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Scaling properties of viscous fingering
Fluid Dynamics · Submitted 31 Oct 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that the area $A$ of a viscous-fingering cluster varies as a simple power law $A \sim L^{\alpha}$ of its interface length $L$.
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The abstract, sentence by sentence
We present a study of viscous fingering using the Volume Of Fluid method and a central injection geometry, assuming a Laplacian field and a simple surface tension law. As in experiments we see branched structures resulting from the Saffman-Taylor instability. We find that the area $A$ of a viscous-fingering cluster varies as a simple power law $A \sim L^{\alpha}$ of its interface length $L$. Our results are compared to previously published simulations in which the viscosity of the invading fluid is vanishing. We find differences in exponent $\alpha$ and in the appearance of detached droplets and bubbles.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a study of viscous fingering using the Volume Of Fluid method and a central injection geometry, assuming a Laplacian field and a simple surface tension law. | method 0.76 | 0.91 | 0.03 | asserted 0.95 |
| s1 | As in experiments we see branched structures resulting from the Saffman-Taylor instability. | result 0.98 | 0.78 | 0.04 | asserted 1.00 |
| s2 | We find that the area $A$ of a viscous-fingering cluster varies as a simple power law $A \sim L^{\alpha}$ of its interface length $L$. | result 1.00 | 0.97 | 0.76 | asserted 1.00 |
| s3 | Our results are compared to previously published simulations in which the viscosity of the invading fluid is vanishing. | background 0.42 | 0.23 | 0.04 | asserted 0.94 |
| s4 | We find differences in exponent $\alpha$ and in the appearance of detached droplets and bubbles. | result 1.00 | 0.94 | 0.21 | asserted 1.00 |
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The paper
Original abstract
We present a study of viscous fingering using the Volume Of Fluid method and a central injection geometry, assuming a Laplacian field and a simple surface tension law. As in experiments we see branched structures resulting from the Saffman-Taylor instability. We find that the area $A$ of a viscous-fingering cluster varies as a simple power law $A \sim L^{\alpha}$ of its interface length $L$. Our results are compared to previously published simulations in which the viscosity of the invading fluid is vanishing. We find differences in exponent $\alpha$ and in the appearance of detached droplets and bubbles.
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