Words

Friday Song Lyric: Nick Cave

Amara reminds me that we haven’t had any poetry here for a while. Don’t have a good stand-alone poem on hand, but I’ve always had a soft spot for these lyrics from Nick Cave’s The Boatman’s Call album.

Into My Arms

I don’t believe in an interventionist God
But I know, darling, that you do
But if I did I would kneel down and ask Him
Not to intervene when it came to you
Not to touch a hair on your head
To leave you as you are
And if He felt He had to direct you
Then direct you into my arms

Into my arms, O Lord
Into my arms, O Lord
Into my arms, O Lord
Into my arms

And I don’t believe in the existence of angels
But looking at you I wonder if that’s true
But if I did I would summon them together
And ask them to watch over you
To each burn a candle for you
To make bright and clear your path
And to walk, like Christ, in grace and love
And guide you into my arms

Into my arms, O Lord
Into my arms, O Lord
Into my arms, O Lord
Into my arms

But I believe in Love
And I know that you do too
And I believe in some kind of path
That we can walk down, me and you
So keep your candles burning
And make a journey bright and pure
That you’ll keep returning
Always and evermore

Into my arms, O Lord
Into my arms, O Lord
Into my arms, O Lord
Into my arms

See the video on YouTube for full effect.

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Science Blogging Anthology

Science Blogging AnthologyIn the shortest turnaround time for a book ever, Bora “coturnix” Zivkovic (of Blog Around the Clock fame) has put together The Open Laboratory, a collection of the greatest science blogging of all time. Which is a little bit less impressive than it sounds, since science blogging hasn’t been around for that many centuries. Still, it’s a fun concept, to take all of those words on the internet and bind them between covers. I’ll admit that I nominated my own quantum puppies post, in the tradition of all great media shamelessness.

For those of you not quite willing to pay for what you find for free by pointing and clicking, you can peruse all 50 of the selected posts, or the complete list of nominees, without ever leaving your computer. For those of you who are willing, here you go.

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The Physics of Imaginary Things

Quadruple digits! Yes, this is our 1000th post here at Cosmic Variance. In honor of which we will — well, nothing special. But I will indulge in some shameless pluggery.

Physics of the Buffyverse Today, you see, is the official publication date of The Physics of the Buffyverse, by the blogosphere’s own Jennifer Ouellette. I’m not going to offer a proper review of the book, because (1) I’ve only had a chance to skim it thus far, and (2) the author bakes me scones, which is a conflict of interest if ever I’ve seen one. But you could do a lot worse than buying a few copies for yourself and all your friends, let me assure you.

The construction of the title — The [field of academic inquiry] of [product of human imagination] — is by now well-known, inspired in large part by Lawrence Krauss’s The Physics of Star Trek. (In addition to the Physics, we’ve learned about the Ethics, the Art, the Computers, the Religions, and the Metaphysics of Star Trek, as well as corresponding studies of Star Wars, Harry Potter, and so on.) And as long as it’s been in circulation, the idea of subjecting TV shows or fantasy genres to scientific investigation has been the target of scoffing from curmudgeonly old folks who are taking a temporary break from chasing kids out of their yards. After all, they will tell you, how can you learn anything about science by studying fiction? Science is all about the real world! It has nothing to say about fake worlds that someone just made up.

Balderdash, of course. Neither physics, nor any other science, is some list of facts and theories to be committed to memory. There are a bunch of established pieces of knowledge that are worth remembering, no doubt about that, but much more important is the process by which that knowledge is acquired. And that process is just as applicable to imaginary worlds as it is to the real one. Any respectable universe, whether we find it out there or make it up ourselves, will be subject to certain internal rules of behavior. (When it comes to fiction, those rules are occasionally sacrificed for the sake of the plot, whereas in the real world they’re a bit more immutable.) Learning how to discover those rules, from the standpoint of an observer rather than one of the creators, is nothing more or less than learning how science is done.

I’ve long thought that video games would be a great way to teach the scientific method to kids. They’re playing them anyway — why not think of it as collecting data? The other day Seed’s Daily Zeitgeist linked to this gravity game.

