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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

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