0.1050
4 2 32 4 - - 28.0 - - - - - 0.2310
5 4 32 4 - - 27.9 - - - - - 0.1710
6 4 32 2 - - 27.7 - - - - - 0.1090
7 2 32 2 - - 27.7 - - - - - 0.1570
8 2 25 2 - - 27.7 - - - - - 0.0699
9 4 25 4 - - 27.4 - - - - - 0.0372
10 4 25 4 120 0.2 25.1 - - 400 Top (Center) 400 0.0767
11 4 25 4 120 0.6 24.5 - - 600 Top (Center) 600 0.0818
12 2 25 4 120 0.6 23.5 - - 600 Top (Center) 600 0.1280
13 4 32 4 240 0.6 23.1 - - 600 Top (Center) 600 0.1740
14 4 25 4 0 - 29.3 30.7 28.6 - - - 0.0771
15 4 25 4 10 0.2 28.8 28.9 28.6 400 Top (Center) 400 0.0813
16 4 25 4 30 0.2 29.1 27.8 28.7 400 Top (Center) 400 0.0803
17 4 25 4 60 0.2 28.1 27.8 28.2 400 Top (Center) 400 0.0808
18 4 25 4 120 0.2 27.3 26.9 27.1 400 Top (Center) 400 0.0705
19 4 25 4 120 0.2 27.1 26.4 26.7 400 Top (Recovery side) 400 0.0693
20 4 25 4 120 0.2 25.0 25.6 26.4 400 Side plate 400 0.0696
21 4 25 4 10 0.2 25.8 26.0 26.1 2000 Top (Center) 2000 0.0671
22 4 25 4 - - 12.3 11.1 12.3 - - - 0.0118
23 4 32 4 - - 11.7 11.0 11.7 - - - 0.0224
24 4 32 2 - - 11.6 11.0 11.6 - - - 0.0119
25 4 25 2 - - 11.6 11.7 11.6 - - - 0.0052
26 4 25 4 - 0.2 11.3 10.3 13.5 - Pipe(Recovery side) 400 0.0144
27 4 25 4 - 0.2 11.1 10.3 13.2 - Pipe(Recovery side) 1000 0.0181
28 4 25 4 - 0.2 11.2 10.1 12.7 - Pipe(Recovery side) 2000 0.0230
29 4 25 4 120 0.2 11.4 9.6 11.5 2000 Top (Center) 2000 0.0085
30 4 25 4 120 0.2 10.9 9.8 12.2 2000 Top+ Pipe 4000 0.0305
1111
Experimental materials and instrument
oil tank
work coil non-woven fabric
set-up of thermo couple Inverter unit
1212
Work coil of pipe type
41ch
43ch
42ch
45ch
44ch
47ch
46ch
48ch
41ch
43ch
42ch
45ch
44ch
47ch
46ch
48ch
thermocouple
heated pipe
work
coil
un-woven fabric
41ch
43ch
42ch
45ch
44ch
47ch
46ch
48ch
41ch
43ch
42ch
45ch
44ch
47ch
46ch
48ch
thermocouple
heated pipe
work
coil
un-woven fabric
1313
Gravity tank and reservoir tank
oil tank
gravity tank gravity tank
oil tank and pipe reservoir tank
load cell
1414
Estimation of oil recovery rate with various experimental conditions
0
0.05
0.1
0.15
0.2
0.25
0 0.0005 0.001 0.0015
Hd4/Lν
Q(k
g/se
c)
no heating
pipe heating
mat heating
Cal
LHgdQ
o
w
128
4
1515
Estimation of oil recovery rate concerning oil temperature on certain experimental condition
0
0.02
0.04
0.06
0.08
0.1
0.12
0 10 20 30 40
temperature(℃)
Q(k
g/se
c)
no heatingpipe heatingmat heatingCal
1616
L2z1
油
gravity tank
reservoir tank
heavy oil tank
ℓ3
P1 V1
P2 V2
Hζ1
ζ2
λ1
ζ4
ζ3
λ2z2
ℓ1
ℓ2
L2z1
油
gravity tank
reservoir tank
heavy oil tank
ℓ3
P1 V1
P2 V2
Hζ1
ζ2
λ1
ζ4
ζ3
λ2z2
ℓ1
ℓ2
Friction loss factor
2L
22
22221
21
22o
2
22
22
4
22
3
23
1
11
23
2
23
12
2222
111
Vd
VV
VdLVVVgzPVgzP
oo
wwwooww
Bernoulli's principle
friction loss coefficient of elbow.
