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Okafor P.U et al. Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829

RESEARCH ARTICLE

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OPEN ACCESS

Investigation of Printing Performance of Solder Paste at Different
Temperatures
Okafor P.U and Eneh I.I
Department of Electrical/Electronic Engineering Enugu State University of Science and Technology Nigeria

Abstract
The properties of solder paste are immensely affected by temperature variations and humidity. Apparently,
temperature plays a vital role in achieving reliability in print performance and good quality. The printing
performance of the solder paste at different temperatures was investigated using two types of lead-free solder
paste. Three temperatures were investigated under three different time intervals. Issues to be considered are the
solder paste deposit defects associated with the pre-printing temperatures.
Keywords: Surface Mount Technology, Printed Circuit Board Assembly, Slump test, Reflow Soldering, Solder
Paste.

I.

Introduction

As the trend toward miniaturization and
compact product continues, the assembling process of
the electronic component or surface mount devices
(SMDs) becomes more complex and there is a need for
some form of automation (Lau et al. 1996). The
automated process of assembling the electronic
component or surface mount devices is known as
Surface Mount Technology (SMT) by means of using
solder paste as interconnecting material to provide
electrical, thermal and mechanical function (Huang et
al, 2002, and Nguty et al, 2001).
Majority of the components used on a printed
circuit board assembly (PCBA) are based on surface
mount technology (SMT) being assembled using
solder paste printing (SPP) and then fixed by the
reflow soldering (RS) process (Lau and Yeung 1996).
There are three major challenges in the fine pitch
stencil printing process. These challenges are the
solder paste formulation, the stencil manufacturing
process and the optimisation of the process parameters
in stencil printing Stencil printing account for a great
percentage of defects in surface mount technology. A
major course of these defects is the solder paste
behaviour during stencil printing, which is greatly
affected by temperature. As a result, it is necessary to
carry out an intensive study on the effects of
temperature on solder paste with respect to its printing
performance (Durairaj et al, 2002).

II.

Experimental design

2.1 Test materials
Two commercially available lead-free solder
pastes P1 (LF318) and P2 (LF328) prepared from
fluxes F1 and F2 were used. The solder particles for all
the paste samples are made of the same tin-silvercopper alloy with a melting point of 217˚C. Both P1
and P2 have a percentage metal loading of 88.5%. P1
is a Type 3 solder paste and P2 is Type 4. The flux
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medium makes up for 11.5% of the solder paste
weight. The flux medium contains a stable resin
system and slow evaporating solvents with minimal
odour. The formulation meets the requirements of the
Telcordia (formerly known as Bellcore) GR-78-CORE
and ANSI/J-STD-004 for a type ROL0 classification.
The two lead-free solder pastes LF318 and LF328 used
in this experiment were separated into nine different
jars respectively, making it eighteen jars in a whole.
Each jar contained one hundred grams of lead-free
solder paste. This separation was to allow for the
number of experiments that was carried out in the
study. For quick and easy identification, LF318 was
named P1 and LF328 was named P2. The temperatures
under investigation were 15˚C, 25˚C, and 35˚C. As
shown in table 1 below, two solder pastes P1 and P2
were stored at each of these temperatures for 24hours,
48hours, and 72hours respectively, making it nine
experiments for each solder paste.
Table 1: Storage parameters for P1 and P2 at the
thermal chamber.
Solder Temperature Storage
Storage
Storage
paste
(˚C)
time
time
time
(minutes) (minutes) (minutes)
P1
15(˚C)
1440
2880
4320
P2
15(˚C)
1440
2880
4320
P1
25(˚C)
1440
2880
4320
P2
25(˚C)
1440
2880
4320
P1
35(˚C)
1440
2880
4320
P2
35(˚C)
1440
2880
4320

III.

Process parameters

The printing parameters used for the
experiment are outlined in table 2. Previous work
reported by Marks et al (2007) was used as a
benchmark.

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Table 2: Printing parameters
Printing parameters
Printing/Squeegee speed
Squeegee
loading
(or
pressure)
Separation speed
Snap-off/Print gap

IV.

Values used
20mm/sec
8kg
100% (3mm/sec)
0.0mm
(On-contact
printing)

Experimental result

All the results recorded were put into the
Gauge calculator. The R&R% got was 19.43%. This is
well below 30% which is the acceptable standard. This
means that the measurement device is capable of the
task.
Plotting the average
In the formation of solder joints, print
thickness determines the volume of solder in the joint.
The thickness of the paste print is determined by the
thickness of the metal mask of the stencil. Though
stencil thickness controls the paste thickness, other
variables such as snap-off height and the condition of

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the printing equipment determine the print height. The
reflow solder height is not just a factor of solder paste
height only, but also the metal content of the paste.
Due to the fact that the print gap for the experiment is
0.0mm, the snap-off height becomes the thickness of
the stencil which is 125µm. Therefore at this stage, the
average of the average heights got from the regions in
the chosen locations on the stencil was computed.
In each of the two locations under
investigation, four regions were measured. In each
region, two deposits were measured. The averages of
the two deposits were taken. Subsequently, the
averages of the locations were then computed based on
the four regions. A sample of the 3-D image of the
measured heights is shown in figures 1 and 2. Figure 1
shows the height of P1 while figure 2 shows that of P2.
The blue base indicates the reference point, which is
surface of the substrate. The red colour indicates
maximum height. The results from the computed
averages are shown in Tables 3 and 4, while figures 3
and 4 shows the graphs of the computed average height
against the solder paste storage/aging time with respect
to the storage temperatures.

