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buletinul institutului politehnic din iaşi - Universitatea Tehnică ...

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Bul. Inst. Polit. Iaşi, t. LVIII (LXII), f. 4, 2012 215<br />

Table 2<br />

Demand conditions<br />

Charge (N) 15<br />

Speed (m.s -1 ) 0.1…1.5<br />

Temperature (°C) 80±5<br />

Browsed distance (m) 19240<br />

Number of performed rotations 1631.16<br />

Theoretical duration (min-s) 35 … 2100<br />

Table 3<br />

Material parameters<br />

Punch (friction) Disc (sample)<br />

Materials Stub X22CrNi17 (AISI431)<br />

Stainless steel martensitic<br />

Elasticity<br />

Toughness H v=247 (H v(30))<br />

Preparing the surfaces<br />

Grin<strong>din</strong>g SiC 240, 400, 1000, 2500, 4000<br />

papers. First 4 papers with thin<br />

adhesive tape, the last paper with<br />

foamy adhesive tape<br />

SiC 600, 1200, 4000 papers. For 5<br />

minutes, each paper.<br />

Speed 150 tr/min<br />

Charge 13 N<br />

Solution Ethanol Water<br />

Device TFA (tribometer) Grinder, Charge 13 N<br />

Cleaning Ethanol Ultrason Ethanol -5min<br />

Oven (60°C)<br />

State of surfaces before friction<br />

Before<br />

(nm)<br />

After (nm) Before (nm) After (nm)<br />

Arithmetic average<br />

rugosity (Ra)<br />

--- 4523 63 4323<br />

Average square<br />

rugosity (Rq)<br />

--- 5566 82 5250<br />

Skewness (Sk) --- -0.34 --- ---<br />

Kurtosis (Ek) --- 2.72 29.58 ---<br />

Due to the fact that the friction device was not dismounted after the<br />

preparation, we do not have images, nor values for the roughness before the test.<br />

The values Ra, Rq, Ssk, Sku are computed accor<strong>din</strong>g to the analysed surface.<br />

The values measured after the test for the sample are taken on the track.<br />

3. Results<br />

Starting from the values enlisted by the couple contact pickoff (Nm) and<br />

knowing the medium radius of the friction track on the disc (r = 0.0135 m) and<br />

the normal force applied on the pawn, the evolution of the friction coefficient in<br />

time can be followed. The friction quotient was deducted from d’Amontons law<br />

(Fig. 2 and Table 4), with the state of the surface presented in Fig. 3.

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