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Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04
www.ijera.com 1 | P a g e
A Study on Stochastic Thermal Characterization of Electronic
Packages
Zakaria El Haddad*, Othmane Bendaou, Larbi El Bakkali
Modeling and Simulation of Mechanical Systems Laboratory, Abdelmalek Essaâdi University, Faculty of
Sciences .BP.2121, Mhannech, 93030, Tetouan, Morocco
ABSTRACT
Insofar as the electronics can be found now in several applications of multiple domains, we have tried to
highlight in this study that, those systems must be based on unquestionable reliability and meet the needs of the
external environment. Starting from the unit "°c / w" concerning the thermal resistance from the gap between
junction temperature and a reference temperature, we have tried to compare the thermal performance of
electronic packages taking into consideration the thermal management. Our approach is based on the Monte
Carlo simulation and the stochastic characterization of the QFN. From the norm of normalization, we have
obtained standardized data sheets allowing accurate comparisons of the thermal performance of electronic
packages as produced by different manufacturers. Our numerical model through simulation, prototyping
concerning the design involves the JEDEC recommendations, which we consider a very interesting alternative.
Through the deterministic analysis, we conducted an analysis from the Matlab program parameters, which
control the Ansys software, the results were processed by statistical techniques to evaluate the times of the
thermal resistance of the QFN. That is why we must consider the electronic package (encapsulating the
integrated circuit), through the printed circuit board (PCB) to ensure the junction temperature maintenance and
avoid the dissipation of the heat. Also our process was based on the union of the finite element method to the
Monte Carlo simulation and stochastic characterization of the QFN.
Keywords: Electronic package; Finite element method; printed circuit board (PCB); Quad Flat No Lead
(QFN); Simulation of Monte Carlo; Thermal resistance.
I. INTRODUCTION
Nowadays electronics play a crucial role in
several applications: medicine, embedded systems of
transportation, and telecommunication. While
achieving electrical functions, electronic systems
must be safe, reliable, have low thermal resistance
(to dissipate the heat properly) and must be durable
and insensitive to the exterior environment
variations (humidity, thermal and mechanical shock
...). [1]
All integrated circuits generate heat when
power is applied. Therefore, to maintain their
junction temperature below the maximum allowed,
electronic package dissipate the effective heat
(encapsulating the integrated circuit) through the
printed circuit board (PCB) and to the ambient air is
essential [2]-[3].
Thus, we should take in account the thermal
management when selecting electronic packages to
ensure high reliability of the final product. Indeed,
designers of electronic systems must have at their
disposal the thermal performance of electronic
packages to determine their environmental limits.
Thermal resistance is a data, which allows the
engineers to compare the performance of electronic
packages of different suppliers. This data is being
assessed in an experiment aligning with international
standards.
A key assumption during the thermal
characterization of electronic packages is that the
problem is deterministic, meaning that the
parameters of the problem are constant. However, by
making a few experiments, we concluded the limits
of a deterministic modeling. Indeed, there are always
differences between calculated quantities and those
measured. The causes are related to the uncertainties
in the geometry, material properties, boundary
conditions or loads. This has a considerable
influence on the thermal behavior of electronic
systems. Hence, the interests to take account these
uncertainties and determine the dispersions of the
output (thermal resistance) [4].
II. THERMAL RESISTANCE
The characterization of the thermal
performance of an electronic package was created
through the "heat resistance". This parameter, which
is appealed by « θ » is internationally evaluated,
compared, and operated by industrial electronics.
This latter is the measure of the ability of a package
to transfer heat generated by the integrated circuit
(die) to the ambient air or to the PCB. Practically,
the thermal resistance is the difference between the
junction temperature and the steady state reference
RESEARCH ARTICLE OPEN ACCESS
Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04
www.ijera.com 2 | P a g e
temperature for each watt of heat flux generated by
the upper surface of the die. Its unit is « c° / w ».
The thermal resistance of the junction at
room temperature « θJA » is the commonly used to
compare the thermal performance of the electronic
package. It is evaluated via the equation (1) knowing
that «TJ » and « TA » are respectively the junction
temperature and the ambient temperature (Fig.1).
1
.