321 ,,
4
friction loss coefficient of entrance
INLETOUTLET
20
1717
Relation between Reynolds number
and friction loss factor
1
10
100
1000
10000
0.01 0.1 1 10
Re
λ
no heatingpipe heatingmat heatingCal 2
2VdL
gHo
w
VdRe
6464
laminar flow
Exp.
1818
Relation between loaded electric
power and improved ratio by heating
1.0
1.2
1.4
1.6
1.8
2.0
2.2
2.4
2.6
2.8
0 1000 2000 3000 4000 5000
power(W)
impr
ove
d r
atio
mat heatingpipe heating
pipe+mat
10 min.pre-heating
mat size0.6m
10min. ~ 2 hourspre-heating
19
Numerical simulation
CFD tool : FLUENT
mesh for half model
density 977.2 (kg/m3) specific heat 2093.025 (kcal/kg℃)
thermal conduction rate 0.1453 (kcal/mh℃)
viscous coefficient 1.9544 (kg/ms) cubical expansion coefficient 0.00099 (/K) density 7850 (kg/m3) specific heat 498.13 (kcal/kg℃) thermal conduction rate 52.3256 (kcal/mh℃)
oil
iron
physical properties of oil and iron
19
20x=5 300 450 595
595
500
300
100
50
10
y=5
T=7200sec(Exp_9)
39.5-40.5
38.5-39.5
37.5-38.5
36.5-37.5
35.5-36.5
34.5-35.5
33.5-34.5
32.5-33.5
31.5-32.5
30.5-31.5
29.5-30.5
28.5-29.5
27.5-28.5
26.5-27.5
25.5-26.5
24.5-25.5
23.5-24.5
22.5-23.5
Particle trajectory and temperature distribution
heating
mmExperimental resultsNumerical results
Exp.9
525sec
1000sec
1680sec
20
21
x=5 300 450 595y=595
500
300
100
50
10
5
T=0(Exp_9)
25-25.5
24.5-25
24-24.5
23.5-24
23-23.5
22.5-23
22-22.5
x=5 300 450 595y=595
500
300
100
50
10
5
T=60secc(Exp_9)
24.5-25
24-24.5
23.5-24
23-23.5
22.5-23
x=5 300 450 595y=595
500
300
100
50
10
5
T=300sec(Exp_9)
28.5-29.5
27.5-28.5
26.5-27.5
25.5-26.5
24.5-25.5
23.5-24.5
22.5-23.5
x=5 300 450 595y=595
500
300
100
50
10
5
T=600sec(Exp_9)
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595y=595
500
300
100
50
10
5
T=1200sec(Exp_9)
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595y=595
500
300
100
50
10
5
T=1800sec(Exp_9)
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595y=595
500
300
100
50
10
5
T=0(Exp_9)
25-25.5
24.5-25
24-24.5
23.5-24
23-23.5
22.5-23
22-22.5
x=5 300 450 595y=595
500
300
100
50
10
5
T=60secc(Exp_9)
24.5-25
24-24.5
23.5-24
23-23.5
22.5-23
x=5 300 450 595y=595
500
300
100
50
10
5
T=300sec(Exp_9)
28.5-29.5
27.5-28.5
26.5-27.5
25.5-26.5
24.5-25.5
23.5-24.5
22.5-23.5
x=5 300 450 595y=595
500
300
100
50
10
5
T=600sec(Exp_9)
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595y=595
500
300
100
50
10
5
T=1200sec(Exp_9)
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595y=595
500
300
100
50
10
5
T=1800sec(Exp_9)
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
Change of temperature distribution
600sec 1200sec 1800sec
300sec0sec 60sec
50mm10mm
Exp.9
21
22
Change of temperature distribution
x=5 300 450 595595
500
300
100
50
10
y=5
T=2400sec(Exp_10)
47.5-50
45-47.5
42.5-45
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595595
500
300
100
50
10
y=5
T=3000sec(Exp_10)
47.5-50
45-47.5
42.5-45
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595595
500
300
100
50
10
y=5
T=4200sec(Exp_10)
47.5-50
45-47.5
42.5-45
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595595
500
300
100
50
10
y=5
T=4800sec(Exp_10)
47.5-50
45-47.5
42.5-45
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 300 450 595595
500
300
100
50
10
y=5
T=5400sec(Exp_10)
47.5-50
45-47.5
42.5-45
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
x=5 150 300 450 595595
500
300
100
50
10
y=5
T=6000sec(Exp10)
47.5-50
45-47.5
42.5-45
40-42.5
37.5-40
35-37.5
32.5-35
30-32.5
27.5-30
25-27.5
22.5-25
50mm10mm