Figure 1: 3-D image of the solder paste deposit for location 1

Figure 2: 3-D image of the solder paste deposit for location 2
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Storage
temperature (˚C)
15
15
15
25
25
25
35
35
35

Table 3: Results for solder paste deposit heights for LF318.
LF318 = P1
Storage time
Target
Height for
Height for
(Hours)
height
Location 1
Location 2
(µm)
(µm)
(µm)
24
125
103.36
89.5
48
125
91.63
109.66
72
125
92.24
115.9
24
125
89.15
115.58
48
125
83.48
122.74
72
125
102.08
116.79
24
125
100.25
120.15
48
125
95.26
118.69
72
125
112.02
119.43

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Average
height (µm)
96.43
100.65
104.07
102.37
103.11
109.44
110.2
106.98
115.74

Figure 3: Temperature effect results for solder paste deposit height for LF318

Storage
temperature (˚C)
15
15
15
25
25
25
35
35
35

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Table 4: Results for solder paste deposit heights for LF328
LF328 = P2
Storage time
Target
Height for
Height for
(Hours)
height
Location 1
Location 2
(µm)
(µm)
(µm)
24
125
120.83
103.06
48
125
89.63
109.66
72
125
92.24
108.31
24
125
108.5
126.26
48
125
98.49
102.08
72
125
100.21
11538
24
125
99.63
114.48
48
125
110.15
133.9
72
125
117.14
129.48

Average
height (µm)
111.95
99.93
96.76
117.38
100.29
107.80
107.06
122.03
123.31

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Figure 4: Temperature effect results for solder paste deposit heights for LF328
During the printing process for LF318 aged at
15˚C for 24 hours, the solder paste just rolled
minimally. The temperature of the solder paste during
the printing was low, and that had a great effect on the
solder paste viscosity. The low temperature made the
solder paste viscosity to be too high. The temperature
was not conducive for the rheological properties of the
solder paste to be at its best. Therefore, the paste could
not role, giving rise to skipping and low aperture
filling which in effect caused ragged edges. This was
one of the contributing factors to the low height seen
after the printing. This is evident from the points of the
height for 15˚C in figure 1.

It can be observed that as the temperature increased,
the height against time also increased. This trend was
seen for both P 1 and P 2, except for P 2 stored at 35˚C
for 24 hours. Normally, it would be expected that
increase in temperature would give rise to decrease in
height, given that higher temperature would cause the
solder paste to slump. Rather than decrease the height
as the temperature increased, the height was
increasing. This is because at low temperature, the
paste’s viscosity increases causing the solder paste
flow to slow down or not to flow at all.

Figure 5 (a): Comparing solder paste deposit heights of P 1 and P 2 for 24 hours aging.

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Height (µm)

After 48 Hours aging
140
120
100
80
60
40
20
0

P1
P2

15

25

35
Temperature('C)

Figure 5 (b): Comparing solder paste deposit heights of P 1 and P 2 for 48 hours aging

Figure 5 (c): Comparing solder paste deposit heights of P 1 and P 2 for 72 hours aging
When the solder pastes were compared, it was
found as shown in figures 5 (a), (b), and (c) that the
height increases as the temperature increases. This
trend was seen as earlier discussed, for all the
experiments except for P2 aged/conditioned at 35˚C
for 24 hours. This shows that increase in height with
increase in temperature and or storage time is common
for both P1 and P2. Judging from common trend of
increased height with increased temperature, the
behaviour of P2 conditioned at 35˚C for 24 hours may
be a special cause of variation.
Considering the relationship between paste
heights, ability of the solder paste to roll during
printing, viscosity, temperature and time, the results
got in this experiment was compared with that got by
Nguty and Ekere (2000). It was shown that there was
an increase of 60% in paste viscosity for samples kept
at room temperature apparently, longer time and higher
temperature increases viscosity thereby increasing the
tendency of the solder paste to roll. However, the
temperature must not be excessive.
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V.

Variability analysis

5.1 Standard Deviation :
The
following
mathematical equation is used to calculate the standard
deviation.

[1]

[2]
Where σ is the standard deviation, µ is the mean
This means that the standard deviation σ is the
square root of the average value of (X − μ) 2. Therefore,
to calculate the standard deviation of the solder paste
heights, we compute the difference of each data point
from the mean, and then square the result.

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A normal standard deviation plot should look like

5.2 Mean-Square Deviation

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figure 6 below.

Figure 6: Normal standard deviation diagram.
Assuming y1, y2, y3,..........yn are n data points,
the MSD for it can be computed as

MSD = ∑(Yi ─ Y0)2 = (Y1 ─Y0)2 + (Y2 ─ Y0)2 + (Y3 ─ Y0)2 + K
[3]
n
n
quantity in all three quality characteristic, in case of
It can also be shown that
bigger quality characteristics, the inverse of the
MSD = σ2 + (Yavg ─ Y0)2
[4]
deviation squares are used as shown below. In this
Where, Y0 is the target value and σ is the standard
way, despite the quality characteristics of the original
deviation (population, using n as the divisor).
results, the desirability of MSD are always retained as
MSD can be seen as deviation with respect to
smaller is better.
the origin. For the fact that like other forms of
deviations, MSD is always preferred to be a smaller
Nominal: MSD = (Y1 ─ Y0)2 + (Y2 ─ Y0)2 + (Y3 ─ Y0)2 + (Yi ─ Y0)2
[5]
n
Smaller: MSD = Y12 + Y22 + Y32 + K
n

[6]

Bigger: MSD = 1∕Y12 + 1∕Y22 +1∕Y32 + K
n

[7]

5.3 Percentage Variation
Assuming that y1 and y2 is a pair of data, the
percentage variation between them will be expressed
by equation 4.8;
Percentage variation = y1 - y2
y1

