Life at Low Reynolds Number

“Life at Low Reynolds Number,” by .

In Chapter 1 of , and I cite ’s wonderful article “ ” (, Volume 45, Pages 3–11, 1977). This paper is a transcript of a talk gave to honor physicist . The transcript captures the casual tone of the talk, and the hand-drawn figures are charming. Below I quote excerpts from the article, including my own versions of a couple of the drawings. Notice how his words emphasize insight. As Purcell says, “some essential hand-waving could not be reproduced.” Enjoy!

I’m going to talk about a world which, as physicists, we almost never think about. The physicist hears about in high school when he’s repeating and never hears about it again, as least not in what I teach. And , of course, is something for the engineers. And the low Reynolds number regime most engineers aren’t even interested in… But I want to take you into the world of very low Reynolds number-a world which is inhabited by the overwhelming majority of the organisms in this room. This world is quite different from the one that we have developed our intuitions in…

Based on Figure 1 from “Life at Low Reynolds Number.”

In Fig. 1, you see an object which is moving through a fluid with velocity v. It has dimension a,… η and ρ are the viscosity and density of the fluid. The ratio of the inertial forces to the viscous forces, as pointed out slightly less than a hundred years ago, is given by av ρ/η or av/ν, where ν is called the . It’s easier to remember its dimensions; for water, ν = 10^−2 cm^2/sec. The ratio is called the Reynolds number and when that number is small the viscous forces dominate… Now consider things that move through a liquid… The Reynolds number for a man swimming in water might be 10^4, if we put in reasonable dimensions. For a goldfish or a tiny guppy it might get down to 10^2. For the animals that we’re going to be talking about, as we’ll see in a moment, it’s about 10^−4 or 10^−5. For these animals is totally irrelevant. We know , but they could scarcely care less. I’ll show you a picture of the real animals in a bit but we are going to be talking about objects which are the order of a micron in size… In water where the kinematic viscosity is 10^−2cm^2/sec these things move around with a typical speed of 10 /sec. If I have to push that animal to move it, and suddenly I stop pushing, how far will it coast before it slows down? The answer is, about 0.1 . And it takes it about 0.6 μsec to slow down. I think this makes it clear what low Reynolds number means. Inertia plays no role whatsoever. If you are at very low Reynolds number, what you are doing at the moment is entirely determined by the forces that are exerted on you at that moment, and by nothing in the past…

Based on Figure 18 from “Life at Low Reynolds Number.”

Diffusion is important because of [a] very peculiar feature of the world at low Reynolds number, and that is, stirring isn’t any good… At low Reynolds number you can’t shake off your environment. If you move, you take it along; it only gradually falls behind. We can use elementary physics to look at this in a very simple way. The time for transporting anything a distance by stirring is about divided by the stirring speed v. Whereas, for transport by , it’s 2 divided by D, the diffusion constant. The ratio of those two times is a measure of the effectiveness of stirring versus that of diffusion for any given distance and diffusion constant. I’m sure this ratio has someone’s name but I don’t know the literature and I don’t know whose number that’s called. Call it S for stirring number. It’s just v/D. You’ll notice by the way that the Reynolds number was v/ν. ν is the kinematic viscosity in cm^2/sec, and D is the diffusion constant in cm^2/sec, for whatever it is that we are interested in following-let’s say a nutrient molecule in water. Now, in water the diffusion constant is pretty much the same for every reasonably sized molecule, something like 10^−5 cm^2/sec. In the size domain that we’re interested in, of micron distances, we find that the stirring number S is 10^−2, for the velocities that we are talking about (Fig. 18). In other words, this bug can’t do anything by stirring its local surroundings. It might as well wait for things to diffuse, either in or out. The transport of wastes away from the animal or food to the animal is entirely controlled locally by diffusion. You can thrash around a lot, but the fellow who just sits there quietly waiting for stuff to diffuse will collect just as much.

The Physics of Life: Life at Low Reynolds Number
Edward Purcell

Originally published at .

--

--

--

Professor of Physics at Oakland University and coauthor of the textbook Intermediate Physics for Medicine and Biology.

Love podcasts or audiobooks? Learn on the go with our new app.

Recommended from Medium

Free Convection and the Origin of Life

Being in the Cosmos:

“Pancreatic Cancer” Science-Research, January 2022, Week 1 — summary from MedlinePlus Genetics…

Were Humans Always A Separate Species?

“Brain Tissue” Science-Research, February 2022, Week 2 — summary from DOAJ, MedlinePlus Genetics…

Can music help plants grow? Fascinating things happen with sound

If time is fuzzy, the idea of causality may be in trouble

“Carbon Capture” Science-Research, September 2021 — summary from Department of Energy Pages |…

Get the Medium app

A button that says 'Download on the App Store', and if clicked it will lead you to the iOS App store
A button that says 'Get it on, Google Play', and if clicked it will lead you to the Google Play store
Brad Roth

Brad Roth

Professor of Physics at Oakland University and coauthor of the textbook Intermediate Physics for Medicine and Biology.

More from Medium

9 More Quotes That Will Change the Way You Think About Nature

woman in a red dress standing in a field of red flowers.

Secrets of the Lost Seal

The Home Doctor — Practical Medicine for Every Household

The Cause of the Fatal Train Accident