Gravity Game

Your job is to give initial conditions (position and velocity) to a little test body, which then moves around under the gravitational field of various heavier bodies, with the goal being to survive for as long as possible without colliding with one of the planets. But the “laws of gravity” certainly aren’t the ones that Newton came up with, as a bit of experimentation shows; for one thing, orbits around just one planet don’t describe conic sections, they decay in spirals. So what are the laws? Does the strength of gravity obey something other than the familiar inverse-square law? Or is there dissipation? Are energy and angular momentum conserved? Even better, is there some definition of “energy” and “angular momentum” such that they are conserved? What about those boundary conditions at the edges of the box? They are in some sense reflective, but the magnitude of momentum certainly isn’t conserved — what’s the rule? We know in this case that there certainly are hard-and-fast rules, as the programmers put them into the code. I would love to see kids in science classes using a game like this as a miniature “laboratory,” in which they designed experiments to test different hypotheses they came up with.

Somewhat more complex is N, the ninja game from metanet.

Ninja game

Here the physics is substantially richer. You are a tiny ninja, whose job is to jump around and avoid threats while doing what it takes to open a door and escape within a specified time limit. But, being a ninja, you have unusual powers — including the ability to alter your center-of-mass momentum in midair by sheer force of will. So: is the trajectory of the ninja uniquely defined by its initial data? Are there any conserved quantities? Are the laws of motion isotropic — are the rules governing left-right motion the same as those governing up-down motion? Can the ability to stick to walls be described in terms of a coefficient of friction? You can be killed by smashing into a wall or floor too quickly — but the allowed velocity depends on the angle of impact. So what quantity is to be calculated to determine whether a landing is safe or not?

You get the point. Those of us who have become enchanted by science see the world as a giant puzzle, and our “job” is to unravel its secrets. The universe is a giant video game that a few of us get to play all the time. Yet somehow we manage to give everyone else the impression that it’s all about pulleys and inclined planes. If we can enlist the help of some imaginary characters — whether Spock or Spike — in illustrating the excitement of science, we’ll have achieved something very real indeed.

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Lost in Translation

I love the internets, because they know more about the ancient Greeks than I do. Timaeus is one of Plato’s Socratic dialogues, the one that deals with the origin of the universe. (Long story short: the demiurge created our universe, but not out of nothing; rather, by organizing some of the pre-existing chaos.) It’s also where Plato talks about Atlantis, and has remained popular for that reason. I don’t know much about Plato, but I do know something about the creation of the universe, so I’ve been invited to a conference on Timaeus to be held in Urbana next year. Which means, I suppose, that I should actually read the thing.

But my ancient Greek is rusty, so I’ll be reading it in translation. Anyone who has made any non-trivial effort to read classics in translation knows that the particular translation makes all the difference in the world — two different translators can render the same text as stilted and incomprehensible or cogent and compelling. But how to choose? I’m not so dedicated to this project that I’m going to pick up six different translations and compare them side by side.

Fortunately — the intertubes have already done it for me! We’ve reached that lovely critical point at which, given any question you have, someone has answered it on a web page somewhere, and Google can lead you to it. A bit of poking around led me to this page by Joseph Wells. He seems more interested in arguing about the existence of Atlantis than in addressing the qualities of different translations, but whatever — I didn’t say your questions would be answered intentionally. The page lists side-by-side tiny excerpts from the Timaeus in six different translations, so you can compare for yourself. For example:

Jowett 1871 Taylor 1793
for in those days the Atlantic was navigable; and there was an island situated in front of the straits which are by you called the Pillars of Heracles; the island was larger than Libya and Asia put together, and was the way to other islands, and from these you might pass to the whole of the opposite continent which surrounded the true ocean; For at that time the Atlantic sea was navigable, and had an island before the mouth which is called by you Pillars of Hercules. But the island was greater than both Libya and all Asia together, and afforded an easy passage to other neighbouring islands; as it was likewise easy to pass from those islands to all the continent which borders on this Atlantis sea.
Bury 1929 Lee 1965
For the ocean there was at that time navigable; for in front of the mouth which you Greeks call, as you say, ‘the pillars of Heracles, there lay an island which was larger than Libya3 and Asia together; and it was possible for the travelers of that time to cross from it to the other islands, and from the islands to the whole of the continent over against them which encompasses that veritable ocean. For in those days the Atlantic was navigable. There was an island opposite the strait which you call the Pillars of Hercules (Straits of Gibraltar), an island larger than Libya (Africa) and Asia combined; from it travelers could in those days reach the other islands, and from them the whole opposite continent which surrounds what can truly be called the ocean.
Kalkavage 2001 Zeyl 2000
For at that time the ocean there could be crossed, since an island was situated in front of the mouth that you people call, so you claim, the Pillars of Hercules. The island was bigger than Libya and Asia together, and from it there was access to the other islands for those traveling at that time, and from the islands to the entire opposing continent that surrounds that true sea. For at that time this ocean was passable, since it had an island in it in front of the strait that you people say you call the Pillars of Heracles. The island was larger than Libya and Asia combined, and it provided passage to the other islands for people who traveled in those days. From those islands one could then travel to the entire continent on the other side, which surrounds that real sea beyond.