× 100%

[8]

For the purpose of this project analysis,
standard deviation and percentage variation were used
to ascertain the level of variability at different levels of
performance. While standard deviation was used to
study the variation at the location level, a more indepth study of variation was conducted at the region
level using percentage variation.
5.4 Applying standard deviation
By applying equation 2 to the results,

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The results for 15˚C at 24 hours, we have that;
µ = 89.85 + 106 + 113.3 + 104.3 = 103.36
4
µ = 103.36
(89.85 – 103.36)2 = (-13.51)2 = 182.52
(106 – 103.36)2 = (2.64)2 = 6.97
(113.3 – 103.36)2 = (9.94)2 = 98.80
(104.3 – 103.36)2 = (0.94)2 = 0.88
σ2 = √ (-13.5)2 + (2.64)2 + (9.94)2 + (0.94)2
4
Therefore, σ =
4
σ = √72.29 = 8.5
This means that for the lead-free solder paste
aged prior to printing at 15˚C for 24 hours, the
standard deviation (σ), of the printed deposits for
location 1 is equal to 8.5. The same process was used
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to compute the standard deviation of all the locations
are shown in table 5.
measured for both P 1 and P 2. The computed results
Table 5: Result of standard deviation for LF318 (P 1) and LF328 (P 2).
Temperature (˚C) Time
Standard deviation (P 1)
Standard deviation (P 2)
(Hours)
Location 1
15
15
15
25
25
25
35
35
35

24
48
72
24
48
72
24
48
72

Location 2

Location 1

8.5
4.0
12.2
10.4
7.6
12.3
8.7
8.6
13.4

9.9
5.2
3.7
8.1
6.1
3.7
8.6
1.9
1.2

8.9
9.2
9
5.3
6.6
7.4
13.1
8.8
12.6

From table 5, it can be seen that the lowest
standard deviation is at (P 1), location 2 of the paste
aged at 35˚C for 72 hours. This means that the solder
paste deposits tend to be very close to the mean. In
other words, the printing was able to produce a normal
distribution at this location, which means that most of
the apertures in that particular location had deposits
that are close to its average.
Generally, location 2 seems to have a normal
distribution than location 1. This is most likely because
the aperture sizes at location 2 are larger than that of

Location
Loc 1

Loc2

Loc 1

Loc 2

Loc 1

Loc 2

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Location
2
7.6
6.1
3.8
5
8.6
6.9
2.9
6
1.8

location 1, therefore enabling the squeegee to deposit
more solder paste at a balanced level.
5.5 Applying Percentage variation
For P1 location 1, region 1, the percentage
variation was calculated as
% variation = 93.2 – 86.5 × 100 = 7.2%
93.2
The same procedure was used to calculate for
all the regions measured.

Table 6: Percentage variation result of deposited solder paste height for LF318.
Region
Time (Hours)
Percentage variation (%) for P1
1
2
3
4
5
6
7
8
1
2
3
4
5
6
7
8
1
2
3
4
5
6
7
8

24
24
24
24
24
24
24
24
48
48
48
48
48
48
48
48
72
72
72
72
72
72
72
72

15˚C
7.2
- 10.7
8.6
16.2
3.4
9.5
2.6
4.3
8.9
3.3
7.5
1.2
1.2
13.8
16.7
8.3
5.3
24.2
14.8
- 3.3
3.6
15.0
4.5
20.5

25˚C
- 0.8
1.2
18.0
- 11
4.0
7.9
- 5.2
5.7
5.2
8.8
1.1
3.7
- 2.2
8.9
- 2.5
13.6
- 0.1
6.6
1.7
7.1
17.3
18.0
7.4
7.8

35˚C
5.2
10.4
1.6
4.1
17.0
5.9
11.0
19.3
- 0.6
4.6
- 2.2
4.5
20.0
- 4.2
14.1
11.1
0.1
4.9
2.0
8.9
6.9
3.1
11.3
13.6
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Table 7: Percentage variation result of deposited solder paste height for LF328
Location
Region
Time
Percentage variation (%) for P2
(Hours)
15˚C
25˚C
35˚C
Loc 1
1
24
18
10.5
0.2
2
24
5.1
3.9
- 5.0
3
24
13.3
- 4.9
8.8
4
24
4.8
- 3.3
27.8
Loc 2
5
24
4.6
6.7
8.2
6
24
0.4
19
10.3
7
24
- 6.9
5.1
19.7
8
24
3.3
9.1
14.4
Loc 1
1
48
5.1
0
7.6
2
48
4.4
- 4.8
10.6
3
48
9.5
5.3
4.9
4
48
29.4
1.9
4.3
Loc 2
5
48
10.6
8.1
18.9
6
48
8.7
2.0
9.5
7
48
- 5.8
2.2
3.6
8
48
0.7
14.2
9.1
Loc 1
1
72
3.6
0.5
12.3
2
72
7.6
11
6.1
3
72
3.4
1.3
- 6.8
4
72
3.3
3.9
13.3
Loc 2
5
72
5
10.6
- 14.4
6
72
13.4
16
- 6.7
7
72
4.7
11.5
- 4.0
8
72
16.5
3.9
3.7
According to Prasad (1997), the maximum
allowable variation in paste height should be about

20%. Figures 7 (a –f) shows the graph of the
percentage variation.

