investigation of thermal equilibrium around an accidental
TRANSCRIPT
0
5
10
15
20
0 5 10 15 20
Heli
um
In
ven
tory [
kg
]
Time [min]
Process Pipe (Liquid ) [kg]
Process Pipe (Vapour ) [kg]
Annular Space (Vapour) [kg]
Investigation of Thermal Equilibrium Around an Accidental Event And Impact on
Possibly Enclosed Surrounding Environment
Problem Definition
Sarkar Biswanath, Shah Nitin, Choukekar Ketan, Kapoor Himanshu, Kumar Uday, Das Jotirmoy, Bhattacharya Ritendra, Vaghela Hitensinh, Muralidhara Srinivasa
ITER-India, Institute for Plasma Research, Gandhinagar and 382016, India
Accidental scenario of
cryogenic transfer line
(major seismic activity or
any unprecedented
mechanical events)
Process failure
(loss of insulation vacuum)
Physical failure
(Rupture of Process pipe and OVJ)
Change in temperature
& pressure of surrounding
enclosed volume
Assumptions and Modelling
Process Pipe
Process Pipe
Cold He
(5 bar, 5 K)
Annular space
Mixture
of Dry air
+ Cold
Helium
Qconv1
Qrad1 Cold He
Enclosed Volume
Qconv2
Qrad2
Outer Vacuum
Jacket
Results from ASPEN HYSYS® modelling
Further attention to safety
Preliminary test proposal
Development of detailed model in ASPEN HYSYS®
Process
pipe Crack as a pipe
Annular
Space
Enclosed
Volume Relief valve
Qconv2 Qrad2 Qconv1 Qrad1
1.0
2.0
3.0
4.0
5.0
0 5 10 15 20
Press
ure [
ba
r(a
)]
Time [min]
Process Pipe [bar(a)]
Annular Space [bar(a)]
Enclosed Volume [bar(a)]
• Cold helium / liquid nitrogen cryogenic
transfer line is enclosed inside duct
made of concrete sheet with normal leak
tight sealing.
• Control valves for simulating leak
through process pipe and OVJ.
• Mass flow meters for measuring the
amount of helium entering into OVJ and
further to Enclosed Volume (EV).
• The facility of ventilation for relieving
the pressure inside EV will be provided.
• Quantifying an accidental event requires near reality assumptions. It is to be
understood that the accidental events are the driving factor for ascertaining
the safety of the designed system.
• The minimum design temperature of surrounding components and systems
should be decided based on minimum temperature possible in such
enclosed environment with a more realistic approach.
• The impact on process pipe and OVJ due to stored energy of gaseous
helium in OVJ annular space and mixture (air + helium) in EV respectively
should be considered, as it will act similar to a pneumatic testing of a vessel
with a leak.
References 1. Chorowski M. et. Al, Risk analysis update of the LHC cryogenic system following the 19th September 2008 incident, Proceedings of ICEC-23/
ICMC 2010, pp 879-884
2. Barron R. F. , Cryogenic Heat transfer, 1999, , ISBN-1-56032-551-8
3. Holman J. P., Heat Transfer
Validation of Average Temperatures using ANSYS Fluent ®
t = 0 seconds t = 5 seconds t = 10 seconds t = 15 seconds t = 20 seconds t = 29 seconds t = 1 seconds t = 2 seconds t = 25 seconds
A: 300 K
H: 300 K
A: 291 K
H: 289 K A: 279 K
H: 278 K
A: 259 K
H: 257 K
A: 242 K
H: 233 K
A: 236 K
H: 223 K
A: 233 K
H: 220 K
A: 229 K
H: 216 K
A: 226 K
H: 214 K
A: Global average temperature from ANSYS Fluent ®
H: Global average temperature from ASPEN HYSYS®
Pressure after 18.5
min 3.86 bar [a]
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
0 10 20 30 40 50 60
Ma
ss f
low
[k
g/s
]
Time [s]
Process Pipe outflow [kg/s]
Annular space outflow [kg/s]
High initial mass flows due
to large differential pressure
~ 202 K
Temperature equalization
at ~ 282 K at 18.5 min
.
..
....
mixp
Theliumpairp
mixcm
QTcmTcmT
heliumair
airair
mm
mx
.. radconvT QQQ
Validation using
analytical modeling
• Smooth crack having equivalent circular cross
section of 10 mm diameter across the thickness of
process pipe
• Discharge area of rupture disc on OVJ is ~ 507
sq.mm
• Enclosed Volume (EV) is occupied with stagnant
dry air at 300 K and 1 bar(a).
• EV is fairly tight for helium, air or mixture of
helium with air (worst case scenario) for exhaust
• Heat transfer through conduction mode has been
neglected
• The concrete wall of EV has been considered at
300K
• Uniform thermal mixing has been assumed
• Stratification of the flows is not considered, as
vertical column of stagnant dry air is considered
in EV [2]
Process parameters at t = 18.5 min (t = 0:
considered to be the rupture of process pipe)
Process
Parameters
Process
Pipe
Annular
space EV
Pressure
bar (a) 3.86 3.86 3.86
Temperature
(K) 282 282.2 283.1
Composition Helium Helium Air (x=0.71) +
Helium (x=0.29)
Pressure Profile for first 60 s
• High helium inventory is normally expected in Cryogenic
Transfer Lines (CTL) during operation of fusion machine.
• In an accidental scenario, the possibility of cold helium
release is evident due to complete breakage of process pipe
and Outer Vacuum Jacket (OVJ)
• The present study aims to estimate the lowest possible
temperature and change in pressure in the surrounding
environment due to the possible accidental scenario,
especially in a closed volume.
The parameters of helium mass flow from OVJ to EV are varied as a function of time.
The same temperature of mass flow is assigned for the entire length of the OVJ, for successive time steps.
Realizable k-epsilon viscous model was employed with enhanced wall treatment.
Temperature , Mass flow from OVJ
to EV at opening of rupture disc
Pressure Profile
Temperature profile
Helium Inventory
Mass flows for first 60s
The lowest temperature has been observed to be function of (i) cold helium inventory, (ii) size of opening in process pipe, (iii) discharge area of safety rupture
disc of OVJ, (iv) size of the surrounding duct or mass of surrounding air.
Unstable flows,
Higher heat loads
LIQUID HELIUM /
NITROGEN SOURCE
T
WARM HELIUM OR
NITROGEN GAS
T
T
T
T
RECOVERY SYSTEM/
VENT
T TT
V
V
V
P F
P F
ENCLOSED VOLUME
PROCESS PIPEOVJ
T
THERMAL IMAGING SYSTEM
P: Pressure Transmitter
T: Temperature Transmitter
F: Flow Transmitter
V: Valve
Conclusion • EV’s pressurization profile demands detailed experimental investigation,
considering the most severe case of accidental scenarios based on, (i) maximum
cold helium inventory, (ii) size of EV and (iii) ventilation requirements, which has to
be considered while designing the subsystems of large fusion reactor related
devices.
• For the purpose of investment protection, the outer vacuum jacket needs to be
designed for internal pressure and with the careful design of rupture disc
considering the maximum inventories in the process pipe.
• Ventilation systems have to be designed considering the possible pressurization of
the enclosed volume.