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Pour mieux affirmer ses missions, le Cemagref devient Irstea
Structuring case-studyCrystallization
Graciela ALVAREZ, H. BENKHELIFA, M. ARELLANO, D. LEDUCQ, D. FLICK ,
Irstea,APT,CSIC, UCL, UNIROMA
Workshop CAFE EFFOST 20th November 2012
2
Workshop CAFE EFFOST 20th November 2012 [email protected]
Process and industrial problem
Pasteurization 85°C
Storage
MixMix Ripening 4°C
12 to 24 hrs
Packaging, Moulding
55°°CC
-- 55°°CC
Initial Freezing Initial Freezing -- Freezer Freezer
Exit TExit T°°C C --5 to 5 to --66°°CC
Mixture 60°C Ingredients
Refrigerant fluid entry
Scraper blades
Refrigerant fluid
exit
Sorbet
mix
entry
Sorbet exit
30-50% ice
Ice crystal size < 50µm to
avoid undesirable quality:
coarse, grainy texture.
Homogenization
60°C - 200 bars
3
Workshop CAFE EFFOST 20th November 2012 [email protected]
On-line sensors
Freezing
MixMix
SorbetSorbet
Water %Water %
Sugar %Sugar %
Gum %Gum %
Ice CreamIce Cream
Energy Energy
ConsumptionConsumption
•• Ice crystal sizeIce crystal size
•• ViscosityViscosity
••TemperatureTemperature
Mix flow rateMix flow rate
[kg/s][kg/s]Dasher rotation speed Dasher rotation speed
[rpm][rpm]
Raw
material
Process
SSHEProduct
TT°°C Evap.C Evap.
[[°°C]C]
Sorbet crystallization : Water/ Sugar/ Gum without air
Controlled variables
Actuators
minmax and φφφφφφφφ ≥≥≥≥≤≤≤≤ iceice ddwithObjective function :
==== .min
ice
elec
m
Wj
&
Objectives
4
Workshop CAFE EFFOST 20th November 2012 [email protected]
Experimental Device
1 - Refrigerated storage tank
2 - Volumetric piston pump
3 - SSHE or Freezer
4 - Outlet pipe
5 - Exit temperature - Pt100 probe
6 - Ice crystal size - FBRM probe
7 - Product exit
FBRM
Probe
Pt100
Probe
Lemon
Sorbet
Lemon
sorbet mix
Frozen sorbet
exit
Pilot-scale SSHE or freezer WCB MF50 - Nominal capacity: 0.007 to 0.021 kg/s
5
Workshop CAFE EFFOST 20th November 2012 [email protected]
Focused beam reflectance measurement
Probe Window
principle Enlarged view
Path of Focused
Beam
Chord length = time period of
reflection light * laser beam
tangential speed
6
Workshop CAFE EFFOST 20th November 2012 [email protected]
Experimental Device
Rheology experimental study
1 - Refrigerated tank
2 - Piston pump
3 - SSHE or freezer
4 - Pt100 probe at inlet
5 - Pipe rheometer
6 - Pressure manometers
7 - Pt100 probe at inlet
8 - Product exit
7
Workshop CAFE EFFOST 20th November 2012 [email protected]
Ice crystallization study
Operating Conditions Coded Values
Factors Unity - αααα -1 0 +1 + αααα
X1 - Mix flow rate (kg/s)kg/h
0.00725
0.01035
0.01450
0.01865
0.02175
X2 - R22 Temperature (°°°°C) -10.60 -12.50 -15.25 -18 -19.90
X3 - Dasher speed(rad/s)
rpm57.07545
62.83600
78.54750
94.25900
104.721000
∑ ∑∑∑= =<=
+++=3
1
3
1
23
10
ˆi ji
jiijiiii
ii XXXXY ββββ
0β iβ iiβ ijβ
ji XX
Interception, linear, quadratic, interaction effect
Experimental conditions
Effect of 3 operating conditions on 2 responses:mean chord length - draw (exit) temperature of sorbe t
Y Predicted response
8
Workshop CAFE EFFOST 20th November 2012 [email protected]
Effect of process on exit temperature
78.54 rad/s (750 rpm)
