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ExponentialHarmonicHyperbolicPower Loss
b = 1b = 00 < b < 1

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bodyD=D_{\infty} + \frac{t^{n-1}}{\tau^{n}}


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q(t)=q_{i} \exp \left( -D \, t \right)



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q(t)=\frac{q_{i}}{1+D \, t} 



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q(t)=q_{i} \cdot \left( 1+b \cdot D \cdot t \right)^{-1/b}



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q(t)=q_{i} \exp \left( -D_{\infty}t- \left( t/\tau \right)^{n} \right)



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Q(t)=\frac{q_{i}-q(t)}{D}



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Q(t)=\frac{q_{i}}{D} \, \ln \left[ (\frac{q_{i}}{q(t)}) \right]



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Q(t)=\frac{q_{i}}{D \, (1-b)}( \, \left[ q_{i}^{1-b}-q(t)^{1-b}) \right]





Exponential decline has a clear physical meaning of pseudo=-steady state production with finite drainage volume.

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