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Device for Measuring Sliding Friction on Highloft Nonwovens

Device for Measuring Sliding Friction on Highloft Nonwovens

Device for Measuring Sliding Friction on Highloft Nonwovens

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smooth polyester transparency film to 0.50 <str<strong>on</strong>g>for</str<strong>on</strong>g> a<br />

rubber mouse pad. Note that both sleds provide<br />

nearly identical fricti<strong>on</strong> coefficients <str<strong>on</strong>g>for</str<strong>on</strong>g> any <strong>on</strong>e<br />

material. The difference between the fricti<strong>on</strong><br />

coefficients determined by the two sleds <str<strong>on</strong>g>for</str<strong>on</strong>g> a single<br />

substrate is not c<strong>on</strong>sidered significant. The substrates<br />

were chosen so that they would not de<str<strong>on</strong>g>for</str<strong>on</strong>g>m<br />

significantly during this test. Thus both sleds measure<br />

the same fricti<strong>on</strong> coefficient when the sample does<br />

not de<str<strong>on</strong>g>for</str<strong>on</strong>g>m readily under the test.<br />

Figure 4 shows the measured fricti<strong>on</strong> coefficient <str<strong>on</strong>g>for</str<strong>on</strong>g><br />

<strong>on</strong>e to four batts of PET where the sled always slides<br />

<strong>on</strong> the same batt. Since the normal load is c<strong>on</strong>stant,<br />

the test speed is c<strong>on</strong>stant, the laboratory temperature<br />

and humidity are c<strong>on</strong>stant, and the two surfaces<br />

sliding against each other are identical, <strong>on</strong>e should<br />

expect the fricti<strong>on</strong> coefficient to be identical. Indeed,<br />

the fricti<strong>on</strong> coefficient measured using the guarded<br />

sled is c<strong>on</strong>stant, regardless of the number of batts.<br />

However, the fricti<strong>on</strong> coefficients measured using the<br />

c<strong>on</strong>venti<strong>on</strong>al sled increase with an increasing number<br />

of batts. Careful observati<strong>on</strong> of the test shows that,<br />

as more batts are added, the sled nestled deeper and<br />

deeper into the batts. When the sled was pulled<br />

across the batts, it de<str<strong>on</strong>g>for</str<strong>on</strong>g>med the batts and the <str<strong>on</strong>g>for</str<strong>on</strong>g>ce<br />

required to compress the batts added to the fricti<strong>on</strong>al<br />

<str<strong>on</strong>g>for</str<strong>on</strong>g>ce due to sliding of the sled across the surface. On<br />

the other hand, the guarded sled slid <strong>on</strong>ly <strong>on</strong> the<br />

already de<str<strong>on</strong>g>for</str<strong>on</strong>g>med batt. Thus, the outer, c<strong>on</strong>venti<strong>on</strong>al<br />

sled de<str<strong>on</strong>g>for</str<strong>on</strong>g>med the substrate during sliding, and<br />

measured the combined <str<strong>on</strong>g>for</str<strong>on</strong>g>ces of sliding across and<br />

de<str<strong>on</strong>g>for</str<strong>on</strong>g>ming the sample, while the inner, guarded sled<br />

<strong>on</strong>ly slid <strong>on</strong> the already de<str<strong>on</strong>g>for</str<strong>on</strong>g>med sample.<br />

μ<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0 1 2 3 4 5<br />

Number of Batts<br />

FIGURE 4. <str<strong>on</strong>g>Fricti<strong>on</strong></str<strong>on</strong>g> coefficients of 1-4 polyester batts. The same<br />

batt is always in c<strong>on</strong>tact with the sled. Circles are fricti<strong>on</strong><br />

coefficients obtained from the guarded sled while the squares are<br />

from the c<strong>on</strong>venti<strong>on</strong>al sled. The horiz<strong>on</strong>tal line represents the<br />

average fricti<strong>on</strong> coefficient determined using the guarded sled. The<br />

other line is a linear regressi<strong>on</strong> fit to straight line through the<br />

fricti<strong>on</strong> coefficient data obtained by the c<strong>on</strong>venti<strong>on</strong>al sled.<br />

μ<br />

0.40<br />

0.35<br />

0.30<br />

0.25<br />

0.20<br />

0 1 2 3 4 5<br />

Number of Batts<br />

FIGURE 5. The fricti<strong>on</strong> coefficient <str<strong>on</strong>g>for</str<strong>on</strong>g> the polyester knit fabric<br />

resting <strong>on</strong> 0-4 polyester batts. Symbols and lines are the same as in<br />

Figure 4.<br />

The true sliding fricti<strong>on</strong> was also obtained by<br />

extrapolating the fricti<strong>on</strong> coefficient to zero batts; i.e.<br />

a thin, incompressible PET layer which was identical<br />

to the batts in all other ways. If the c<strong>on</strong>venti<strong>on</strong>al sled<br />

data were extrapolated to 0 batts, the resulting<br />

fricti<strong>on</strong> coefficient was 0.3. On the other hand, the<br />

guarded sled gave a value of 0.31, regardless of the<br />

number of batts. Thus no extrapolati<strong>on</strong> was needed<br />

when the fricti<strong>on</strong> coefficient was measured using the<br />

guarded sled. This is especially important <str<strong>on</strong>g>for</str<strong>on</strong>g><br />

materials where extrapolati<strong>on</strong> to zero thickness is<br />

impractical. For example, in a fabric-foam laminate,<br />

changing the thickness of the foam may not be<br />

practical, while stacking multiple layers of the<br />

laminate may not faithfully represent the mechanic<br />

de<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong> behavior of the laminate.<br />

To c<strong>on</strong>firm that the guarded sled measures the true<br />

sliding fricti<strong>on</strong>, the fricti<strong>on</strong> of the sled <strong>on</strong> a PET knit<br />

fabric was tested resting <strong>on</strong> the aluminum plate or <strong>on</strong><br />

1-4 of the batts used above, (Figure 5). In this case,<br />

the sled slid <strong>on</strong> the same surface of the PET knit<br />

regardless of the number of batts interspersed<br />

between the fabric and the aluminum plate. Again,<br />

the guarded sled provided the sliding fricti<strong>on</strong><br />

coefficient of the sled <strong>on</strong> the knit fabric, while the<br />

c<strong>on</strong>venti<strong>on</strong>al sled included a c<strong>on</strong>tributi<strong>on</strong> from the<br />

compressi<strong>on</strong> and de<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong> of the underlying<br />

polyester batts. When no batts were present, both<br />

sleds measured the same fricti<strong>on</strong> coefficient. In other<br />

words, while sliding across the surface of a<br />

de<str<strong>on</strong>g>for</str<strong>on</strong>g>mable substrate, the c<strong>on</strong>venti<strong>on</strong>al sled de<str<strong>on</strong>g>for</str<strong>on</strong>g>med<br />

4

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