↘↘↘↘↘↘↘↘ TeTe↘↘↘↘↘↘↘↘ Draw temperature Draw temperature ↗↗↗↗↗↗↗↗ XiceXice
MFR (MFR (↗↗↗↗↗↗↗↗ residence times) residence times) ↘↘↘↘↘↘↘↘ Draw Draw
temperaturestemperatures
Process ResultsProcess Results
DS and Te effect
↗↗↗↗↗↗↗↗ Dasher speed results in a slightly warming of Dasher speed results in a slightly warming of
the draw temperaturethe draw temperature
Te and MFR effect
(50 kg/h)
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Workshop CAFE EFFOST 20th November 2012 [email protected]
Effect of process conditions on mean chord lengthEffect of process conditions on mean chord length
78.54 rad/s (750 rpm) = cte
↘↘↘↘↘↘↘↘ TeTe↘↘↘↘↘↘↘↘ CL (Chord lenght)CL (Chord lenght)
MFR (MFR (↗↗↗↗↗↗↗↗ residence times) residence times) ↘↘↘↘↘↘↘↘not not
significant effect on CLsignificant effect on CL
Process ResultsProcess Results
DS and Te effect
↗↗↗↗↗↗↗↗ DS slightly warming of the exit temperatureDS slightly warming of the exit temperature
Te and MFR effect
(50 kg/h)= cte
↘↘↘↘↘↘↘↘ TeTe↘↘↘↘↘↘↘↘ CL (Chord lenght)CL (Chord lenght)
10
Workshop CAFE EFFOST 20th November 2012 [email protected]
Apparent viscosity measurementsApparent viscosity measurements
1 - Refrigerated tank
2 - Piston pump
3 - Freezer
4 - Outlet pipe
5 - Pt100 probe
6 - FBRM probe
7 - Product exit
8 - Tube viscometer
Lemon
sorbet mix
Laboratory scale pilot freezer WCB MF50
8
Frozen sorbet
exit stream
11
Workshop CAFE EFFOST 20th November 2012 [email protected]
Tube viscometerTube viscometer
w
w
d
dn
γσ&ln
ln=
; 2
)(
L
PRstressshearWall w
∆=σ
P∆
Slope:
Correction factor of wall
shear rate
3
4
R
VrateshearWall w π
γ&
& =
V&
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Workshop CAFE EFFOST 20th November 2012 [email protected]
1napp *K −= γη &
w
w
d
dn
γσ&ln
ln=
n
K
Slope:
flow behaviour index
Intercept:
consistency index
Tube viscometerTube viscometer
3
4*
4
13
R
V
n
ncorrectedw π
γ&
&+=
13
Workshop CAFE EFFOST 20th November 2012 [email protected]
Sorbet characterisation Sorbet characterisation withoutwithout airair
91.0
*66.12
54.0
=
=
R
w γσ &
94.0
*88.32
45.0
=
=
R
w γσ &
5% Ice 5% Ice contentcontent
9% Ice 9% Ice contentcontent
92.0
*81.72
41.0
=
=
R
w γσ &
14% Ice 14% Ice contentcontent
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Workshop CAFE EFFOST 20th November 2012 [email protected]
Sorbet characterisation Sorbet characterisation withoutwithout airair
Sorbet becomes more shear-thinning and more viscous
with the increase in the ice volume fraction within sorbet.
↗ Ice volume fraction ↘ Flow behaviour index ↗ Ice volume fraction ↗ Consistency index
15
Workshop CAFE EFFOST 20th November 2012 [email protected]
Sorbet characterisation with airSorbet characterisation with air
1
10
100
1 10 100
Sh
ear
stre
ss
(Pa)
Shear Rate (1/s)
Xv.a.=0.5 - Xv.i.=0.23
Xv.a.=0.335 - Xv.i.=0.23
Xv.a.=0.2 - Xv.i.=0.23
Xv.a.=0 - Xv.i.=0.23
airmix
air
VV
V.a.Xv
+= 100
V
VO%
mix
air ×=
shear-thinning behaviour
increases in the air volume
fraction
Fig. 2. Flow behaviour of sorbet at -3.9°C (Xv.i. = 0.23) as a function of the air volume fraction (Xv.a.) at mix flow rate of
0.007 kg.s-1 and rotational speed of 78.5 rad.s-1.