% variation

P 1 at 24 hours
25
20
15
10
5
0
-5
-10
-15

15˚
C
25˚
C

35˚
C

1

2

3

4

5

6

7

8

Regions

Figure 7(a): Percentage variation plot for P1 at 24 hours

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% variation

P 1 at 48 hours
25
20
15

15˚
C

10
5
0
-5
-10

25˚
C
35˚
C

1

2

3

4

5

6

7

8

Regions

Figure 7(b): Percentage variation plot for P1 at 48 hours

% variation

P 1 at 72 hours

30
25
20
15
10
5
0
-5

15˚
C
25˚
C
35˚
C

1

2

3

4

5

6

7

8

Regions

Figure 7(c): Percentage variation plot for P1 at 72 hours

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P 2 at 24 hours

% variation

30
25

20
15

15˚
C

10

25˚
C

5

35˚
C

0
-5

1

2

3

4

5

6

7

8

-10
Regions

Figure 7(d): Percentage variation plot for P2 at 24 hours

Figure 7(e): Percentage variation plot for P2 at 48 hours

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Figure 7(f): Percentage variation plot for P2 at 72 hours
Since 20% is the maximum allowable
percentage variation, upper control limit (UCL) and
lower control limit (LCL) was set at 20% and -20%
respectively for this experiment. Therefore, these
control limits was used to check for out of control
conditions in the printing process. For the whole
process/experiment, only four out of control conditions
(freak) were found at the region which is an
infinitesimal part of the deposits.

VI.

Slump Test Results

Lee (2002) stated that slump is a phenomenon
where the paste viscosity is not high enough to resist
the collapsing force exerted by gravity, and
consequently results in spreading beyond the area to be
deposited. Cold slump was used to determine the
solder paste behaviour. Cold slump refers to the
slumping behaviour at room temperature while hot
slump refers to slumping during reflow. Figure 8
shows the slump location that was visually observed
using a Leica S6D zoom stereomicroscope. From the
observations, paste stored at 35˚C had the highest level
of slumping.

Figure 8: Four edges of the slump location for P1

VII.

Conclusion

From the measured heights of the solder paste
deposit, the paste stored at 35˚C for 72 hours, produced
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the height closest to the target. However, it was found
that a lot of slumping occurred, making it
unfavourable. Though more slumping occurred for the
paste stored at 35˚C, it was not enough to get the
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height lower than that stored at 25˚C or 15˚C. Because
of slumping behaviour of solder paste, it was believed
that the height of the solder paste would decrease as
the temperature increased. This was not exactly the
case, the height rather increased slightly as the
temperature increased.
This behaviour was as a result of some
factors. First, paste was not able to role at low
temperatures such 15˚C. Secondly, as the temperature
increased, the paste rolled and was able to fill the
apertures effectively. Therefore, considering this
slumping phenomenon, the paste stored at 25˚C for 48
hours produced the best results of good height with
minimal slumping. Analysis shows that variability of
the paste distribution was lowest and more uniform for
paste stored at 25˚C for 48 hours. The percentage
variation showed zero variation in one of the regions
for P2. With the results of the variability analysis, 25˚C
showed less variability. From the analysis, it is obvious
that temperature has tremendous effects on the printing
performance of solder paste. This study recommends
25˚C as a good temperature for solder paste printing.

[8]

[9]

[10]

[11]

[12]

References
[1]

[2]

[3]

[4]

[5]

[6]

[7]

Clements, D., Desmulliez, M. P. Y. and
Abraham, E (2007), “The evolution of paste
pressure during stencil printing”, Soldering
and Surface Mount Technology, 19, 3, pp. 9 14.
Colin C. Johnson and Joseph Kevra (1989).
Solder paste technology: principles and
applications. Edition: Illustrated. Publisher
TAB Professional and Reference Books.
Durairaj, R, Ekere, N. N. and Salam, B.
(2004), “Thixotropy flow behaviour of solder
and conductive adhesive pastes”, Journal of
materials science: materials in electronics, 15,
677 – 683.
Durairaj, R, Nguty, T. A. and Ekere, N. N.
(2001), “Critical Factors Affecting Paste Flow
During Stencil Printing of Solder Paste”,
Soldering and Surface Mount Technology, 13,
2, pp 30 – 34..
John H. Lau, C. P Wong, Ning-Cheng Lee, S.
W
Ricky
Lee
(2002).
Electronics
manufacturing: with lead-free, halogen-free,
and conductive-adhesive materials. Edition:
illustrated. Published by McGraw-Hill
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ISBN:
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829 | P a g e

