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Injection Moulding Simulation
of Engineering Rubber Components
Modelling of Elastomeric Materials and Products14 Oct 2010 - London, UK
G.Ramorino
S. Agnelli , A.Franceschini , F.Baldi, T.Riccò
1University of Brescia (Italy) – Department of Mechanical and Industrial Engineering
2CF Gomma, Brescia (Italy)
- INJECTION MOULDED RUBBER COMPONENTS
� ANTIVIBRATION RUBBER COMPONENTS
CF GOMMA Spa (Brescia, Italy)
rubber compound
• ENGINE MOUNTS
• BUSHES FOR THE SUSPENSIONS
metal
rubber compound
► OPTIMIZE THE PERFORMANCE OF NEW PRODUCTS ◄
� COMPUTER AIDED ENGINEERING SOFTWARE
DESIGN TECHNOLOGY
PREVENT MOULDING PROBLEMS
Incomplete mould filling / air traps
► QUICKLY ANALISIS OF COMPONENT/MOULD
► AVOID SEVERAL ERRORS
(early phase of product development)
- NUMERICAL SIMULATION
► SAVE COST AND TIME ON MOULD TRYOUTS
� CORRECT EVALUATION OF THE CURING TIME
optimize the time cycle of the vulcanization phase of the component
► USEFUL FOR COST SAVING IN THE PRODUCT PROCESS ◄
► OPTIMIZE PART DESIGN
► SAVE COST AND TIME ON MOULD TRYOUTS
► REDUCE TIME TO MARKET
- COMMERCIAL SOFTWARE
� extensive materials property database
► THERMOPLASTIC – THERMOSET MATERIALS
� developed in close cooperation with the plastics industry
MOLDFLOW ���� LEADING CAE SOFTWARE OF INJECTION MOULDING
� measurements of curing rate - material viscosity are needed
► RUBBER COMPOUNDS
� database is out of material property
► PROPER CURING REACTION AND VISCOSITY MODELS
� MOLDFLOW SIMULATIONS
VERIFY THE CAPABILITY OF THE MOLDFLOW SOFTWARE TO PERFORM FLOW SIMULATIONS OF
RUBBER INJECTION MOULDING PARTS
- AIM OF THE PRESENT WORK
1. MOULD CAVITY FILLING STAGE
2. STATE OF CURE IN THE
POST-FILLING PROCESS
� EXPERIMENTAL TESTS
POST-FILLING PROCESS
► COMPARISON ◄
► ANTIVIBRATION ENGINE MOUNT
� thickness: 1.5 mm to 20 mm
� two metal inserts
200 mm
� overall dimensions: 170x80x45 mm
- RUBBER COMPONENT
METAL INSERT
80 m
m
TYPICAL INDUSTRIAL FORMULATION
NATURAL RUBBER COMPOUND (carbon black-silica-oil-zinc oxide curing system)
� composition of the rubber compound
� test temperature
� method employed to characterize the material
� vulcanization of NR compounds is conducted in a DSC
DSC (Heat Flux from TA Instruments)
- MATERIAL CHARACTERIZATION
(Dynamic Scanning Calorimeter)
CURE KINETIKS
DSC (Heat Flux from TA Instruments)
� isothermal and non-isothermal conditions
� INDUCTION PERIOD
� RATE OF CURE
1. SPECIFIC HEAT OF REACTION H (J/G)
2. CONSTANTS OF THE MODELS - “CLAXTON-LISKA” - “KAMAL-SOUROUR”
11
11.5
12
12.5
Heat
Flo
w (
mW
)A
non-isothermal DSC test
� SPECIFIC HEAT OF REACTION ���� H (J/g)
- MATERIAL CHARACTERIZATION
9.5
10
10.5
12 13 14 15 16 17
Time (min)
Heat
Flo
w (
mW
)
� heating rate of 10°C/min
� mass of the sample m = 10 mg
H (J/g) =A (mJ)
m (mg)� temperature range 70-220°C.
