annenberg media ♪ ¿y es muy difícil ser actor en puerto rico? es difícil en cualquier parte del mundo. y dime algo de ti. ¿estás casada? no. narrador: bienvenidos al episodio 24 de destinos: an introduction to spanish. en este episodio raquel empieza a dudar de las relaciones

entre jorge y angela. ¿mamá? durante una llamada por teléfono raquel le cuenta a su mamá del problema con jorge. en este episodio no hay nuevo vocabulario que aprender. presten atención a la historia y a los personajes. ¿pasa algo? vámonos, jorge. hay muchas cosas que hacer. hasta luego, raquel. te llamo más tarde. angela... hablaremos más tarde, raquel. captioning of this program is made possible by the annenberg/cpb project and the geraldine r. dodge foundation.

al final de su estancia en san germán la abuela, doña carmen, le da a angela un objeto muy especial un regalo de su padre. desde el hotel, raquel hace una llamada a buenos aires. le cuenta a arturo que angel ya murió y que angel tenía dos hijos. angela y raquel hablan con la supervisora del banco donde angela trabaja. le pide dos semanas libres para ir a méxico a visitar a su abuelo, don fernando. don fernando está muy enfermo y angela le explica a la supervisora que es urgente.

raquel y angela hacen los preparativos para salir mañana para méxico. luego, van a la universidad para ver a jorge, el novio de angela. en un patio de la universidad angela y jorge hablan de la copa. es la copa de bodas de mi abuela, rosario. ella se la dio a mi padre. claro, de padre a hijo. tengo una idea. cuando nos casemos podemos brindar con esta copa. ¿me estás proponiendo matrimonio? bueno... ( coro canta )

esta historia de la familia de angela en méxico... no sé. interesante, ¿no? ¿interesante? es como... como una obra de teatro. basada en una historia increíble. increíble pero cierta. ( siguen cantando ) raquel: este coro es excelente. es el coro de la universidad de puerto rico. ¿te gusta la canción?

sí, es muy bonita. me gustaría comprar un cassette. podemos ir a río piedras. allí hay varias tiendas donde venden cassettes, discos... ¿queda lejos río piedras? bueno. la universidad queda en el pueblo de río piedras. las tiendas de discos están muy cerca. ¿vamos? esperen un momento. tengo que hacer un mandado de urgencia. está bien. mientras tanto conversaré con raquel. bien.

¿y salen mañana para méxico? sí, mañana. ¿y ud. estudió aquí en la universidad? me puedes tutear. el tuteo es... más íntimo, ¿no? nunca he visto un "oscar" de cerca. ¿quién lo ganó? josé ferrer. por su actuación en la película "cyrano de bergerac". ¿y es difícil ser actor en puerto rico? es difícil en cualquier parte del mundo. y dime algo de ti. ¿estás casada? no. ¿y tú, viajas con frecuencia a nueva york?

sí. en nueva york tengo... bueno... tengo más oportunidades que aquí en puerto rico. sí, me imagino. bueno. estoy seguro de que angela te habrá hablado mucho de mí. ¿qué más quieres saber? gracias, jorge. pero creo que ya sé lo suficiente por ahora. pero no te parece que... bueno, ¿qué te parece jorge? ¿te está tratando bien? sí, angela. tu novio es... un encanto. ¿quieres ver un poco la universidad antes de volver? sí, ¿cómo no? jorge, ¿por qué no la llevamos a ver la colección de oller? llévala tú, amor. acabo de recordar que un estudiante quería verme en la oficina. las busco luego. pero... ¿no quieres a acompañarnos a río piedras?

no puedo. vayan uds. las buscaré más tarde. hasta luego. iqué raro! hace un momento quería acompañarnos y luego... ise evaporó! sí, es muy raro. entonces, angela lleva a raquel a ver las obras de francisco oller un pintor puertorriqueño de mucha importancia. el velorio. ¿es esto el velorio de un niño? pero si parece una fiesta. están celebrando el hecho de que el niño va directamente al cielo pues no ha pecado. qué interesante.

pues, ¿qué me cuentas? yo creí que estabas en una cita con una estudiante. no apareció. así que vine a buscarlas. jorge, ¿hay algo que quieras decirme? ¿por qué me preguntas eso? porque estás actuando muy raro. eso es lo que tú imaginas. angela, debemos volver al hotel. quiero recoger los boletos. ay, es cierto. y yo tengo que empacar y llamar a roberto otra vez. raquel, ¿no quieres comprar ese cassette? pues, sí, si la tienda está cerca. bien. vamos.

raquel, angela y jorge van al paseo de diego en río piedras. es un lugar de mucha actividad donde muchas personas van de compras. déme tres piraguas, por favor. ¿de qué sabor las quiere? frambuesa, tamarindo, coco, vainilla y anís. yo la quiero de frambuesa. ¿y tú? raquel: yo también la quiero de frambuesa. jorge: yo quiero la mía de tamarindo. gracias. ¿quieres comprar ese cassette ahora? sí, pero ya no tengo mucho tiempo. pues, por aquí...

y ese cassette te va a gustar mucho. ay, se hace tarde. ¿por qué no regresamos al hotel? después de recoger los boletos podemos descansar, tomar el sol nadar, si quieres. me parece bien. ¿pasamos por mi casa a recoger mi traje de baño? sí. nos podemos encontrar en el hotel dentro de una hora. de acuerdo. gracias. gracias. angela: iay! me encanta esta isla... la playa... el mar... el sol...