What more could you ask for? On this basis I’m going for the Zeyl translation, which seems to read the most like something that could have been written in English. I kind of like “navigable” rather than “passable,” but you can’t have everything.

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Toward a Unified Epistemology of the Natural Sciences

Donald Rumsfeld Dr. Free-Ride reminds us of the celebrated free-verse philosophizing of Donald Rumsfeld, from a 2002 Department of Defense news briefing.

As we know,
There are known knowns.
There are things we know we know.

We also know
There are known unknowns.
That is to say
We know there are some things
We do not know.

But there are also unknown unknowns,
The ones we don’t know
We don’t know.

We tease our erstwhile Defense Secretary, but beneath the whimsical parallelisms, the quote actually makes perfect sense. In fact, I’ll be using it in my talk later today on the nature of science. One of the distinguishing features of science, I will argue, is that we pretty much know which knowns are known. That is to say, it’s obviously true that there are plenty of questions to which science does not know the answer, as well as some to which it does. But the nice thing is that we have a pretty good idea of where the boundary is. Where people often go wrong — and I’ll use examples of astrology, Intelligent Design, perpetual-motion machines, and What the Bleep Do We Know? — is in attempting to squeeze remarkable and wholly implausible wonders into the tightly-delimited regimes where science doesn’t yet have it all figured out, or hasn’t done some explicit experiment. (For example, it may be true that we haven’t taken apart and understood your specific perpetual-motion device, but it pretty obviously violates not only conservation of energy, but also Maxwell’s equations and Newton’s laws of motion. We don’t need to spend time worrying about your particular gizmo; we already know it can’t work.)

Rumsfeld’s comprehensive classification system did, admittedly, leave out the crucial category of unknown knowns — the things you think you know, that aren’t true. Those had something to do with his ultimate downfall.

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After Reading a Child’s Guide to Modern Physics

Abbas at 3 Quarks reminds us that next year is W.H. Auden’s centenary (and that Britain is curiously unenthusiastic about celebrating the event). The BBC allows you to hear Auden read this poem at a 1965 festival; his father was a physicist.

If all a top physicist knows
About the Truth be true,
Then, for all the so-and-so’s,
Futility and grime,
Our common world contains,
We have a better time
Than the Greater Nebulae do,
Or the atoms in our brains.

Marriage is rarely bliss
But, surely it would be worse
As particles to pelt
At thousands of miles per sec
About a universe
Wherein a lover’s kiss
Would either not be felt
Or break the loved one’s neck.

Though the face at which I stare
While shaving it be cruel
For, year after year, it repels
An ageing suitor, it has,
Thank God, sufficient mass
To be altogether there,
Not an indeterminate gruel
Which is partly somewhere else.

Our eyes prefer to suppose
That a habitable place
Has a geocentric view,
That architects enclose
A quiet Euclidian space:
Exploded myths – but who
Could feel at home astraddle
An ever expanding saddle?

This passion of our kind
For the process of finding out
Is a fact one can hardly doubt,
But I would rejoice in it more
If I knew more clearly what
We wanted the knowledge for,
Felt certain still that the mind
Is free to know or not.

It has chosen once, it seems,
And whether our concern
For magnitude’s extremes
Really become a creature
Who comes in a median size,
Or politicizing Nature
Be altogether wise,
Is something we shall learn.

Ol’ Wystan is right; we do have a better time than most of the universe. It would be no fun to constantly worry that “a lover’s kiss / Would either not be felt / Or break the loved one’s neck.” And in a sense, it’s surprising (one might almost say unnatural) that our local conditions allow for the build-up of the delicate complexity necessary to nurture passion and poetry among we creatures of median size.