Power of Die
T T
J A c w
JA



 
 
  
(1)
Fig.1.TJ and TA
III. NORMS
The evaluation of the thermal resistance of
an electronic package is as follows: the latter is
welded onto a PCB. We fuels the die, once the
steady state is established; the junction and ambient
temperatures are reported via thermocouples, and
finally, the resistance is calculated using the
equation (1). The factors, which can influence the
evaluation of «θJA» (except for the concerned
package), are:
- Geometry (dimensions and thickness) and the
PCB’s materials.
- The countenance rates of the PCB in copper.
- The orientation of the PCB (horizontal or
vertical).
- The volume of the air surrounding the PCB and
flow velocity.
In order to eliminate the influence of these
factors on the thermal performance they must report
the industrial packaging on the data sheets of their
products; standards were developed and adopted by
"Electronics Industries Association (EIA)". These
standards describe the procedures and settings with
which we must align during thermal characterization
of electronic packages. The purpose of this standard
is to have standardized data sheets to enable an
accurate and meaningful comparison of the thermal
performance of electronic packages produced by
different manufacturers.
3-1 Three standardized tests for basic PCB
The JEDEC standards [3] focus mainly on
the PCB used for measures seen the major influence
of the latter. Thus, three standardized PCBs are used
for the assessment of « θJA »:
- "Low Effective" Thermal Conductivity Board
(1S0P: Top surface of Cu traces only);
- "High Effective" Thermal Conductivity Board
(1S2P: Top surface of Cu traces buried planar
Cu + 2);
- "High Effective" Thermal Conductivity Board
with Features Direct Attach (1S2P+ Vias: Top
Surface traces Cu + Cu + 2 buried planar+
thermal Vias).
The PCB Standards are in FR4 and have
geometrical characteristics (Tab.I):
Table 1: Dimensions of PCB
3-2 Units Standardized environmental
conditions: air at rest case
According to the JEDEC standards [2], the
PCB must be positioned horizontally (top package)
in a closed chamber, which prevents the intrusion of
air currents, allowing only the transfer of heat by
natural convection with air at rest. The enclosure
must have internal dimensions as nominal « 305 x
305 x 305 (mm3) » and must be made of low
thermal conductivity material (less than 0.5 W /
m.K). The enclosure is placed on a support also low
thermal conductivity material.
IV. NUMERICAL MODEL
During the phase of design and prototyping,
the standardized thermal characterization of
electronic packages may prove costly in terms of
time and means. Developing a reliable numerical
model that is realistic and which integrates the
JEDEC recommendations is a very interesting
alternative. Thus, the designing of experiments can
be carried out without limitations via the simulation.
In our case, the most appropriate approach
is the one based on the finite element method
combined with the method of Monte Carlo.
The finite element method allows the
resolution of the heat equation, something you
cannot achieve analytically due to the complexity of
the geometry (PCB Electronics Package +). In this
case, the output of the model is the temperature
field, while the entries of the model of the finite
elements are:
- Geometry: electronic package welded to a
standardized PCB;
- Material properties: thermal conductivities of
the various layers of materials;
PCB 114.3×76.2×1.6 (mm3
)
Buried Planes 74.2×74.2×0.035 (mm3
)
Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04
www.ijera.com 3 | P a g e
- Load: the created power (By the Joule effect) on
the upper side of the IC (die);
- Boundary conditions: natural convection with
air at rest modeled via convection coefficients.
On the other hand, the estimation of the
moments (average and variance) of the thermal
resistance can be obtained by Monte Carlo
simulation, [5] which we will combine with the
finite element model. Despite its high cost in
calculation time, this classic method is widely used
and serves as a reference for approximate
calculations. The thermal resistance « θJA » will be
viewed as a random variable image of basic random
variables. The simulations include the construction
of a sample « (θJA)1, (θJA)2… (θJA)n » of the random
variable « θJA » and to treat this sample by the usual
statistical techniques. The "n" simulations are carried
out in an independent manner under the law of
distribution of basic random variables.
V. STOCHASTIC THERMAL
CHARACTERIZATION OF A QFN
In this work, we applied the proposed
approach to characterize a type of electronic package
"Quad Flat No Lead (QFN)" [6] (Fig.2) that is part of
the family of packages with a scale similar to that of
CI and which are welded directly on the PCB. The
QFN has connections at its lower perimeter; they
allow the electrical connection between the IC and
the electrical PCB layout. It also has a thermal pad to
increase the heat transfer.