n=0.397
n=0.312
n=0.269
n=0.257
Air volume fraction % Overrun
100 %
50%
25%
No Overrun
16
Workshop CAFE EFFOST 20th November 2012 [email protected]
Sorbet characterisation with airSorbet characterisation with air
App viscosity as a function of the shear rate for sorbet at -3.9 °C
(Xv.i. = 23%), 0.007 kg.s -1 and rotational speed of 78.5 rad.s -1.
0
10
20
30
40
50
1 10 100Shear rate 1/s
App
aren
t vis
cosi
ty (
Pa.
s) Sorbet NoOverrun
Sorbet 100%Overrun (50%v/v)
= 0.8 Pa.s without air
airwithapp ....η = 1.6 Pa.s with air
appη
17
Workshop CAFE EFFOST 20th November 2012 [email protected]
Flow rate kg/h
Rotation speed rpm
Tsortie ºC
Fat content Fat content % %
Overrun %
n K (Pa.s) n ηηηη app (Pa.s) à10s-1
25 600 -5 66 75 0,395 48,423 12.00
25 400 -5 66 75 0.463 38.249 11.11
25 600 -5 1212 75 0.431 81.648 22.03
25 400 -5 1212 75 0.594 60.129 23.61
Ice cream characterisation with air Ice cream characterisation with air
+ + fat globulesfat globules
↗ Fat content % ↗ Apparent viscosity
Ice cream becomes more viscous with the increase in the fat
content.
18
Workshop CAFE EFFOST 20th November 2012 [email protected]
18
Ice Crystallisation modelling in the freezerIce Crystallisation modelling in the freezer
z=
r
• Plug flow in axial direction z : t resid = V/ Mix flow rate
• Crystallisation and heat transfer studied in functi on of
radial and axial position (t = z / v axial )
• Output variables : T out , Dmean, µout at steady state
Ri
Re Tmean
ωmean
at the scale of a REVRepresentative Elementary Volume
di
Dm
19
Workshop CAFE EFFOST 20th November 2012 [email protected]
19
Ice Crystallization modelling in the freezer
Equations : Population balance equation
+ Energy balance equation
+ State equation (u,T,ϕi)
Growth
G = ββββ (Tsat – T)γγγγ
Breakage
Nucleationheterogeneous nucleation at wall
(((( ))))δδδδ−−−−αααα==== esat TTN
Assumptions
Non equilibrium approach
Equilibrium curve
-16
-14
-12
-10
-8
-6
-4
-2
0
2
0 0,1 0,2 0,3 0,4 0,5 0,6 0,7
Sugar fraction
Fre
ezin
g P
oint
(°C
)
mix lemon
sucrose solution
Tsat for the mix obtained experimentally
νννν••••
ϕϕϕϕεεεε==== iscrapNB
20
Workshop CAFE EFFOST 20th November 2012 [email protected]
Model building, and model reduction
(((( ))))(L)B )RR()LL( N))t,L(.G(
Ltt,L
bec ++++−−−−δδδδ−−−−δδδδ====ψψψψ∂∂∂∂∂∂∂∂++++
∂∂∂∂∂ψ∂ψ∂ψ∂ψ� Population balance equation (without radial mixing)
2020
� PBE multiplied by Lj and integrated to obtain the moments� Balance equation for the moment given by:
(((( )))) 1j3/j1j
c1jj M.B.12NLM.G.j
dt
dM++++
−−−−−−−− −−−−++++++++====
� Ordinary equations :
dMo/dt = N + B M1
dM1/dt = G.Mo + N.Lc + B (22/3-1) M2
dM2/dt = 2.G.M1 + N. Lc2 + B (21/3-1) M3
dM3/dt = 3.G.M2 + N.Lc3 With
(((( ))))2
ee TTShdtdu ••••
γγγγµµµµ++++−−−−====
νννν••••
ϕϕϕϕεεεε==== iscrapNB
21
Workshop CAFE EFFOST 20th November 2012 [email protected]
Crystallization Model
Moments model
Energy balance
Growth, Nucleation and Breakage
Viscosity
The Parameters to be identified
22
Workshop CAFE EFFOST 20th November 2012 [email protected]
WP4: Model building, process dynamics and model reduction
22
Model parameters range