In most physical systems, we can get a pretty good idea of the relevant scales of length and time just by using dimensional analysis. If you have some fundamental timescale governing the behavior of a system, you naturally expect most processes characteristic of that system to happen on approximately that timescale, give or take an order of magnitude here or there. But our universe doesn’t work that way at all — there are dramatic balancing acts that stretch the relevant timescales far past their natural values. In the absence of any fine-tunings, the relevant timescale for the universe would be the Planck time, 10-44 seconds, whereas the actual age of the universe is more like 1018 seconds. This is actually two problems in one: why doesn’t the vacuum energy rapidly dominate over the energy density in matter and radiation — the cosmological constant problem — and, imagining that we’ve solved that one, why doesn’t spatial curvature dominate over all the energy density — the flatness problem. It would be much more “natural,” in other words, to live in either a cold and empty universe, or one that recollapsed in a jiffy.

But given that the universe does linger around, it’s still a surprise that the matter within it exhibits interesting dynamics on timescales much longer than the Planck time. A human lifespan, for example, is about 109 seconds. The human/Planck hierarchy actually owes its existence to a multi-layered series of hierarchies. First, the characteristic energy scale of particle physics is set by electroweak symmetry breaking to be about 1011 electron volts, far below the Planck energy at 1027 electron volts. (That’s known to particle physicists as “the” hierarchy problem.) And then the mass of the electron (me ~ 5 x 105 electron volts) is smaller than it really should be, as it is suppressed with respect to the electroweak scale by a Yukawa coupling of about 10-6. But then the weakness of the electromagnetic interaction, as manifested in the small value of the fine-structure constant α = 1/137, implies that the Rydberg (which sets the scales for atomic physics) is even lower than that:

Ry ~ α2 me ~ 10 electron volts.

This energy corresponds to timescales (by inserting appropriate factors of Planck’s constant and the speed of light) of about 10-18 seconds; much longer than the Planck time, but still much shorter than a human lifetime. The cascade of hierarchies continues; molecular binding energies are typically much smaller than a Rydberg, the timescales characteristic of mesocopic collections of slowly-moving molecules are correspondingly longer still, etc.

Because we don’t yet fully understand the origin of these fantastic hierarchies, we can conclude that God exists. Okay, no we can’t. Really we can conclude that we live in a multiverse in which all of the constants of nature take on different values in different places. Okay, we can’t actually conclude that either. What we can do is keep thinking about it, not jumping to too many conclusions while we try to fill one of those pesky “gaps” in our understanding that people like to insist must be evidence for their personal favorite story of reality.

But “politicizing Nature,” now that’s just bad. Not altogether wise at all.

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The Trouble With Physics

I was asked to review Lee Smolin’s The Trouble With Physics by New Scientist. The review has now appeared, although with a couple of drawbacks. Most obviously, only subscribers can read it. But more importantly, they have some antiquated print-journal notion of a “word limit,” which in my case was about 1000 words. When I started writing the review, I kind of went over the limit. By a factor of about three. This is why the Intelligent Designer invented blogs; here’s the review I would have written, if the Man hadn’t tried to stifle my creativity. (Other reviews at Backreaction and Not Even Wrong; see also Bee’s interview with Lee, or his appearance with Brian Greene on Science Friday.)

——————————————————————

It was only after re-reading and considerable head-scratching that I figured out why Lee Smolin’s The Trouble With Physics is such a frustrating book: it’s really two books, with intertwined but ultimately independent arguments. One argument is big and abstract and likely to be ignored by most of the book’s audience; the other is narrow and specific and part of a wide-ranging and heated discussion carried out between scientists, in the popular press, and on the internet. The abstract argument — about academic culture and the need to nurture speculative ideas — is, in my opinion, important and largely correct, while the specific one — about the best way to set about quantizing gravity — is overstated and undersupported. It’s too bad that vociferous debate over the latter seems likely to suck all the oxygen away from the former.

Fundamental physics (for want of a better term) is concerned with the ultimate microscopic laws of nature. In our current understanding, these laws describe gravity according to Einstein’s general theory of relativity, and everything else according to the Standard Model of particle physics. The good news is that, with just a few exceptions (dark matter and dark energy, neutrino masses), these two theories are consistent with all the experimental data we have. The bad news is that they are mutually inconsistent. The Standard Model is a quantum field theory, a direct outgrowth of the quantum-mechanical revolution of the 1920’s. General relativity (GR), meanwhile, remains a classical theory, very much in the tradition of Newtonian mechanics. The program of “quantum gravity” is to invent a quantum-mechanical theory that reduces to GR in the classical limit.