Fig.2.Quad Flat No leads (QFN)
The proposed package to be characterized is
a « QFN -28 IO - 7.2 x 7.2 x 1.4 mm3 » and the
dimensions and the material properties are shown in
the figures below (Fig.3) and (Tab.II). The
temperature of the ambient air is assumed «20°c ».
While, the power generated by the IC is assumed to
be «1 Watt».
Fig.3. Dimensions of QFN
Table 2: Conductivities of the materials of QFN.
Component material   K w/m.c°
Die Si 148
Die Attach Epoxy 60
Overmold Epoxy 1.04
Cu Cu 385
PCB FR4 0.4
Solder SnAg 55
Finite element analysis was performed using
the commercial code "Ansys". We opted for a regular
mesh (made possible by a programming script)
whose elements are rectangular parallelepipeds at 8
knots (Fig.4). This allows for the control of the
number of mesh layers and an increase in accuracy.
Fig.4. Mesh geometry of QFN welded on a PCB
5-1 Deterministic Analysis
At first, the thermal characterizations of the
QFN were performed assuming that all the
parameters of the problem are deterministic. The
junction temperature output of the FE model is «
67°c » (Fig.5). Therefore, the thermal resistance of
QFN is « 47 c°/w ». This result correlates with the
thermal performance provided by electronic
packages for QFN producers whose dimensions are
close to those of QFN characterized in this work.
Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04
www.ijera.com 4 | P a g e
Fig.5. Temperature field result of FE model
5-2 Stochastic Analysis
The stochastic analysis was performed
assuming that the following parameters are Gaussian
when a standard deviation is « 8% » of the nominal
value: Conductivity of PCB, PCB dimensions, IC’s
power and Ambient Temperature. 300 samples of
the parameters have been created via a Matlab
program that controls the Ansys software and gives
the results to it. These are processed by statistical
techniques to assess the times of the thermal
resistance of the QFN. The results of the Monte
Carlo simulation (Tab.III) show that the thermal
resistance is sensitive to the input variations. Indeed,
in our case, the standard deviation is « 12% ».
Table 3: Moments of the Thermal Resistance of
QFN
Average Standard Deviation
 JAθ c°/w 47.35 5.75
VI. CONCLUSION
In this work, we have adopted an approach
allowing the thermal characterization of electronic
packages through simulation taking into
consideration the uncertainties. This approach
consists of combining the finite element method
with the Monte Carlo simulation. Stochastic
characterization QFN revealed a significant
dispersion of its thermal resistance. This information
is crucial; it will allow for the development of more
reliable electronic systems, since the consideration
of the dispersions of the resistances in the design
will define realistic junction temperatures that do not
exceed their limits.
REFERENCES
[1]. S. ASSIF, M. AGOUZOUL, A. EL HAMI,
O. BENDAOU and Y.GBATI. “Numerical
model to simulate the drop test of printed
circuit board (PCB)”. Advanced Materials
Research, Vol.423, pp 26-30, Trans Tech
Publications, Switzerland doi:
10.4028www.scientific.net/AMR.423.26.
2012.
[2]. JEDEC Standard n° 51-2A, “Integrated
Circuits Thermal Test Method
Environmental Conditions - Natural
Convection (Still Air)”, 2008.
[3]. JEDEC Standard n° 51-7, “High Effective
Thermal Conductivity Test Board for
Leaded Surface Mount Packages”, 2005.
[4]. O. Bendaou, J. E. Rojas, A. El Hami, A.
Aannaque, M. Agouzoul, “Stochastic and
reliability analysis of a propeller with
model reduction”, European Journal of
Computational Mechanics. Volume 18 –
No. 2/2009.
[5]. O. Bendaou, F. Bourzeix, B. Lakssir, A. El
Hami, M. Agouzoul, L. El Bakkali, “BGA
Warpage Investigations by Measurement
and Stochastic FEA”, Congrès Marocain de
Mécanique, Agadir, Avril 2013.
[6]. J. Wilde, E. Zukowski, “Comparative
Sensitivity Analysis for BGA and QFN
Reliability” Thermal, Mechanical and
Multi-Physics Simulation Experiments in
Microelectronics and Micro-Systems, 2007.
