Product Guide for Design Engineers - Quadrant
Product Guide for Design Engineers - Quadrant
Product Guide for Design Engineers - Quadrant
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Effective Selection & <strong>Design</strong> Techniques<br />
The modulus of elasticity of most plastics is temperature dependent [decreases with increasing temperature]<br />
and in order to allow calculation of de<strong>for</strong>mation under short term loads at various temperatures, we have<br />
included in this brochure several graphs showing stiffness versus temperature of our materials [see pages<br />
36 and 55].<br />
When a plastics part is subjected to a constant static load, it de<strong>for</strong>ms quickly to a strain roughly predicted by<br />
its short-term modulus of elasticity [Hooke‘s law] and then continues to de<strong>for</strong>m at a slower rate indefi nitely,<br />
or if the load is high enough until rupture occurs. This phenomenon, which also occurs in structural metals at<br />
very high temperatures, is called creep.<br />
Fig. 2: Tensile Creep Behaviour of Ertacetal ® C at 23 °C [*]<br />
5<br />
4<br />
1 - 6 : different stress levels<br />
6<br />
5<br />
10 MPa<br />
15 MPa<br />
20 MPa<br />
25 MPa<br />
30 MPa<br />
35 MPa<br />
Strain [%]<br />
3<br />
2<br />
4<br />
3<br />
[*]: based on raw<br />
material supplier data<br />
2<br />
1<br />
1<br />
0<br />
0.1<br />
1 10 100<br />
1000 10000 100000<br />
Loading time [h]<br />
Fig. 3:<br />
Isometric Stress-Time Curve <strong>for</strong> a<br />
De<strong>for</strong>mation of 2%<br />
Fig. 4:<br />
Isochronous Stress-Strain Curve<br />
40<br />
60<br />
Stress [MPa]<br />
30<br />
20<br />
10<br />
2% strain<br />
Stress [MPa]<br />
50<br />
40<br />
30<br />
20<br />
10<br />
10 h loading time<br />
0<br />
0.1<br />
1 10 100 1000 10000 100000<br />
0<br />
0<br />
1 2 3 4 5 6 7 8 9 10 11 12 13<br />
Loading time [h]<br />
Strain [%]<br />
8