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  • 1. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 RESEARCH ARTICLE www.ijera.com OPEN ACCESS Investigation of Printing Performance of Solder Paste at Different Temperatures Okafor P.U and Eneh I.I Department of Electrical/Electronic Engineering Enugu State University of Science and Technology Nigeria Abstract The properties of solder paste are immensely affected by temperature variations and humidity. Apparently, temperature plays a vital role in achieving reliability in print performance and good quality. The printing performance of the solder paste at different temperatures was investigated using two types of lead-free solder paste. Three temperatures were investigated under three different time intervals. Issues to be considered are the solder paste deposit defects associated with the pre-printing temperatures. Keywords: Surface Mount Technology, Printed Circuit Board Assembly, Slump test, Reflow Soldering, Solder Paste. I. Introduction As the trend toward miniaturization and compact product continues, the assembling process of the electronic component or surface mount devices (SMDs) becomes more complex and there is a need for some form of automation (Lau et al. 1996). The automated process of assembling the electronic component or surface mount devices is known as Surface Mount Technology (SMT) by means of using solder paste as interconnecting material to provide electrical, thermal and mechanical function (Huang et al, 2002, and Nguty et al, 2001). Majority of the components used on a printed circuit board assembly (PCBA) are based on surface mount technology (SMT) being assembled using solder paste printing (SPP) and then fixed by the reflow soldering (RS) process (Lau and Yeung 1996). There are three major challenges in the fine pitch stencil printing process. These challenges are the solder paste formulation, the stencil manufacturing process and the optimisation of the process parameters in stencil printing Stencil printing account for a great percentage of defects in surface mount technology. A major course of these defects is the solder paste behaviour during stencil printing, which is greatly affected by temperature. As a result, it is necessary to carry out an intensive study on the effects of temperature on solder paste with respect to its printing performance (Durairaj et al, 2002). II. Experimental design 2.1 Test materials Two commercially available lead-free solder pastes P1 (LF318) and P2 (LF328) prepared from fluxes F1 and F2 were used. The solder particles for all the paste samples are made of the same tin-silvercopper alloy with a melting point of 217˚C. Both P1 and P2 have a percentage metal loading of 88.5%. P1 is a Type 3 solder paste and P2 is Type 4. The flux www.ijera.com medium makes up for 11.5% of the solder paste weight. The flux medium contains a stable resin system and slow evaporating solvents with minimal odour. The formulation meets the requirements of the Telcordia (formerly known as Bellcore) GR-78-CORE and ANSI/J-STD-004 for a type ROL0 classification. The two lead-free solder pastes LF318 and LF328 used in this experiment were separated into nine different jars respectively, making it eighteen jars in a whole. Each jar contained one hundred grams of lead-free solder paste. This separation was to allow for the number of experiments that was carried out in the study. For quick and easy identification, LF318 was named P1 and LF328 was named P2. The temperatures under investigation were 15˚C, 25˚C, and 35˚C. As shown in table 1 below, two solder pastes P1 and P2 were stored at each of these temperatures for 24hours, 48hours, and 72hours respectively, making it nine experiments for each solder paste. Table 1: Storage parameters for P1 and P2 at the thermal chamber. Solder Temperature Storage Storage Storage paste (˚C) time time time (minutes) (minutes) (minutes) P1 15(˚C) 1440 2880 4320 P2 15(˚C) 1440 2880 4320 P1 25(˚C) 1440 2880 4320 P2 25(˚C) 1440 2880 4320 P1 35(˚C) 1440 2880 4320 P2 35(˚C) 1440 2880 4320 III. Process parameters The printing parameters used for the experiment are outlined in table 2. Previous work reported by Marks et al (2007) was used as a benchmark. 818 | P a g e
  • 2. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 Table 2: Printing parameters Printing parameters Printing/Squeegee speed Squeegee loading (or pressure) Separation speed Snap-off/Print gap IV. Values used 20mm/sec 8kg 100% (3mm/sec) 0.0mm (On-contact printing) Experimental result All the results recorded were put into the Gauge calculator. The R&R% got was 19.43%. This is well below 30% which is the acceptable standard. This means that the measurement device is capable of the task. Plotting the average In the formation of solder joints, print thickness determines the volume of solder in the joint. The thickness of the paste print is determined by the thickness of the metal mask of the stencil. Though stencil thickness controls the paste thickness, other variables such as snap-off height and the condition of www.ijera.com the printing equipment determine the print height. The reflow solder height is not just a factor of solder paste height only, but also the metal content of the paste. Due to the fact that the print gap for the experiment is 0.0mm, the snap-off height becomes the thickness of the stencil which is 125µm. Therefore at this stage, the average of the average heights got from the regions in the chosen locations on the stencil was computed. In each of the two locations under investigation, four regions were measured. In each region, two deposits were measured. The averages of the two deposits were taken. Subsequently, the averages of the locations were then computed based on the four regions. A sample of the 3-D image of the measured heights is shown in figures 1 and 2. Figure 1 shows the height of P1 while figure 2 shows that of P2. The blue base indicates the reference point, which is surface of the substrate. The red colour indicates maximum height. The results from the computed averages are shown in Tables 3 and 4, while figures 3 and 4 shows the graphs of the computed average height against the solder paste storage/aging time with respect to the storage temperatures. Figure 1: 3-D image of the solder paste deposit for location 1 Figure 2: 3-D image of the solder paste deposit for location 2 www.ijera.com 819 | P a g e
