Prony Series Conversion - PolymerFEM · mined from the following implicit equations [see the ABAQUS...

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Calculation of Prony Series Parameters From Dynamic Frequency Data orgen Bergstr¨ om, Ph.D. [email protected] http://PolymerFEM.com 1 Definition of a Prony Series Let G R (t) be the shear stress relaxation modulus. Define G and G 0 by the following limits: G = lim t→∞ G R (t) (1) G 0 = G R (0). (2) From the shear relaxation modulus we can define a dimensionless relaxation modulus from: g R (t) = G R (t) G 0 . (3) The normalized shear stress relaxation modulus is often represented by a series expansion in ex- ponential terms: g R (t) = 1 - N i=1 g i 1 - e -ti , (4) where g i and τ i are material parameters. This series expansion is called the Prony series. 2 Dynamic Frequency Experiments The viscoelastic behavior of a material is often determined from dynamic vibrational experiments. In these experiments the material is exposed to small strain vibrations and the resulting storage modulus (G ) and loss modulus (G ) are determined as a function of the applied frequency: G (ω), G (ω). 3 Conversion from Dynamic Frequency Data to Prony Series Data In most finite element packages the linear viscoelasticity model is specified by a Prony series (Eq. 4). If only dynamic frequency data is available for a material then the Prony series can be deter- c orgen S. Bergstr¨ om, 2005. [email protected] 1

Transcript of Prony Series Conversion - PolymerFEM · mined from the following implicit equations [see the ABAQUS...

Page 1: Prony Series Conversion - PolymerFEM · mined from the following implicit equations [see the ABAQUS theory manual for a derivation]: G0(ω) = G 0 1− XN i=1 g i +G

Calculation of Prony Series Parameters From DynamicFrequency Data

Jorgen Bergstrom, Ph.D.

[email protected]://PolymerFEM.com

1 Definition of a Prony SeriesLet GR(t) be the shear stress relaxation modulus. Define G∞ and G0 by the following limits:

G∞ = limt→∞

GR(t) (1)

G0 = GR(0). (2)

From the shear relaxation modulus we can define a dimensionless relaxation modulus from:

gR(t) =GR(t)

G0. (3)

The normalized shear stress relaxation modulus is often represented by a series expansion in ex-ponential terms:

gR(t) = 1 −N∑

i=1

gi

[1 − e−t/τi

], (4)

where gi and τi are material parameters. This series expansion is called the Prony series.

2 Dynamic Frequency ExperimentsThe viscoelastic behavior of a material is often determined from dynamic vibrational experiments.In these experiments the material is exposed to small strain vibrations and the resulting storagemodulus (G′) and loss modulus (G′′) are determined as a function of the applied frequency: G′(ω),G′′(ω).

3 Conversion from Dynamic Frequency Data to Prony SeriesData

In most finite element packages the linear viscoelasticity model is specified by a Prony series (Eq.4). If only dynamic frequency data is available for a material then the Prony series can be deter-

c©Jorgen S. Bergstrom, [email protected]

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Page 2: Prony Series Conversion - PolymerFEM · mined from the following implicit equations [see the ABAQUS theory manual for a derivation]: G0(ω) = G 0 1− XN i=1 g i +G

mined from the following implicit equations [see the ABAQUS theory manual for a derivation]:

G′(ω) = G0

1 − N∑i=1

gi

+G0

N∑i=1

giτ2iω

2

1 + τ2iω

2(5)

G′′(ω) = G0

N∑i=1

giτiω

1 + τ2iω

2. (6)

These equations determine the storage modulus and the loss modulus for a given Prony series. Inthis case we are interested in the reverse relationship, that is, if we know G′(ω) and G′′(ω) thenwhat is the Prony series (G0, N, gi, τi)?

To solve this problem we can use the following approach.

1. Pick a value for N.

2. Guess values for G0, gi, τi.

3. Calculate G′(ω) and G′′(ω).

4. Calculate the residual between the calculated dynamic data and the experimental dynamicdata.

5. Optimize the parameters G0, gi, and τi using any minimization algorithm (e.g. the Simplexmethod). Goto 3.

c©Jorgen S. Bergstrom, [email protected]

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