This is obviously a crucially important problem, but one that has traditionally been a sidelight in the world of theoretical physics. For one thing, coming up with good models of quantum gravity has turned out to be extremely difficult; for another, the weakness of gravity implies that quantum effects don’t become important in any realistic experiment. There is a severe conceptual divide between GR and the Standard Model, but as a practical matter there is no pressing empirical question that one or the other of them cannot answer.

Quantum gravity moved to the forefront of research in the 1980’s, for two very different reasons. One was the success of the Standard Model itself; its triumph was so complete that there weren’t any nagging experimental puzzles left to resolve (a frustrating situation that persisted for twenty years). The other was the appearance of a promising new approach: string theory, the simple idea of replacing elementary point particles by one-dimensional loops and segments of “string.” (You’re not supposed to ask what the strings are made of; they’re made of string stuff, and there are no deeper layers.) In fact the theory had been around since the late 1960’s, originally investigated as an approach to the strong interactions. But problems arose, including the unavoidable appearance of string states that had all the characteristics one would expect of gravitons, particles of gravity. Whereas most attempts to quantize gravity ran quickly aground, here was a theory that insisted on the existence of gravity even when we didn’t ask for it! In 1984, Michael Green and John Schwarz demonstrated that certain potentially worrisome anomalies in the theory could be successfully canceled, and string mania swept the particle-theory community.

In the heady days of the “first superstring revolution,” triumphalism was everywhere. String theory wasn’t just a way to quantize gravity, it was a Theory of Everything, from which we could potentially derive all of particle physics. Sadly, that hasn’t worked out, or at least not yet. (String theorists remain quite confident that the theory is compatible with everything we know about particle physics, but optimism that it will uniquely predict the low-energy world is at a low ebb.) But on the theoretical front, there have been impressive advances, including a “second revolution” in the mid-nineties. Among the most astonishing results was the discovery by Juan Maldacena of gauge/gravity duality, according to which quantum gravity in a particular background is precisely equivalent to a completely distinct field theory, without gravity, in a different number of dimensions! String theory and quantum field theory, it turns out, aren’t really separate disciplines; there is a web of dualities that reveal various different-looking string theories as simply different manifestations of the same underlying theory, and some of those manifestations are ordinary field theories. Results such as this convince string theorists that they are on the right track, even in the absence of experimental tests. (Although all but the most fervent will readily agree that experimental tests are always the ultimate arbiter.)

But it’s been a long time since the last revolution, and contact with data seems no closer. Indeed, the hope that string theory would uniquely predict a model of particle physics appears increasingly utopian; these days, it seems more likely that there is a huge number (10500 or more) phases in which string theory can find itself, each featuring different particles and forces. This embarrassment of riches has opened a possible explanation for apparent fine-tunings in nature — perhaps every phase of string theory exists somewhere, and we only find ourselves in those that are hospitable to life. But this particular prediction is not experimentally testable; if there is to be contact with data, it seems that it won’t be through predicting the details of particle physics.

It is perhaps not surprising that there has been a backlash against string theory. Lee Smolin’s The Trouble With Physics is a paradigmatic example, along with Peter Woit’s new book Not Even Wrong. Both books were foreshadowed by Roger Penrose’s massive work, The Road to Reality. But string theorists have not been silent; several years ago, Brian Greene’s The Elegant Universe was a surprise bestseller, and more recently Leonard Susskind’s The Cosmic Landscape has focused on the opportunities presented by a theory with 10500 different phases. Alex Vilenkin’s Many Worlds in One also discusses the multiverse, and Lisa Randall’s Warped Passages enthuses over the possibility of extra dimensions of spacetime — while Lawrence Krauss’s Hiding in the Mirror strikes a skeptical note. Perhaps surprisingly, these books have not been published by vanity presses — there is apparently a huge market for popular discussions of the problems and prospects of string theory and related subjects.

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Quantum Mechanics Made Easy?

I was recently asked to recommend a good popular-level book on quantum mechanics. I don’t think I know of any, at least not first hand. We had a whole thread on the Greatest Popular Science Book, filled with good suggestions, but none specifically about quantum mechanics. A quick glance through amazon.com reveals plenty of books on particle physics, or even specific notions like quantum computing, but not one book that I could recommend in good conscience to someone who just wants to know what quantum mechanics is all about. It is the greatest intellectual achievement of the twentieth century, after all.