2400sec 3000sec 4200sec
4800sec 5400sec 6000sec
Exp.9
22
2323
small coil(100×100mm) large coil(150×150mm)
Coil arrangement on top plate
Reservoir tank
Water
Heavy oil
Work coilh
L
H d
Heavy oil tank
WaterLoad measure
WGravity tank
Arrangement of work coil In another experiment
Oil recovery system
2424
Measuring positions of thermo couples
仕切り板
蓋
油出口
タンク壁面の穴位置
5
150
5
150
510
50
100
5300
117 177
75
正面図 平面図
①
②
③④
⑤
⑥ ⑦
⑧
⑨
⑩
⑪
⑧ ⑪
⑮
⑯
⑰
⑱⑲
⑳
㉑㉒
㉓
㉘
⑰ ㉓
㉗
㉙
㉚
㉛ ㉜
㉔㉕
㉖
⑫⑬
⑭
仕切り板
蓋
油出口
タンク壁面の穴位置
5
150
5
150
510
50
100
5300
117 177
75
正面図 平面図
①
②
③④
⑤
⑥ ⑦
⑧
⑨
⑩
⑪
⑧ ⑪
⑮
⑯
⑰
⑱⑲
⑳
㉑㉒
㉓
㉘
⑰ ㉓
㉗
㉙
㉚
㉛ ㉜
㉔㉕
㉖
⑫⑬
⑭
Position of the hole of the tank
Top view
Partition plate
Tank lid
Oil outlet
Front view
2525
Exp.No.
Pipelength
L(m)
Pipediameterdd
(mm)
Water pressurehead h(m)
Heat timebefore Exp.
(min)
Mat size &number of
use(m) ×
Watertemperature
(℃)
Atmospheretemperature
(℃)
Oiltemperature
(℃)Heating position
Injectionelectricity
(W)
Recoveryrate
(kg/min)
1 4 25 4 - - 13.3 12.4 15.3 - - 0.72
2 4 25 4 - 0.2×2 12.9 12.1 13.9 Central edge 2000 0.90
3 4 25 4 120 0.2×1 11.0 10.2 11.6 Center rear 2000 0.58
4 4 25 4 - 0.14×2 9.9 9.6 11.7 Central edge 2000 0.37
5 4 25 4 - 0.2×2 9.9 10.5 9.2 One side edge 2000 0.52
6 4 25 4 - 0.14×2 9.8 9.0 11.5 Central edge 2000 0.49
Experimental conditions and results
2626
Time history of oil recovery weight in each case of experiments
2727
y = 8E+06x-2.05
y = 3839.8x-1
0.0
0.5
1.0
1.5
2.0
2.5
1500 2000 2500 3000 3500 4000 4500 5000
Q(k
g/m
in.)
ν(cSt)
Exp_1
Exp_2
Exp_3
Exp_4
Exp_5
Exp_6
mean line
Cal.
without heating
Relation between oil recovery rate and kinematic viscosity of oil
2828
Modeling for computer simulation
2929
Streamline of oil and water inside the model tank (Section distance:X=0.3m,t=50sec)
Streamline of oil and water inside the model tank (Section distance:X=0.15m,t=100sec)
Streamline of oil and water inside the model tank (Section distance:X=0.3m,t=100sec)
Streamline of oil and water inside the tank
3030
Streamline of oil and water inside the model tank (Section distance:X=0.3m,t=50sec)
Streamline of oil and water inside the model tank(Section distance:X=0.15m,t=100sec)
Streamline of oil and water inside the model tank (Section distance:X=0.3m,t=100sec)
1680 sec
1000 sec
Without partitionWith partition
Comparison of streamline of oil and water inside the tank
Experimental conditions and oil recovery rate
Pipe length : 4 mPipe diameter : 25 mmWater pressure head : 4 mWater temperature : 25.1 ℃Electric power before oil recovery : 400 w/2 hour
3131
(1) The oil recovery rate has been estimated by the simple method using various parameters.
(2) The improved oil recovery rate comparing with the case of no heating as for the pipe type of heating increases linearly with the increase of electric power.
(3) The combination of pipe and mat type of heating can improve the oil recovery rate.
Conclusion
3232
(4) The numerical calculation results of oil temperature inside the tank does not agree well with the experimental results and represent the natural convection of heat
(5) The heating at the cutout part of the partition plate does not improve the effect of fluidization.
(6) The size of the coil mat does not show the significant difference of the oil recovery efficiency.
(7) The partition plate prevents the oil from fluidizing because of making the route of water. This phenomenon is seen in the practical operation of salvage.
Conclusion
3333
Thank you for your kind attention.