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PANDA-D: Interface-free determination of two dynamic contact angles

The paper introduces PANDA-D, an interface-free method that jointly analyzes density profiles and layerwise center-of-mass displacements to accurately and automatically determine both advancing and receding dynamic contact angles in molecular simulations, thereby eliminating the need for error-prone interface extraction and tangent fitting.

Original authors: Georgii K. Vandyshev, Grigorii S. Gorkaev, Nikolay D. Kondratyuk, Kirill M. Gerke, Ilia V. Kopanichuk

Published 2026-10-16
📖 6 min read🧠 Deep dive

Original authors: Georgii K. Vandyshev, Grigorii S. Gorkaev, Nikolay D. Kondratyuk, Kirill M. Gerke, Ilia V. Kopanichuk

Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). ✨ This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

When a drop of water sits on a leaf, it forms a distinct shape, resting at a specific angle where the liquid, the solid surface, and the air meet. This angle, known as the contact angle, is the most compact way scientists describe how well a liquid wets a surface. If the angle is small, the liquid spreads out; if it is large, it beads up. This simple measurement governs everything from how ink dries on paper to how oil moves through the tiny pores of underground rock. However, the world is rarely still. When a liquid moves, such as a drop sliding down a window or fluid being pushed through a narrow channel, the angle at the front of the liquid changes from the angle at the back. The front, which is pushing into new territory, usually becomes steeper, while the back, which is retreating, becomes flatter. Measuring these two different angles while the liquid is in motion is notoriously difficult, especially when the liquid is confined to spaces so small that it behaves more like a collection of individual particles than a continuous fluid.

In the microscopic world of molecular simulations, researchers have long struggled to capture these moving angles accurately. The standard method involves taking a snapshot of the liquid, drawing a line around its edge to define the surface, and then calculating the angle where that line meets the wall. This approach is fraught with trouble at the nanoscale. Because the liquid is made of discrete atoms, the edge is never perfectly sharp; it is fuzzy and fluctuating. To draw a line, a scientist must choose a specific density threshold, decide which atoms to include, and guess where the wall actually ends. These choices are arbitrary, and changing them even slightly can lead to different answers. Furthermore, when the liquid is moving, the front and back of the drop can look very similar in a simple side view, making it easy to confuse which angle is which. This ambiguity has made it hard to get a consistent, reproducible measurement of how liquids behave when they are forced to move through tiny spaces.

To solve this puzzle, a team of researchers from the Moscow Institute of Physics and Technology developed a new approach called PANDA-D. Instead of trying to trace the fuzzy edge of the liquid, they decided to look at the liquid from a different perspective entirely. They realized that while the edge is hard to define, the distribution of the liquid's mass is not. They focused on two specific things that can be measured easily from the positions of the atoms: how wide the liquid is at every height, and where the center of that width sits relative to the middle of the whole drop. The first measurement, the width, tells them how much liquid is there, but it cannot tell them if the front is steep and the back is flat, or vice versa, because the total width would be the same in both cases. It is like knowing the total length of a shadow without knowing which way the object casting it is leaning.

The breakthrough came when they added the second measurement: the center of mass. By calculating the average horizontal position of the atoms at each height, they could detect a subtle shift that reveals the direction of the tilt. If the front of the liquid is advancing, the center of mass at a given height shifts in one direction; if the back is receding, it shifts in the other. By combining the width of the liquid with this center-of-mass shift, the researchers created a mathematical model that can distinguish between the advancing and receding angles without ever needing to draw a line around the liquid's edge. This method, which they named PANDA-D, effectively turns the problem of finding a fuzzy boundary into a problem of measuring the distribution of mass, which is much more stable and easier to calculate automatically.

The team tested their new method in two ways. First, they created perfect, computer-generated models of liquid rolls with known angles and checked if PANDA-D could recover those exact numbers. It did, with an average error of less than half a degree, proving that the math works perfectly when the data is clean. Next, they applied the method to complex simulations of liquid rolls moving between solid walls, driven by an external force. In these realistic scenarios, the traditional method of drawing a line around the edge often failed to capture the correct asymmetry, sometimes matching the width of the liquid but getting the angles completely wrong. In contrast, PANDA-D successfully reproduced the observed behavior of the atoms and provided two distinct angles that agreed with independent, more traditional measurements to within less than one degree.

The researchers then used this reliable tool to explore how the angles change as they pushed the liquid harder. They found a clear, consistent pattern: as the force driving the liquid increased, the angle at the front became steeper, and the angle at the back became flatter. This relationship held true across different types of wall materials, from those that barely attract the liquid to those that pull on it strongly. The change in the angles was roughly linear, meaning that for every increase in force, the angles shifted by a predictable amount. This provides a solid, reproducible baseline for understanding how liquids move in confined spaces, free from the guesswork of defining a fuzzy boundary.

The significance of this work lies not in discovering a new law of physics, but in providing a much clearer way to see the physics that is already there. By removing the need to manually define the edge of a liquid, PANDA-D allows for automated, consistent analysis of thousands of simulation steps. This is crucial for studying complex systems where the liquid interface is constantly changing and where human intervention is too slow or too subjective. The method does not claim that the liquid always forms a perfect circle or that the angles are universal constants, but it offers a robust way to measure them in the messy, dynamic reality of molecular motion. As the researchers move forward, they plan to test this approach on even more complex fluids and surfaces, hoping to bring this clarity to the study of wetting in everything from industrial coatings to biological systems. The result is a tool that lets scientists see the invisible angles of moving liquids with a precision that was previously out of reach.

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