  • 3. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 Storage temperature (˚C) 15 15 15 25 25 25 35 35 35 Table 3: Results for solder paste deposit heights for LF318. LF318 = P1 Storage time Target Height for Height for (Hours) height Location 1 Location 2 (µm) (µm) (µm) 24 125 103.36 89.5 48 125 91.63 109.66 72 125 92.24 115.9 24 125 89.15 115.58 48 125 83.48 122.74 72 125 102.08 116.79 24 125 100.25 120.15 48 125 95.26 118.69 72 125 112.02 119.43 www.ijera.com Average height (µm) 96.43 100.65 104.07 102.37 103.11 109.44 110.2 106.98 115.74 Figure 3: Temperature effect results for solder paste deposit height for LF318 Storage temperature (˚C) 15 15 15 25 25 25 35 35 35 www.ijera.com Table 4: Results for solder paste deposit heights for LF328 LF328 = P2 Storage time Target Height for Height for (Hours) height Location 1 Location 2 (µm) (µm) (µm) 24 125 120.83 103.06 48 125 89.63 109.66 72 125 92.24 108.31 24 125 108.5 126.26 48 125 98.49 102.08 72 125 100.21 11538 24 125 99.63 114.48 48 125 110.15 133.9 72 125 117.14 129.48 Average height (µm) 111.95 99.93 96.76 117.38 100.29 107.80 107.06 122.03 123.31 820 | P a g e
  • 4. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 www.ijera.com Figure 4: Temperature effect results for solder paste deposit heights for LF328 During the printing process for LF318 aged at 15˚C for 24 hours, the solder paste just rolled minimally. The temperature of the solder paste during the printing was low, and that had a great effect on the solder paste viscosity. The low temperature made the solder paste viscosity to be too high. The temperature was not conducive for the rheological properties of the solder paste to be at its best. Therefore, the paste could not role, giving rise to skipping and low aperture filling which in effect caused ragged edges. This was one of the contributing factors to the low height seen after the printing. This is evident from the points of the height for 15˚C in figure 1. It can be observed that as the temperature increased, the height against time also increased. This trend was seen for both P 1 and P 2, except for P 2 stored at 35˚C for 24 hours. Normally, it would be expected that increase in temperature would give rise to decrease in height, given that higher temperature would cause the solder paste to slump. Rather than decrease the height as the temperature increased, the height was increasing. This is because at low temperature, the paste’s viscosity increases causing the solder paste flow to slow down or not to flow at all. Figure 5 (a): Comparing solder paste deposit heights of P 1 and P 2 for 24 hours aging. www.ijera.com 821 | P a g e
  • 5. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 www.ijera.com Height (µm) After 48 Hours aging 140 120 100 80 60 40 20 0 P1 P2 15 25 35 Temperature('C) Figure 5 (b): Comparing solder paste deposit heights of P 1 and P 2 for 48 hours aging Figure 5 (c): Comparing solder paste deposit heights of P 1 and P 2 for 72 hours aging When the solder pastes were compared, it was found as shown in figures 5 (a), (b), and (c) that the height increases as the temperature increases. This trend was seen as earlier discussed, for all the experiments except for P2 aged/conditioned at 35˚C for 24 hours. This shows that increase in height with increase in temperature and or storage time is common for both P1 and P2. Judging from common trend of increased height with increased temperature, the behaviour of P2 conditioned at 35˚C for 24 hours may be a special cause of variation. Considering the relationship between paste heights, ability of the solder paste to roll during printing, viscosity, temperature and time, the results got in this experiment was compared with that got by Nguty and Ekere (2000). It was shown that there was an increase of 60% in paste viscosity for samples kept at room temperature apparently, longer time and higher temperature increases viscosity thereby increasing the tendency of the solder paste to roll. However, the temperature must not be excessive. www.ijera.com V. Variability analysis 5.1 Standard Deviation : The following mathematical equation is used to calculate the standard deviation. [1] [2] Where σ is the standard deviation, µ is the mean This means that the standard deviation σ is the square root of the average value of (X − μ) 2. Therefore, to calculate the standard deviation of the solder paste heights, we compute the difference of each data point from the mean, and then square the result. 822 | P a g e