There are some books that either come close, or might very well be perfect but I’m not familiar with them. In the latter category we have The Quantum World by Ken Ford, and David Lindley’s Where Does the Weirdness Go? These might be great, I just haven’t read them. I’m sure that the Mr. Tompkins books by George Gamow are good, since I love One, Two, Three… Infinity (and Gamow was a genius), but I haven’t actually read them. Feynman’s QED is another classic, but focuses more on quantum electrodynamics (duh) than on QM more generally. David Deutsch’s The Fabric of Reality is a fantastic book, especially if you are curious about the Many-Worlds Interpretation of quantum mechanics; but I’m not sure if it’s the best first introduction (I haven’t looked at it closely in years). And David Albert’s Quantum Mechanics and Experience is great for a careful philosophical account of what QM is all about, but again maybe not the best first exposure.

Any suggestions? Not for a good book that is related to quantum mechanics or perhaps mentions it in a chapter or two, but for something whose major goal is to provide a clear account of QM. Surely there is something?

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The Cash Value of Astronomical Ideas

Can’t … stop … blogging … must … resist …

So you may have heard that Pluto is still a planet, and indeed we have a few new ones as well! Phil Plait, Rob Knop, Clifford, and Steinn have all weighed in. Hey, it’s on the front page of the New York Times, above the fold!

The problem is that Pluto is kind of small, and far away. Those aren’t problems by themselves, but there are lots of similar-sized objects that are also out beyond Neptune, in the Kuiper Belt. As we discover more and more, should they all count as planets? And if not, shouldn’t Pluto be demoted? Nobody wants to lose Pluto among the family of planets — rumors to that effect were previously enough to inspire classrooms around the globe to write pleading letters to the astronomical powers that be, begging them not to discard the plucky ninth planet. But it’s really hard to come up with some objective criteria of planet-ness that would include the canonical nine but not open the doors to all sorts of unwanted interlopers. Now the Planet Definition Committee of the International Astronomical Union has proposed a new definition:

1) A planet is a celestial body that (a) has sufficient mass for its self-gravity to overcome rigid body forces so that it assumes a hydrostatic equilibrium (nearly round) shape, and (b) is in orbit around a star, and is neither a star nor a satellite of a planet.

It turns out that, by this proposed definition, there are twelve planets — not just the usual nine, but also Ceres (the largest asteroid, between Mars and Jupiter), and also Charon (Pluto’s moon, but far enough away that apparently it doesn’t count as a “satellite,” but as a double-planet), and UB313, a faraway rock that is even bigger than Pluto. I’m not sure why anyone thinks this is an improvement.

The thing is, it doesn’t matter. Most everyone who writes about it admits that it doesn’t matter, before launching into a passionate defense of what they think the real definition should be. But, seriously: it really doesn’t matter. We are not doing science, or learning anything about the universe here. We’re just making up a definition, and we’re doing so solely for our own convenience. There is no pre-existing Platonic nature of “planet-ness” located out there in the world, which we are trying to discover so that we may bring our nomenclature in line with it. We are not discovering anything new about nature, nor even bringing any reality into existence by our choices.

The Pragmatists figured this out long ago: we get to choose the definition to be whatever we want, and the best criterion by which to make that choice is whatever is most useful and convenient for our purposes. But people have some deep-seated desire to believe that our words should be brought in line with objective criteria, even if it’s dramatically inconvenient. (These are the same people, presumably, who think that spelling reform would be really cool.) But as Rob says, there is no physically reasonable definition that would let us stick with nine planets. That’s okay! We have every right to define “planet” to mean “Mercury, Venus, Earth, Mars, Jupiter, Saturn, Uranus, Neptune, and Pluto, plus whatever other large rocky bodies we find orbiting other stars.” Or whatever else we want. It’s completely up to us.

So we really shouldn’t have to tear up a century’s worth of textbooks and illustrations, and start trying to figure out when the shape of some particular body is governed by hydrostatic equilibrium, just to pat ourselves on the back for obeying “physically reasonable” definitions. But it looks like that’s what the IAU Planet Definition Committee wants us to do. Of course that’s what you’d expect a Planet Definition Committee to suggest; otherwise why would we need a Planet Definition Committee?