EuroSime 2007. International Conference.
London, pp. 1-7, April 2007.
[7]. X. He, ANSYS Tutorial, Department of
Mechanical Engineering, University of
Minnesota, Class material for short course
for ANSYS (7.0) in Mechanical
Engineering Department , October 2003.

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A Study on Stochastic Thermal Characterization of Electronic Packages

  • 1. Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04 www.ijera.com 1 | P a g e A Study on Stochastic Thermal Characterization of Electronic Packages Zakaria El Haddad*, Othmane Bendaou, Larbi El Bakkali Modeling and Simulation of Mechanical Systems Laboratory, Abdelmalek Essaâdi University, Faculty of Sciences .BP.2121, Mhannech, 93030, Tetouan, Morocco ABSTRACT Insofar as the electronics can be found now in several applications of multiple domains, we have tried to highlight in this study that, those systems must be based on unquestionable reliability and meet the needs of the external environment. Starting from the unit "°c / w" concerning the thermal resistance from the gap between junction temperature and a reference temperature, we have tried to compare the thermal performance of electronic packages taking into consideration the thermal management. Our approach is based on the Monte Carlo simulation and the stochastic characterization of the QFN. From the norm of normalization, we have obtained standardized data sheets allowing accurate comparisons of the thermal performance of electronic packages as produced by different manufacturers. Our numerical model through simulation, prototyping concerning the design involves the JEDEC recommendations, which we consider a very interesting alternative. Through the deterministic analysis, we conducted an analysis from the Matlab program parameters, which control the Ansys software, the results were processed by statistical techniques to evaluate the times of the thermal resistance of the QFN. That is why we must consider the electronic package (encapsulating the integrated circuit), through the printed circuit board (PCB) to ensure the junction temperature maintenance and avoid the dissipation of the heat. Also our process was based on the union of the finite element method to the Monte Carlo simulation and stochastic characterization of the QFN. Keywords: Electronic package; Finite element method; printed circuit board (PCB); Quad Flat No Lead (QFN); Simulation of Monte Carlo; Thermal resistance. I. INTRODUCTION Nowadays electronics play a crucial role in several applications: medicine, embedded systems of transportation, and telecommunication. While achieving electrical functions, electronic systems must be safe, reliable, have low thermal resistance (to dissipate the heat properly) and must be durable and insensitive to the exterior environment variations (humidity, thermal and mechanical shock ...). [1] All integrated circuits generate heat when power is applied. Therefore, to maintain their junction temperature below the maximum allowed, electronic package dissipate the effective heat (encapsulating the integrated circuit) through the printed circuit board (PCB) and to the ambient air is essential [2]-[3]. Thus, we should take in account the thermal management when selecting electronic packages to ensure high reliability of the final product. Indeed, designers of electronic systems must have at their disposal the thermal performance of electronic packages to determine their environmental limits. Thermal resistance is a data, which allows the engineers to compare the performance of electronic packages of different suppliers. This data is being assessed in an experiment aligning with international standards. A key assumption during the thermal characterization of electronic packages is that the problem is deterministic, meaning that the parameters of the problem are constant. However, by making a few experiments, we concluded the limits of a deterministic modeling. Indeed, there are always differences between calculated quantities and those measured. The causes are related to the uncertainties in the geometry, material properties, boundary conditions or loads. This has a considerable influence on the thermal behavior of electronic systems. Hence, the interests to take account these uncertainties and determine the dispersions of the output (thermal resistance) [4]. II. THERMAL RESISTANCE The characterization of the thermal performance of an electronic package was created through the "heat resistance". This parameter, which is appealed by « θ » is internationally evaluated, compared, and operated by industrial electronics. This latter is the measure of the ability of a package to transfer heat generated by the integrated circuit (die) to the ambient air or to the PCB. Practically, the thermal resistance is the difference between the junction temperature and the steady state reference RESEARCH ARTICLE OPEN ACCESS
  • 2. Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04 www.ijera.com 2 | P a g e temperature for each watt of heat flux generated by the upper surface of the die. Its unit is « c° / w ». The thermal resistance of the junction at room temperature « θJA » is the commonly used to compare the thermal performance of the electronic package. It is evaluated via the equation (1) knowing that «TJ » and « TA » are respectively the junction temperature and the ambient temperature (Fig.1). 