hehe alphapalphap betabeta xixi epsilonepsilon chichi LcLc
1400 1400 -- 32003200
W.mW.m--11.K.K--11
4.e8 4.e8 –– 1.5.e91.5.e9
ss--11.m.m--33.K.K--11
3.e3.e--7 7 –– 8.e8.e--77
m.sm.s--11.K.K--11
2020--3535 10 10 –– 50 50
mm--11
1.5 1.5 -- 33 4 4 –– 8 8
µµmm
Wall heat transfer coefficient heHeterogeneous Nucleation coefficient alphap
Growth coefficient beta
Adjustment parameter of sorbet viscosity xiViscous dissipation parameter chi
Initial crystal size Lc
Breakage constant epsilon
Results steady state approach
23
Workshop CAFE EFFOST 20th November 2012 [email protected]
Parameter identification WP6Parameter identification WP6
� Heterogeneous Nucleation coefficient α = 11.34 108 s-1m-2K-1
� Wall heat transfer coefficient h = 2894 Wm-2K-1
� Growth coefficient ββββ = 6.37 .10-7 ms -1K-1,
�Viscous dissipation parameter X= 25,82
�The initial crystal size Lc= 6.98 µm
�Viscosity coefficient ξξξξ = 3.85
CSIC : Eva Balsa, Carlos Vilas, Antonio Alonso
AMIGO Tools optimisation and IdentificationAMIGO Tools optimisation and Identification
24
Workshop CAFE EFFOST 20th November 2012 [email protected]
Parameter estimation
Weighting cost function
Fit quality (mean relative residual in %):> Temperature at the output: 6.9%> Chord length: 5.1%> Viscosity: 24.1%
he : 2.89428e+003� : 1.13448e+009� : 6.37008e-007�:25.82076Lc : 6.98353e-006 : 3.85328
5 10 15 20 25 30 35 40-40
-20
0
20
Rel pred error: 100*(Tdata-T)/Tdata). Mean error output:6.91630765477107
5 10 15 20 25 30 35 40
-505
1015
Rel pred error: 100*(Lcdata-Lc)/Lcdata). Mean error:5.09405012728256
2 4 6 8 10 12 14 16-80-60-40-20
020
Rel pred error: 100*(mudata-mu)/mudata). Mean error:24.0936050368514
CSIC : Eva Balsa, Carlos Vilas, Antonio Alonso
AMIGO Tools optimisation and AMIGO Tools optimisation and IdentificationIdentification
25
Workshop CAFE EFFOST 20th November 2012 [email protected]
Evaporation temperature results Experimental vs simulation
2525
(mix flow rate = 35 kg/h, dasher speed = 750 rpm)
steady state approach
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Workshop CAFE EFFOST 20th November 2012 [email protected]
Effet of evaporation temperature on Chord lenght .. Exp vs simulated
262626
(mix flow rate = 35 kg/h, dasher speed = 750 rpm)
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Workshop CAFE EFFOST 20th November 2012 [email protected]
WP5: Sensors
University of RomaResults of Electronic Nose Experiment at Irstea
� 6 experimental conditions created varying the following parameters:� Flow ice-cream machine (from 25 to 35 l/h)� Tevap refrigerant liquid (from -9 °C to -16.2 °C)� Mix flow rate (from 25 to 35 l/h(?))
� 36 measurements in two consecutive days.� Target parameters:
� Size crystals [µm]� Model estimated viscosity [Pa s]
28
Workshop CAFE EFFOST 20th November 2012 [email protected]
WP7 : Process monitoring and controlCeline Casenave (INRA) & Denis Dochain (UCL)
29
Workshop CAFE EFFOST 20th November 2012 [email protected]
Thank you for you attentionThank you for you attention
The research leading to these results has received funding from the European Community‘s Seventh Framework Programme