Now if you’ll excuse me, I have change-of-address forms to fill out.

[And don’t even contemplate accusing me of hypocrisy for dragging myself away from a much-deserved blog-vacation to carry on about something that I claim doesn’t matter. The definition of “planet” doesn’t matter; but appreciating that the choice of definition is a matter of our own convenience, not a matter of necessarily conforming to some objective criteria about the physical world, matters a lot.]

Update: Chris Clarke for the opposition.

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Science Plays Come of Age

“I’m too creative to do astronomy.” That was the line used, in all seriousness, by a student I once had in an astronomy lab course. The lab in question involved learning about the motion of the planets around the Sun. “If I could just write a play instead of doing the lab, I’d be fine.” Well, I replied, if you write a play demonstrating that you understand Kepler’s laws of planetary motion, and have students in the class perform it, I’ll be happy to give you full credit for the lab.

Lauren Gunderson Sadly, the requested play never materialized, as I suspected it wouldn’t. But happily, in a similar set of circumstances Lauren Gunderson responded very differently, as she explains in an article in The Scientist:

My career as a science playwright started when I asked my undergraduate physics professor to let me write a play instead of a term paper. Luckily he agreed, and the result was a time-twisting play called Background, based on cosmologist Ralph Alpher. Unexpectedly, the play not only satisfied my physics professor, it went on to receive awards and inspire productions across the country.

Lauren is a young playwright (and author of the occasionally-updated blog Deepen the Mystery) specializing in plays with scientific themes. She’s not the only one, of course; it’s become quite the cottage industry, these science plays. As Dennis Overbye put it at a conference in Santa Barbara, “Is anyone writing plays that aren’t about quantum mechanics any more?”

I’d be happy to summarize Lauren’s article, but she puts it better herself:

But what does it take to write a good science play? As a playwright, I believe in communicating science effectively, but not taking out what makes science hard. So it is absolutely essential to learn the relevant science well enough to represent it accurately — otherwise the whole play fails. I always do a lot of research from online magazines, scientists’ Web sites, and books on history and theory — everything from Brian Greene’s books on string theory to Newton’s Principia itself has passed across my desk. And many playwrights, myself included, consult scientists in person for critique, advice, and content.

In a science play, you want to make your scientists sound like real scientists. I’m not afraid to use a lot of jargon — I sometimes use what I call the “verbal wall of science” effect, in which I allow a character to speak freely like a scientist, without any further explanation. This isn’t to confuse a general audience, but to allow an appreciation of the character’s expertise. Yet I also try to combine effective science with effective poetry to create something that is true both in the concrete and the abstract. Science metaphors work best this way. For example, the particle physicist in my play Baby M explains her work this way:

We move in secrets. Fundamentals locked, related in code. What is obvious is not always what is. And what is isn’t always what is known. Essentially, we deal in thought made manifest, and this work represents the world.

The best scientific characters do all the things that make us human, not just the things that make us brilliant. So it is not enough for me to show you scientists doing science; I need to show you why they do it. Why do they venture into the essence of nature? Why do they subject themselves to deadlines and peer reviews and failure?

Okay, we wish that most scientists spoke as eloquently about their work as Lauren’s character does. But the point remains: if you’re going to have scientific themes, it’s worth the effort to get the science right, and — perhaps even harder — to get the attitude and language of the scientists right. Nothing different than would be expected if you were writing about lawyers or doctors.

Last year I gave two “literary lectures” at local theaters that were putting on plays with science themes. The first one was a production of Charlotte Jones’s Humble Boy
at Remy Bumppo Theatre. The protagonist was a string theorist, who used physics as an escape from the messy complications of human interaction; it was a great play, in which the physics was scientifically correct and cleverly deployed to illuminate the plot. The second play will remain nameless. Its protagonist was also a string theorist, but the moral of this story was that the best way to make a breakthrough in string theory would be to give up all those bothersome equations and hike around the mountains in India seeking enlightenment. There’s a joke in there somewhere about the Landscape, but I don’t think that’s what the author was aiming for.

So it’s worth supporting the good stuff — for example, you could do worse than starting with Lauren’s book, a collection of three of her plays. As Sir Isaac Newton says, in words Lauren put in his mouth:

Men have died chasing what I’m after! Sacrificed life and loyalty. It is not funny. This consciousness is as serious as you can possibly come close to knowing. You should treat it as such.

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