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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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are all variati<strong>on</strong>s of Da Vinci's sled method. However,<br />

when measuring the fricti<strong>on</strong> of high loft n<strong>on</strong>woven<br />

fabric batts using these methods, large scale<br />

de<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong> of the fabric occurs and the apparent<br />

fricti<strong>on</strong> changes with the number of batts or the<br />

thickness of the batts, even though the material, the<br />

pressure and the normal load are unchanged. This<br />

implies that the measured fricti<strong>on</strong> includes<br />

comp<strong>on</strong>ents due to the de<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong> of the substrate<br />

as well as the sliding fricti<strong>on</strong>. The result is an<br />

incorrect value <str<strong>on</strong>g>for</str<strong>on</strong>g> the fricti<strong>on</strong>.<br />

To address the issue of sliding and de<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong> in the<br />

critical area of automobile tires, special test devices<br />

have been built, including highly instrumented<br />

automobiles with professi<strong>on</strong>al drivers. The sliding<br />

fricti<strong>on</strong> and tire de<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong> are separated by<br />

modeling. 10 In another example, when some<strong>on</strong>e is<br />

sitting in an upholstered seat and tries to get up, they<br />

both slide across the seat and de<str<strong>on</strong>g>for</str<strong>on</strong>g>m the cushi<strong>on</strong>s.<br />

Thus the energy required to get out of the seat<br />

includes both fricti<strong>on</strong> and cushi<strong>on</strong> de<str<strong>on</strong>g>for</str<strong>on</strong>g>mati<strong>on</strong>.<br />

However, the engineering soluti<strong>on</strong> to manipulate the<br />

required energy <str<strong>on</strong>g>for</str<strong>on</strong>g> each comp<strong>on</strong>ent is different and<br />

it would be useful to clearly separate these factors so<br />

that the seat or tire could be designed rati<strong>on</strong>ally <str<strong>on</strong>g>for</str<strong>on</strong>g><br />

each c<strong>on</strong>tributi<strong>on</strong> to the energy.<br />

This manuscript describes a new fricti<strong>on</strong> measuring<br />

instrument designed to directly separate the <str<strong>on</strong>g>for</str<strong>on</strong>g>ce<br />

required to de<str<strong>on</strong>g>for</str<strong>on</strong>g>m the substrate from the <str<strong>on</strong>g>for</str<strong>on</strong>g>ce<br />

required to overcome fricti<strong>on</strong>. The c<strong>on</strong>cept that led to<br />

our design is the same as that used to eliminate the<br />

effects of stray electrical fields or edge effects in<br />

measuring high impedances in dielectric<br />

measurements or bulk c<strong>on</strong>ductivity in polymers. In<br />

these measurements, an additi<strong>on</strong>al electrode<br />

surrounds the test electrode, thus screening edge<br />

effects. This approach is mimicked in the new,<br />

guarded fricti<strong>on</strong> sled, where an outer sled de<str<strong>on</strong>g>for</str<strong>on</strong>g>ms the<br />

substrate and acts as a c<strong>on</strong>venti<strong>on</strong>al sled, while an<br />

inner sled – which is the guarded sled – measures<br />

<strong>on</strong>ly the sliding fricti<strong>on</strong> <strong>on</strong> the already de<str<strong>on</strong>g>for</str<strong>on</strong>g>med<br />

substrate.<br />

DESCRIPTION OF FRICTOMETER<br />

Figure 1 shows a picture of the guarded fricti<strong>on</strong><br />

meter. It is made from a single piece of steel,<br />

measuring 12 cm x 15 cm x 2.5 cm. The outer,<br />

c<strong>on</strong>venti<strong>on</strong>al sled, S, is pulled by a tensi<strong>on</strong> load<br />

transducer (Omegadyne LCFD-50, Sunbury, OH), F c ,<br />

via cord C. A semicircular secti<strong>on</strong> is cut out of the<br />

center of this sled to <str<strong>on</strong>g>for</str<strong>on</strong>g>m the guarded sled, G, which<br />

is pulled by a compressi<strong>on</strong> load transducer<br />

(Omegadyne LC8100-250-25), F g , via a screw that<br />

passes through F g , through a washer, and through a<br />

slot, which allows G to move vertically relative to S.<br />

Appropriate spacing between S and G is maintained<br />

by an additi<strong>on</strong>al washer. Both S and G are made from<br />

the same material and are the same thickness so that<br />

the pressure is the same under both sleds. Additi<strong>on</strong>al<br />

weights can be added to alter the loads and the<br />

pressures. The shape of the inner sled can be chosen<br />

as appropriate <str<strong>on</strong>g>for</str<strong>on</strong>g> the desired test c<strong>on</strong>diti<strong>on</strong>s. In our<br />

instrument, it is semicircular to avoid snagging <strong>on</strong> a<br />

fibrous substrate. The fr<strong>on</strong>t edges of both sleds are<br />

rounded slightly to avoid digging into soft substrates.<br />

A motor (1 rpm, Merkle Korff Industries, Des Plaines,<br />

IL) attached to a 10:1 reducti<strong>on</strong> gearbox (Gam Gear,<br />

Chicago, IL) pulls the compound sled via a cord at a<br />

rate of 5.30 mm/min. The load transducers are read<br />

using an A/D card (CIO-DAS801 from Omega<br />

Engineering, Inc., Stam<str<strong>on</strong>g>for</str<strong>on</strong>g>d, CT) and the data are<br />

collected using LabView (Nati<strong>on</strong>al Instruments,<br />

Austin, TX).<br />

FIGURE 1. The compound sled that <str<strong>on</strong>g>for</str<strong>on</strong>g>ms the guarded fricti<strong>on</strong><br />

meter is shown. The c<strong>on</strong>venti<strong>on</strong>al sled, S, is pulled by cord, C, and<br />

tensi<strong>on</strong> load transducer, T 2 , which measures the <str<strong>on</strong>g>for</str<strong>on</strong>g>ce, F c , required<br />

to pull the compound sled. S, in turn, pulls the guarded sled, G, via<br />

compressi<strong>on</strong> load transducer, T 1 , which measures the <str<strong>on</strong>g>for</str<strong>on</strong>g>ce, F g ,<br />

required to pull <strong>on</strong>ly the guarded sled. The guarded sled floats<br />

freely within the c<strong>on</strong>venti<strong>on</strong>al sled, restrained <strong>on</strong>ly by T 1 .<br />

TEST PROCEDURES<br />

During a test, the sample is placed <strong>on</strong> an aluminum<br />

block and the back edge is clamped in place. The<br />

compound sled is placed <strong>on</strong> a flat surface and the<br />

unloaded readings, R unloaded , <str<strong>on</strong>g>for</str<strong>on</strong>g> the transducers are<br />

read. Next, the load cells are calibrated by<br />

suspending the compound sled via the towing cord<br />

and reading the load cells again to obtain the loaded<br />

reading, R loaded . The calibrati<strong>on</strong> factor is simply:<br />

2

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