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arxiv: 1907.02802 · v1 · pith:MOML56P4new · submitted 2019-07-05 · ❄️ cond-mat.soft

Spinning drop dynamics in miscible and immiscible environments

Pith reviewed 2026-05-25 02:06 UTC · model grok-4.3

classification ❄️ cond-mat.soft
keywords spinning dropmiscible fluidsimmiscible fluidsinterfacial tensionextensional dynamicspower-law elongationrelaxation time
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0 comments X

The pith

Miscible spinning drops elongate indefinitely as length grows with time to the 2/5 power, while immiscible drops relax exponentially to a fixed shape, showing that composition gradients produce no measurable interfacial tension.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper compares the response of spinning drops to a sudden increase in rotation rate when the surrounding liquid is either fully miscible or immiscible. Immiscible drops settle to an equilibrium shape after an exponential relaxation whose time scale matches one existing theory and stays independent of the applied centrifugal force. Miscible drops never stop stretching; their length follows a clean power law that matches the prediction for drops with zero tension. The contrast leads directly to the claim that gradual composition changes in miscible pairs do not create an effective surface tension that spinning-drop methods can detect.

Core claim

Drops surrounded by an immiscible fluid relax exponentially to a steady shape with a relaxation time independent of rotation speed and in quantitative agreement with the Stone-Bush model for quasi-spherical drops; drops in a miscible fluid instead elongate without bound according to l(t) proportional to t to the 2/5, matching the Lister-Stone inviscid-drop dynamics. These observations imply that low compositional gradients in miscible fluids generate no effective interfacial tension detectable by spinning-drop tensiometry.

What carries the argument

Spinning-drop tensiometry with a rotation-speed jump, whose observed relaxation or elongation is compared directly to the Stone-Bush exponential model for immiscible drops and the Lister-Stone power-law model for inviscid drops.

If this is right

  • The relaxation time of immiscible drops does not change with the strength of the centrifugal forcing.
  • Only the Stone-Bush model matches the measured relaxation times; other published models do not.
  • Spinning-drop tensiometry cannot register any effective tension arising from weak composition gradients.
  • Miscible drops follow the same indefinite elongation law predicted for completely inviscid drops.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Alternative measurement techniques would be required if any weak effective tension exists in low-gradient miscible systems.
  • Models of fluid mixing or emulsion stability that assume an apparent tension from composition gradients may need revision for the low-gradient regime.
  • Repeating the speed-jump protocol with steeper initial composition profiles could reveal the gradient strength at which measurable tension appears.

Load-bearing premise

The indefinite elongation is produced solely by the complete absence of interfacial tension, with no modification from diffusion or other mixing effects.

What would settle it

A miscible spinning-drop experiment that reaches a steady finite length or deviates from the t to the 2/5 growth law under the same conditions.

read the original abstract

We report on the extensional dynamics of spinning drops in miscible and immiscible background fluids following a rotation speed jump. Two radically different behaviours are observed. Drops in immiscible environments relax exponentially to their equilibrium shape, with a relaxation time that does not depend on the centrifugal forcing. We find an excellent quantitative agreement with the relaxation time predicted for quasi-spherical drops by Stone and Bush (Q. Appl. Math. 54, 551 (1996)), while other models proposed in the literature fail to capture our data. By contrast, drops immersed in a miscible background fluid do not relax to a steady shape: they elongate indefinitely, their length following a power-law $l(t)\sim t^{\frac{2}{5}}$ in very good agreement with the dynamics predicted by Lister and Stone (J. Fluid Mech. 317, 275 (1996)) for inviscid drops. Our results strongly suggest that low compositional gradients in miscible fluids do not give rise to an effective interfacial tension measurable by spinning drop tensiometry.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The manuscript reports experiments on the extensional dynamics of spinning drops following a rotation-speed jump. In immiscible background fluids the drops relax exponentially to a steady shape whose relaxation time is independent of the imposed centrifugal force; the measured times agree quantitatively with the Stone-Bush (1996) prediction for quasi-spherical drops. In miscible background fluids the drops elongate indefinitely with length scaling as l(t)∼t^{2/5}, in good agreement with the inviscid-drop theory of Lister & Stone (1996). The authors conclude that low compositional gradients in miscible fluids do not produce an effective interfacial tension detectable by spinning-drop tensiometry.