1 . Power of Die T T J A c w JA           (1) Fig.1.TJ and TA III. NORMS The evaluation of the thermal resistance of an electronic package is as follows: the latter is welded onto a PCB. We fuels the die, once the steady state is established; the junction and ambient temperatures are reported via thermocouples, and finally, the resistance is calculated using the equation (1). The factors, which can influence the evaluation of «θJA» (except for the concerned package), are: - Geometry (dimensions and thickness) and the PCB’s materials. - The countenance rates of the PCB in copper. - The orientation of the PCB (horizontal or vertical). - The volume of the air surrounding the PCB and flow velocity. In order to eliminate the influence of these factors on the thermal performance they must report the industrial packaging on the data sheets of their products; standards were developed and adopted by "Electronics Industries Association (EIA)". These standards describe the procedures and settings with which we must align during thermal characterization of electronic packages. The purpose of this standard is to have standardized data sheets to enable an accurate and meaningful comparison of the thermal performance of electronic packages produced by different manufacturers. 3-1 Three standardized tests for basic PCB The JEDEC standards [3] focus mainly on the PCB used for measures seen the major influence of the latter. Thus, three standardized PCBs are used for the assessment of « θJA »: - "Low Effective" Thermal Conductivity Board (1S0P: Top surface of Cu traces only); - "High Effective" Thermal Conductivity Board (1S2P: Top surface of Cu traces buried planar Cu + 2); - "High Effective" Thermal Conductivity Board with Features Direct Attach (1S2P+ Vias: Top Surface traces Cu + Cu + 2 buried planar+ thermal Vias). The PCB Standards are in FR4 and have geometrical characteristics (Tab.I): Table 1: Dimensions of PCB 3-2 Units Standardized environmental conditions: air at rest case According to the JEDEC standards [2], the PCB must be positioned horizontally (top package) in a closed chamber, which prevents the intrusion of air currents, allowing only the transfer of heat by natural convection with air at rest. The enclosure must have internal dimensions as nominal « 305 x 305 x 305 (mm3) » and must be made of low thermal conductivity material (less than 0.5 W / m.K). The enclosure is placed on a support also low thermal conductivity material. IV. NUMERICAL MODEL During the phase of design and prototyping, the standardized thermal characterization of electronic packages may prove costly in terms of time and means. Developing a reliable numerical model that is realistic and which integrates the JEDEC recommendations is a very interesting alternative. Thus, the designing of experiments can be carried out without limitations via the simulation. In our case, the most appropriate approach is the one based on the finite element method combined with the method of Monte Carlo. The finite element method allows the resolution of the heat equation, something you cannot achieve analytically due to the complexity of the geometry (PCB Electronics Package +). In this case, the output of the model is the temperature field, while the entries of the model of the finite elements are: - Geometry: electronic package welded to a standardized PCB; - Material properties: thermal conductivities of the various layers of materials; PCB 114.3×76.2×1.6 (mm3 ) Buried Planes 74.2×74.2×0.035 (mm3 )
  • 3. Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04 www.ijera.com 3 | P a g e - Load: the created power (By the Joule effect) on the upper side of the IC (die); - Boundary conditions: natural convection with air at rest modeled via convection coefficients. On the other hand, the estimation of the moments (average and variance) of the thermal resistance can be obtained by Monte Carlo simulation, [5] which we will combine with the finite element model. Despite its high cost in calculation time, this classic method is widely used and serves as a reference for approximate calculations. The thermal resistance « θJA » will be viewed as a random variable image of basic random variables. The simulations include the construction of a sample « (θJA)1, (θJA)2… (θJA)n » of the random variable « θJA » and to treat this sample by the usual statistical techniques. The "n" simulations are carried out in an independent manner under the law of distribution of basic random variables. V. STOCHASTIC THERMAL CHARACTERIZATION OF A QFN In this work, we applied the proposed approach to characterize a type of electronic package "Quad Flat No Lead (QFN)" [6] (Fig.2) that is part of the family of packages with a scale similar to that of CI and which are welded directly on the PCB. The QFN has connections at its lower perimeter; they allow the electrical connection between the IC and the electrical PCB layout. It also has a thermal pad to increase the heat transfer. Fig.2.Quad Flat No leads (QFN) The proposed package to be characterized is a « QFN -28 IO - 7.2 x 7.2 x 1.4 mm3 » and the dimensions and the material properties are shown in the figures below (Fig.3) and (Tab.II). The temperature of the ambient air is assumed «20°c ». While, the power generated by the IC is assumed to be «1 Watt». Fig.3. Dimensions of QFN Table 2: Conductivities of the materials of QFN. Component material   K w/m.c° Die Si 148 Die Attach Epoxy 60 Overmold Epoxy 1.04 Cu Cu 385 PCB FR4 0.4 Solder SnAg 55 Finite element analysis was performed using the commercial code "Ansys". We opted for a regular mesh (made possible by a programming script) whose elements are rectangular parallelepipeds at 8 knots (Fig.4). This allows for the control of the number of mesh layers and an increase in accuracy. Fig.4. Mesh geometry of QFN welded on a PCB 5-1 Deterministic Analysis At first, the thermal characterizations of the QFN were performed assuming that all the parameters of the problem are deterministic. The junction temperature output of the FE model is « 67°c » (Fig.5). Therefore, the thermal resistance of QFN is « 47 c°/w ». This result correlates with the thermal performance provided by electronic packages for QFN producers whose dimensions are close to those of QFN characterized in this work.