  • 6. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 A normal standard deviation plot should look like 5.2 Mean-Square Deviation www.ijera.com figure 6 below. Figure 6: Normal standard deviation diagram. Assuming y1, y2, y3,..........yn are n data points, the MSD for it can be computed as MSD = ∑(Yi ─ Y0)2 = (Y1 ─Y0)2 + (Y2 ─ Y0)2 + (Y3 ─ Y0)2 + K [3] n n quantity in all three quality characteristic, in case of It can also be shown that bigger quality characteristics, the inverse of the MSD = σ2 + (Yavg ─ Y0)2 [4] deviation squares are used as shown below. In this Where, Y0 is the target value and σ is the standard way, despite the quality characteristics of the original deviation (population, using n as the divisor). results, the desirability of MSD are always retained as MSD can be seen as deviation with respect to smaller is better. the origin. For the fact that like other forms of deviations, MSD is always preferred to be a smaller Nominal: MSD = (Y1 ─ Y0)2 + (Y2 ─ Y0)2 + (Y3 ─ Y0)2 + (Yi ─ Y0)2 [5] n Smaller: MSD = Y12 + Y22 + Y32 + K n [6] Bigger: MSD = 1∕Y12 + 1∕Y22 +1∕Y32 + K n [7] 5.3 Percentage Variation Assuming that y1 and y2 is a pair of data, the percentage variation between them will be expressed by equation 4.8; Percentage variation = y1 - y2 y1 × 100% [8] For the purpose of this project analysis, standard deviation and percentage variation were used to ascertain the level of variability at different levels of performance. While standard deviation was used to study the variation at the location level, a more indepth study of variation was conducted at the region level using percentage variation. 5.4 Applying standard deviation By applying equation 2 to the results, www.ijera.com The results for 15˚C at 24 hours, we have that; µ = 89.85 + 106 + 113.3 + 104.3 = 103.36 4 µ = 103.36 (89.85 – 103.36)2 = (-13.51)2 = 182.52 (106 – 103.36)2 = (2.64)2 = 6.97 (113.3 – 103.36)2 = (9.94)2 = 98.80 (104.3 – 103.36)2 = (0.94)2 = 0.88 σ2 = √ (-13.5)2 + (2.64)2 + (9.94)2 + (0.94)2 4 Therefore, σ = 4 σ = √72.29 = 8.5 This means that for the lead-free solder paste aged prior to printing at 15˚C for 24 hours, the standard deviation (σ), of the printed deposits for location 1 is equal to 8.5. The same process was used 823 | P a g e
  • 7. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 www.ijera.com to compute the standard deviation of all the locations are shown in table 5. measured for both P 1 and P 2. The computed results Table 5: Result of standard deviation for LF318 (P 1) and LF328 (P 2). Temperature (˚C) Time Standard deviation (P 1) Standard deviation (P 2) (Hours) Location 1 15 15 15 25 25 25 35 35 35 24 48 72 24 48 72 24 48 72 Location 2 Location 1 8.5 4.0 12.2 10.4 7.6 12.3 8.7 8.6 13.4 9.9 5.2 3.7 8.1 6.1 3.7 8.6 1.9 1.2 8.9 9.2 9 5.3 6.6 7.4 13.1 8.8 12.6 From table 5, it can be seen that the lowest standard deviation is at (P 1), location 2 of the paste aged at 35˚C for 72 hours. This means that the solder paste deposits tend to be very close to the mean. In other words, the printing was able to produce a normal distribution at this location, which means that most of the apertures in that particular location had deposits that are close to its average. Generally, location 2 seems to have a normal distribution than location 1. This is most likely because the aperture sizes at location 2 are larger than that of Location Loc 1 Loc2 Loc 1 Loc 2 Loc 1 Loc 2 www.ijera.com Location 2 7.6 6.1 3.8 5 8.6 6.9 2.9 6 1.8 location 1, therefore enabling the squeegee to deposit more solder paste at a balanced level. 5.5 Applying Percentage variation For P1 location 1, region 1, the percentage variation was calculated as % variation = 93.2 – 86.5 × 100 = 7.2% 93.2 The same procedure was used to calculate for all the regions measured. Table 6: Percentage variation result of deposited solder paste height for LF318. Region Time (Hours) Percentage variation (%) for P1 1 2 3 4 5 6 7 8 1 2 3 4 5 6 7 8 1 2 3 4 5 6 7 8 24 24 24 24 24 24 24 24 48 48 48 48 48 48 48 48 72 72 72 72 72 72 72 72 15˚C 7.2 - 10.7 8.6 16.2 3.4 9.5 2.6 4.3 8.9 3.3 7.5 1.2 1.2 13.8 16.7 8.3 5.3 24.2 14.8 - 3.3 3.6 15.0 4.5 20.5 25˚C - 0.8 1.2 18.0 - 11 4.0 7.9 - 5.2 5.7 5.2 8.8 1.1 3.7 - 2.2 8.9 - 2.5 13.6 - 0.1 6.6 1.7 7.1 17.3 18.0 7.4 7.8 35˚C 5.2 10.4 1.6 4.1 17.0 5.9 11.0 19.3 - 0.6 4.6 - 2.2 4.5 20.0 - 4.2 14.1 11.1 0.1 4.9 2.0 8.9 6.9 3.1 11.3 13.6 824 | P a g e
  • 8. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 www.ijera.com Table 7: Percentage variation result of deposited solder paste height for LF328 Location Region Time Percentage variation (%) for P2 (Hours) 15˚C 25˚C 35˚C Loc 1 1 24 18 10.5 0.2 2 24 5.1 3.9 - 5.0 3 24 13.3 - 4.9 8.8 4 24 4.8 - 3.3 27.8 Loc 2 5 24 4.6 6.7 8.2 6 24 0.4 19 10.3 7 24 - 6.9 5.1 19.7 8 24 3.3 9.1 14.4 Loc 1 1 48 5.1 0 7.6 2 48 4.4 - 4.8 10.6 3 48 9.5 5.3 4.9 4 48 29.4 1.9 4.3 Loc 2 5 48 10.6 8.1 18.9 6 48 8.7 2.0 9.5 7 48 - 5.8 2.2 3.6 8 48 0.7 14.2 9.1 Loc 1 1 72 3.6 0.5 12.3 2 72 7.6 11 6.1 3 72 3.4 1.3 - 6.8 4 72 3.3 3.9 13.3 Loc 2 5 72 5 10.6 - 14.4 6 72 13.4 16 - 6.7 7 72 4.7 11.5 - 4.0 8 72 16.5 3.9 3.7 According to Prasad (1997), the maximum allowable variation in paste height should be about 20%. Figures 7 (a –f) shows the graph of the percentage variation. % variation P 1 at 24 hours 25 20 15 10 5 0 -5 -10 -15 15˚ C 25˚ C 35˚ C 1 2 3 4 5 6 7 8 Regions Figure 7(a): Percentage variation plot for P1 at 24 hours www.ijera.com 825 | P a g e
  • 9. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 www.ijera.com % variation P 1 at 48 hours 25 20 15 15˚ C 10 5 0 -5 -10 25˚ C 35˚ C 1 2 3 4 5 6 7 8 Regions Figure 7(b): Percentage variation plot for P1 at 48 hours % variation P 1 at 72 hours 30 25 20 15 10 5 0 -5 15˚ C 25˚ C 35˚ C 1 2 3 4 5 6 7 8 Regions Figure 7(c): Percentage variation plot for P1 at 72 hours www.ijera.com 826 | P a g e
  • 10. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 www.ijera.com P 2 at 24 hours % variation 30 25 20 15 15˚ C 10 25˚ C 5 35˚ C 0 -5 1 2 3 4 5 6 7 8 -10 Regions Figure 7(d): Percentage variation plot for P2 at 24 hours Figure 7(e): Percentage variation plot for P2 at 48 hours www.ijera.com 827 | P a g e