Significance. If the reported scalings and model comparisons hold, the work supplies a clear experimental distinction between true interfacial tension and its absence in miscible systems. The direct, parameter-free comparison to two independent prior theories (Stone-Bush and Lister-Stone) without fitting to the present data set is a strength and supports the claim that spinning-drop tensiometry can be used to test for effective tension arising from compositional gradients.

major comments (1)
  1. [miscible-drop results and discussion] The central claim that the observed l(t)∼t^{2/5} elongation demonstrates the absence of measurable effective interfacial tension rests on the direct applicability of the Lister-Stone (1996) inviscid-drop model. That model assumes a sharp interface with no compositional evolution. The manuscript must therefore supply a concrete argument or auxiliary calculation showing that diffusion or mixing cannot alter the exponent or produce an accidental match to the t^{2/5} law (see the discussion of the miscible case and the comparison to Lister-Stone).
minor comments (2)
  1. [Abstract] The abstract states 'very good agreement' with Lister-Stone but does not indicate the time window, number of decades, or fitting procedure used to extract the exponent; this information should be added to the main text or a supplementary figure.
  2. [Methods/Experimental section] Experimental parameters (drop size, viscosity ratio, rotation rates, and compositional gradient magnitudes) are referenced only qualitatively in the abstract; a concise table or paragraph summarizing the range of conditions would improve reproducibility.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading and constructive feedback. We address the single major comment below.

read point-by-point responses
  1. Referee: [miscible-drop results and discussion] The central claim that the observed l(t)∼t^{2/5} elongation demonstrates the absence of measurable effective interfacial tension rests on the direct applicability of the Lister-Stone (1996) inviscid-drop model. That model assumes a sharp interface with no compositional evolution. The manuscript must therefore supply a concrete argument or auxiliary calculation showing that diffusion or mixing cannot alter the exponent or produce an accidental match to the t^{2/5} law (see the discussion of the miscible case and the comparison to Lister-Stone).

    Authors: We agree that the Lister–Stone model assumes a sharp interface without compositional evolution via diffusion. Our experiments use fluid pairs with low compositional gradients by construction, and the measured l(t)∼t^{2/5} scaling agrees with the inviscid theory over more than a decade in time with no adjustable parameters. Such precise, parameter-free agreement would be improbable if diffusion were modifying the leading-order exponent. Nevertheless, the referee’s request for an explicit auxiliary argument is well taken. In the revised manuscript we will add a short paragraph in the miscible-case discussion that estimates the diffusive mixing time across the drop radius (using the known molecular diffusivity) and compares it to the experimental observation window, showing that the Péclet number remains large and that significant mixing does not occur on the relevant timescales. This addition will directly address the concern while leaving the central conclusions unchanged. revision: yes

Circularity Check

0 steps flagged

No circularity: experimental scalings compared to independent external theory

full rationale

The paper reports direct experimental observations of drop elongation and relaxation, then compares the measured l(t) ~ t^{2/5} exponent and the immiscible relaxation time to scaling predictions taken from two 1996 papers by Lister/Stone and Stone/Bush. These are external citations whose derivations predate the present work and contain no parameters fitted to the current dataset. No self-citation chain, no parameter fitted on a subset then renamed as a prediction, and no redefinition of the observed power law as a derived result. The interpretation that the match implies zero effective IFT is an inference from the data-theory agreement, not a reduction of the theory to the data by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

Experimental comparison paper that relies on two prior theoretical models for interpretation; no new free parameters, axioms, or entities introduced.

axioms (2)
  • domain assumption Stone and Bush model for quasi-spherical drops applies to the immiscible relaxation data.
    Abstract states excellent quantitative agreement with this model.
  • domain assumption Lister and Stone model for inviscid drops applies to the miscible elongation data.
    Abstract states very good agreement with the predicted power law.

pith-pipeline@v0.9.0 · 5717 in / 1320 out tokens · 41754 ms · 2026-05-25T02:06:08.005637+00:00 · methodology

discussion (0)

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