26.03.2017 Views

Materials for engineering, 3rd Edition - (Malestrom)

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

66<br />

<strong>Materials</strong> <strong>for</strong> <strong>engineering</strong><br />

(a) (b) (c)<br />

2.22 Spring-and-dashpot models of viscoelastic solids (a) Maxwell,<br />

(b) Voigt and (c) four-element model.<br />

same and the total strain or strain rate is determined from the sum of the two<br />

components:<br />

de<br />

d = σ<br />

+ 1d σ<br />

t η E dt<br />

Voigt model<br />

When the spring and dashpot are in parallel (Fig. 2.22(b)), the strains in the<br />

two elements are equal and the total stress on them is given by the sum:<br />

de<br />

σ T ( t) = Ee + η<br />

dt<br />

If the applied stress is constant, as in a creep test, this differential equation<br />

may be directly integrated to give the strain as a function of time:<br />

et ( ) =<br />

σ –t/ τ<br />

(1 – e )<br />

E<br />

where the time constant, τ = η/E.<br />

Four-element model<br />

A more realistic description of polymer behaviour is obtained with a fourelement<br />

model consisting of Maxwell and Voigt elements in series (Fig.<br />

2.22(c)). By combining the above equations, the total strain experienced by<br />

this model is given by:<br />

et ( ) =<br />

σ<br />

+<br />

σ –t/ τ<br />

(1 – e ) +<br />

σ<br />

t<br />

E E<br />

η<br />

1 2

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!