  • 4. Zakaria El Haddad.et al. Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 8, ( Part -1) August 2016, pp.01-04 www.ijera.com 4 | P a g e Fig.5. Temperature field result of FE model 5-2 Stochastic Analysis The stochastic analysis was performed assuming that the following parameters are Gaussian when a standard deviation is « 8% » of the nominal value: Conductivity of PCB, PCB dimensions, IC’s power and Ambient Temperature. 300 samples of the parameters have been created via a Matlab program that controls the Ansys software and gives the results to it. These are processed by statistical techniques to assess the times of the thermal resistance of the QFN. The results of the Monte Carlo simulation (Tab.III) show that the thermal resistance is sensitive to the input variations. Indeed, in our case, the standard deviation is « 12% ». Table 3: Moments of the Thermal Resistance of QFN Average Standard Deviation  JAθ c°/w 47.35 5.75 VI. CONCLUSION In this work, we have adopted an approach allowing the thermal characterization of electronic packages through simulation taking into consideration the uncertainties. This approach consists of combining the finite element method with the Monte Carlo simulation. Stochastic characterization QFN revealed a significant dispersion of its thermal resistance. This information is crucial; it will allow for the development of more reliable electronic systems, since the consideration of the dispersions of the resistances in the design will define realistic junction temperatures that do not exceed their limits. REFERENCES [1]. S. ASSIF, M. AGOUZOUL, A. EL HAMI, O. BENDAOU and Y.GBATI. “Numerical model to simulate the drop test of printed circuit board (PCB)”. Advanced Materials Research, Vol.423, pp 26-30, Trans Tech Publications, Switzerland doi: 10.4028www.scientific.net/AMR.423.26. 2012. [2]. JEDEC Standard n° 51-2A, “Integrated Circuits Thermal Test Method Environmental Conditions - Natural Convection (Still Air)”, 2008. [3]. JEDEC Standard n° 51-7, “High Effective Thermal Conductivity Test Board for Leaded Surface Mount Packages”, 2005. [4]. O. Bendaou, J. E. Rojas, A. El Hami, A. Aannaque, M. Agouzoul, “Stochastic and reliability analysis of a propeller with model reduction”, European Journal of Computational Mechanics. Volume 18 – No. 2/2009. [5]. O. Bendaou, F. Bourzeix, B. Lakssir, A. El Hami, M. Agouzoul, L. El Bakkali, “BGA Warpage Investigations by Measurement and Stochastic FEA”, Congrès Marocain de Mécanique, Agadir, Avril 2013. [6]. J. Wilde, E. Zukowski, “Comparative Sensitivity Analysis for BGA and QFN Reliability” Thermal, Mechanical and Multi-Physics Simulation Experiments in Microelectronics and Micro-Systems, 2007. EuroSime 2007. International Conference. London, pp. 1-7, April 2007. [7]. X. He, ANSYS Tutorial, Department of Mechanical Engineering, University of Minnesota, Class material for short course for ANSYS (7.0) in Mechanical Engineering Department , October 2003.