exothermic reaction peak
� MODEL TO CHARACTERIZE THE INDUCTION PERIOD
T (°C) 170 175 180 183
t (s) 133 79 46 34
)/exp( TBAt ⋅=
� CLAXON - LISKA MODEL
A, B = constants
4.2
4.4
Isothermal DSC testsT(°C)
Arrenhius type expression
T = temperature
- MATERIAL CHARACTERIZATION
INDUCTION TIME
3
3.2
3.4
3.6
3.8
4
4.2
0 100 200 300 400
Time (s)
He
at
Flo
w (
mW
)
Isothermal DSC testsT(°C)
� INDUCTION TIME ���� t (s)
T (°C) 170 175 180 183
t (s) 133 79 46 34
4.2
4.4
Heat
Flo
w (
mW
)
)/exp( TBAt ⋅=
� CLAXON - LISKA MODEL
Isothermal DSC data
A, B = constants
T = temperature
∆∆∆∆Ht1
- MATERIAL CHARACTERIZATION
INDUCTION TIME
(data of ti obtained at each isothermal DSC tests)
INDUCTION PERIOD OF THE NR
COMPOUND
3
3.2
3.4
3.6
3.8
4
0 50 100 150 200 250 300 350 400
Time (s)
Heat
Flo
w (
mW
)
temperature = 183°C
t
∆∆∆∆Htot
∆∆∆∆Htot
cure degree αt1 = ∆∆∆∆Ht1
t1
exothermic reaction
0.4
0.6
0.8
1
Cu
re d
eg
ree
, α
T
� CURE KINETICS CURVES
� MODEL TO CHARACTERIZE THE CURE KINETICS
- MATERIAL CHARACTERIZATION
(from the isothermal DSC data)
(100% cure)
0
0.2
0 100 200 300 400
Time (s)
Cu
re d
eg
ree
,
nmKK
dt
d)1()( 21 αα
α−⋅⋅+=
rate of cure m, n = constants K1 (T) , K2 (T)
� KAMA-SOUROUR MODEL *
A. Arrillaga et al. European Polymer Journal,43: 4783–4799, 2007.
*
temperature T (170,175,180,183 °C)
(0% cure)
� CURE KINETICS CURVES
0.008
0.012
0.016
0.02
0.024
Rate
of
cu
re,
dα
/dt
temperature T (170,175,180,183°C)
T
- MATERIAL CHARACTERIZATION
(data used to obtain the
constants of the
Kama-Sorour Model )
0
0.004
0.008
0 0.2 0.4 0.6 0.8 1
Cure degree, α
Rate
of
cu
re
Isothermal tests
nmKK
dt
d)1()( 21 αα
α−⋅⋅+=
rate of cure
� KAMA-SOUROUR MODEL *
m, n = constants K1 (T) , K2 (T)
A. Arrillaga et al. European Polymer Journal,43: 4783–4799, 2007.
*
0.004
0.008
0.012
0.016
0.02
0.024
Ra
te o
f c
ure
dα
/dt
temperature T (170,175,180,183°C)
T
GOOD AGREEMENT
- MATERIAL CHARACTERIZATION
0
0.004
0 0.2 0.4 0.6 0.8 1Cure degree, α
Ra
te o
f c
ure
d
Isothermal tests
nmKK
dt
d)1()( 21 αα
α−⋅⋅+=
rate of cure
A. Arrillaga et al. European Polymer Journal,43: 4783–4799, 2007.
*
m, n = constants K1 (T) , K2 (T)
� KAMA-SOUROUR MODEL * (open symbols)
experimentalmodel
� capillary rheometer (CEAST)
� flow curves at different temperatures
RHEOLOGICAL PROPERTIES
- MATERIAL CHARACTERIZATION
(data used to obtain the
constants of the
Reactive Viscosity Model )
3.8
4.2temperature T (120, 130, 140, 150 °C)
2.2
2.6
3.0
3.4
3.8
1.0 1.5 2.0 2.5 3.0 3.5
Log γγγγ (1/s)
Lo
g η
η
η
η
(P
a·s
)
T
� REACTIVE VISCOSITY MODEL
( )α+
−
α−α
α
τ
γη+
η=γαη
21 CC
g
g
n1
0
0
)T(1
)T(),T,(
&
&
5.0
6.0
Reactive viscosity model (120°C)
η0(T) = viscosity at shear rate � 0;
T = temperature;
n = shear rate sensitivity;
τ = shear stress;
α = cure degree;
C1, C2, αg = constants.