  • 11. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 www.ijera.com Figure 7(f): Percentage variation plot for P2 at 72 hours Since 20% is the maximum allowable percentage variation, upper control limit (UCL) and lower control limit (LCL) was set at 20% and -20% respectively for this experiment. Therefore, these control limits was used to check for out of control conditions in the printing process. For the whole process/experiment, only four out of control conditions (freak) were found at the region which is an infinitesimal part of the deposits. VI. Slump Test Results Lee (2002) stated that slump is a phenomenon where the paste viscosity is not high enough to resist the collapsing force exerted by gravity, and consequently results in spreading beyond the area to be deposited. Cold slump was used to determine the solder paste behaviour. Cold slump refers to the slumping behaviour at room temperature while hot slump refers to slumping during reflow. Figure 8 shows the slump location that was visually observed using a Leica S6D zoom stereomicroscope. From the observations, paste stored at 35˚C had the highest level of slumping. Figure 8: Four edges of the slump location for P1 VII. Conclusion From the measured heights of the solder paste deposit, the paste stored at 35˚C for 72 hours, produced www.ijera.com the height closest to the target. However, it was found that a lot of slumping occurred, making it unfavourable. Though more slumping occurred for the paste stored at 35˚C, it was not enough to get the 828 | P a g e
  • 12. Okafor P.U et al. Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.818-829 height lower than that stored at 25˚C or 15˚C. Because of slumping behaviour of solder paste, it was believed that the height of the solder paste would decrease as the temperature increased. This was not exactly the case, the height rather increased slightly as the temperature increased. This behaviour was as a result of some factors. First, paste was not able to role at low temperatures such 15˚C. Secondly, as the temperature increased, the paste rolled and was able to fill the apertures effectively. Therefore, considering this slumping phenomenon, the paste stored at 25˚C for 48 hours produced the best results of good height with minimal slumping. Analysis shows that variability of the paste distribution was lowest and more uniform for paste stored at 25˚C for 48 hours. The percentage variation showed zero variation in one of the regions for P2. With the results of the variability analysis, 25˚C showed less variability. From the analysis, it is obvious that temperature has tremendous effects on the printing performance of solder paste. This study recommends 25˚C as a good temperature for solder paste printing. [8] [9] [10] [11] [12] References [1] [2] [3] [4] [5] [6] [7] Clements, D., Desmulliez, M. P. Y. and Abraham, E (2007), “The evolution of paste pressure during stencil printing”, Soldering and Surface Mount Technology, 19, 3, pp. 9 14. Colin C. Johnson and Joseph Kevra (1989). Solder paste technology: principles and applications. Edition: Illustrated. Publisher TAB Professional and Reference Books. Durairaj, R, Ekere, N. N. and Salam, B. (2004), “Thixotropy flow behaviour of solder and conductive adhesive pastes”, Journal of materials science: materials in electronics, 15, 677 – 683. Durairaj, R, Nguty, T. A. and Ekere, N. N. (2001), “Critical Factors Affecting Paste Flow During Stencil Printing of Solder Paste”, Soldering and Surface Mount Technology, 13, 2, pp 30 – 34.. John H. Lau, C. P Wong, Ning-Cheng Lee, S. W Ricky Lee (2002). Electronics manufacturing: with lead-free, halogen-free, and conductive-adhesive materials. Edition: illustrated. Published by McGraw-Hill Professional. ISBN: 0071386246, 9780071386241 Lau, F. K. H. and Yeung, V. W. S., (1997), “A hierarchical evaluation of the solder paste printing process”, Journal of Materials Processing Technology, Vol. 69 pp. 79-89 Lee, N. C. (2002), “Reflow Soldering Processes: SMT, BGA, CSP and Flip-Chip Technologies”, Newnes Publication, USA, pp. 41 – 44, 101 – 103. Available at: http://books.google.co.uk/books?id=Tv_AuIP rZmEC (accessed 17 March 2008). www.ijera.com [13] [14] [15] [16] [17] www.ijera.com Leo P. Lambert (1988). Soldering for Electronic Assemblies. Edition: Illustrated. Published by Marcel Dekker. ISBN: 082477681X, 9780824776817 Marks, A., Mallik, S., Durairaj, R. and Ekere, N. N. (2007), ‘Effect of Abandon Time on Print Quality and Rheological Characteristics for Lead-Free Solder Pastes used for FlipChip Assembly’, 32nd International Electronics Manufacturing Technology Symposium (IEMT 2007) October 3-5 2007, San Jose/Silicon Valley, California, USA N. N Ekere and S. Mallik. (2008). A methodology for Characterising New LeadFree Solder Paste Formulations used for Flipchip Assembly Applications. Smart Processing Technology. 2 (1), 59-64. Nguty, T. A. and Ekere, N. N. (2000), “The rheological properties of solder and solar pastes and the effect on stencil printing”. Rheologica Acta, 39, 607 – 612. Puttlitz, K. L. and Stalter, K. A. (2004), “Handbook of Lead-free Solder Technology for Microelectronic Assemblies”, Marcel Dekker, New York, p 503, Available at: http://books.google.co.uk/books?id=H75Tyw RXUK4C (accessed 09 August 2009). R. Durairaj, S. Mallik and N. N. |Ekere. (2008). Solder paste characterisation: towards. Soldering & Surface mount technology. 20 (3), 34-40. Emeral Group Pulishing limited. ISSN: 0954-0911 R. Durairaj, S. Mallik, A. Marks, M. Winter, R. Bauer and N.N. Ekere: Rheological Characterisation of New Lead-Free Solder Paste Formulations for Flip-Chip Assembly. 2006. Electronics Manufacturing Engineering Research Group Medway School of Engineering, University of Greenwich Chatham Maritime R. Durairaj, S. Ramesh, S. Mallik, A. Seman, N. N. Ekere. (2009). Rheological characterisation and printing performance of Sn/Ag/Cu solder pastes. Material and Design. 30 (3), 3812-3818. S. Mallik, N. N. Ekere, R. Durairaj, and A. E. Marks (2008). An investigation into the rheological properties of different lead-free solder paste for surface mount application. Soldering & Surface mount technology. 3-10. Emerald Group publishing limited. ISSN: 0954-0911 T.A Nguty and N. N Ekere. (2000). Modelling the effects of temperature on the rheology of solder paste and flux system. Journal of material science: materials in Electronics. 11 (1), 39-43. 829 | P a g e