- MATERIAL CHARACTERIZATION
1.0
2.0
3.0
4.0
5.0
0.0 1.0 2.0 3.0 4.0 5.0
Log γγγγ (1/s)
Lo
g η
(P
a·s
)
120°C
150°C
Reactive viscosity model (150°C)
Experimental data
GOOD AGREEMENT
- MOLDFLOW MODELLING
0.016
0.02
0.024
Ra
te o
f c
ure
dα
/dt
temperature T (170,175,180,183°C)
T
3
3.2
3.4
3.6
3.8
4
4.2
4.4
0 100 200 300 400
Time (s)
He
at
Flo
w (
mW
)
- MOLDFLOW DATA INPUT
MODEL PARAMETERS
INPUT TO MOLDFLOW
0
0.004
0.008
0.012
0 0.2 0.4 0.6 0.8 1Cure degree, α
Ra
te o
f c
ure
d
1.0
2.0
3.0
4.0
5.0
6.0
0.0 1.0 2.0 3.0 4.0 5.0
Log γγγγ (1/s)
Lo
g η
(P
a·s
)
120°C
150°C
Reactive viscosity model (150°C)
Reactive viscosity model (120°C)
Experimental data
“REACTIVE MOULDING” MODULE
� PROCESS PARAMETERS
Injection machine: Mod. V/MP 70/800
Injection time (s): 20
Injection temperature (°C): 65
Mold temperature (°C): 165
Cure times (s): 380, 420, 475, 520
INPUT TO MOLDFLOW
- MOLDFLOW DATA INPUT
INPUT TO MOLDFLOW
- 3D MOLDFLOW MODELLING – CAVITY FILLING
METAL
FEED SYSTEM
METAL INSERT
POSITION OF THE FLOW FRONT AS THE CAVITY FILLS vs INTERRUPTED FILLING EXPERIMENTS
FILL TIME RESULT
METAL INSERT
CAVITY
MOULD
6 gate system
- 3D MOLDFLOW MODELLING – CAVITY FILLING
“comparison between the pictures of the incomplete
molded parts and the corresponding filling patterns
predicted by computer simulation”
- FILL TIME RESULT
THE PREDICTIONS ARE REPRESENTATIVE OF THE FLOW
DURING THE FILLING STAGE
REMARKABLE AGREEMENT
- MATERIAL CURING
ACTUAL MATERIAL CONVERSION (CURE) AT A NODE, CALCULATED OVER THE ENTIRE MOLDING PROCESS
CONVERSION AT NODE RESULT
N1
N1: located near the
cavity surface
N2
sectionsimulations are
performed in a part of
variable thickness
N2: located in the centre of the higher thickness
cure profile evolution
- MATERIAL CURING
CONVERSION AT NODE RESULT: XY PLOT – cure profile evolution
MO
LD
FL
OW
PR
ED
ICT
ION
S N2
N1
~ 0.75
~ 0.95
scorchC
ure
deg
ree
MO
LD
FL
OW
PR
ED
ICT
ION
S
FILLING (20 s) + CURING PHASES
N1: located near the
cavity surface (↑ T)
N2: located in the centre
of the higher thickness
slower heat transfer
scorch
Total cycle
Cu
re d
eg
ree
slower rate of cure
- MECHANICAL COMPRESSION TEST
TO EVALUATE WHICH CURING TIME PROVIDES THE
HIGHER STIFFNESS OF THE PART, SO INDICATING THE BEST CURING TIME
components obtained at different cure times (380, 420, 475, 520 s)
- COMPARISON
150
155
160
Sti
ffn
ess (
N/m
)
Experimental data
GOOD AGREEMENT
THE SOFTWARE PREDICTS 400-430 s THAT IS IN GOOD AGREEMENT WITH THE 440 s
FOUND THROUGH COMPRESSION TESTS
140
145
350 400 450 500 550 600
total cycle time (s)
Sti
ffn
ess (
N/m
)
MOLDFLOW PREDICTIONS
FILLING (20 s) + CURING PHASES
- CONCLUSIONS
� This study shows that it is possible to model very accurately the filling and cure
stages of rubber injection molding process.
� The computations are found in good agreement with the experimental results,
indicating that reliable information on material viscosity and curing kinetic play a
key role for well-founded predictions.key role for well-founded predictions.
ACKNOWLEDGEMENT
The authors want to acknowledge CF Gomma Spa (Brescia, Italy) and Fondazione
Cariplo for the financial supports.