¿dónde está jorge? quiero nadar. ijorge! ivamos! jorge: ya voy. iay! iqué lentitud! idios mío! ita ta ta ta! pues, ¿qué te parece mi nuevo traje de baño? iqué colores más chillones! si quieren hacer esnorqueling necesitan presentar la llave al encargado. ¿vienes? más tarde. tengo que hacer unas llamadas importantes. bueno... vamos. que lo pasen bien.

¿mamá? ah, sí, raquel. ¿dónde estás? en san juan, mamá. ¿cómo están? por aquí muy bien. tu papá acaba de salir. tengo buenas noticias, mamá. a ver. mañana salgo para méxico y después para los angeles. iay, qué bien! ¿y para eso llamaste o te sucede algo? nada, mamá. pues... esta chica, angela, la nieta de don fernando... tiene un novio mujeriego y parece que ella no lo sabe. no te metas en las vidas privadas de los demás. ya lo sé, mamá, pero... la pobre me parece tan inocente, no sabe lo que ocurre. ¿cuánto tiempo hace que la conoces? unos días. ¿unos días? pues no es tu mejor amiga, ¿eh?

olvídate de ese asunto. no sé si pueda. mamá, llamé para decirles que voy a méxico. realmente no tengo tiempo para seguir conversando. bueno, es una lástima que tu papá no esté aquí. dale un beso de mi parte. te llamo desde méxico para decirte cuándo voy a regresar a los angeles. está bien. cuando regreses, te voy a hacer unos tamales porque me imagino que ya estás cansada de comer la comida de allá. está bien, mamá. voy a colgar. hablaremos en unos días. cuídate, hija. una chica sola por allí... una mujer. ah, sí, sí, se me olvidaba. nosotras las madres no debemos preocuparnos cuando nuestros hijos están grandes. adiós, mamá. adiós, hija.

arturo. ¿sí? arturo, ¿me oyes? sí, raquel, te oigo perfectamente. ¿cómo estás? qué pasa? estoy muy bien. acabo de confirmar las reservaciones. pues sí, dame los datos. sí, perfectamente.

ya casi termina mi viaje. y entonces, nuestro viaje puede comenzar. arturo, eres imposible. lo sé. pero es parte de mi encanto, ¿no? tengo que colgar. pero te llamo desde la capital. chau, querida. chau, arturo. ¿se divirtieron? ay, el agua estaba muy sabrosa. lo pasamos muy bien. vengo ahora. ¿quieres comer piña? está muy rica. iqué deliciosa! en nueva york, no hay piñas frescas como aquí. la extraño mucho. pero lo que más extrañas es a tu adorada novia. ¿por qué no nos vamos a vivir a nueva york?

no, gracias. me gusta visitar esa ciudad, pero ¿vivir? no. además... ¿no vas formar una compañía de teatro acá en san juan? hay en san juan un cine que puede funcionar como teatro. tiene que ser caro. sí, lo es. pero es el mejor sitio. perdónenme, voy a cambiar. tengo un plan. ¿cuál es? cuando venda mi casa voy a darle a jorge una parte del dinero. así podrá abrir su teatro. pues... yo podría trabajar allí también. pero tú ya trabajas en un banco. trabajaría en el teatro de noche. has pensado en todo. ahora tengo que convencer a jorge.

angela... ¿no crees que es mejor que él mismo compre el cine? hablas como mi abuela. bueno, tu abuela tiene mucha experiencia. ha vivido muchos años. ¿y qué? ¿por qué todo el mundo se opone a mis relaciones con jorge? angela, no es que yo quiera oponerme. sólo digo que... no me digas más. ¿por qué no te gusta jorge a ti? angela, no te enfades conmigo. no he dicho nada. pues dime entonces por qué te opones a eso del teatro. ibasta con eso de oponerme! no te pongas tan defensiva. mira, si quieres que te diga la verdad... iajái lo sabía. igual que mi abuela. iolvídalo! mi madre tiene razón. no me deben importar los asuntos de otros.

¿pasa algo? vámonos, jorge. hay muchas cosas que hacer. hasta luego, raquel. te llamo más tarde. angela... hablaremos más tarde, raquel. bueno. tengo muchas cosas de que hablar. hoy fui con angela a la universidad. y allí conocí a su novio, jorge. iy qué sorpresa para mí! jorge en seguida quería tutearme. ¿recuerdan? ¿y ud. estudió aquí en la universidad?

me puedes tutear. el tuteo es... más íntimo, ¿no? bueno. por sus acciones, yo pensé que jorge era un mujeriego o sea un don juan. raquel: y más tarde, cuando angela quería llevarme al museo ¿quería acompañarnos jorge o no? ¿quieres ver un poco la universidad antes de volver? sí, ¿cómo no? jorge, ¿por qué no la llevamos a ver la colección de oller? llévala tú, amor. acabo de recordar que un estudiante quería verme en la oficina. jorge no quería acompañarnos. dijo que un estudiante lo esperaba en su oficina.

para decir la verdad, yo creo que era una excusa... una excusa porque se sentía incómodo. bueno, angela y yo fuimos solas al museo. ¿y quién nos esperaba cuando salimos de allí? yo creí que estabas en una cita con un estudiante. no apareció. así que vine a buscarlas. jorge nos esperaba. ¿ven uds.? ningún estudiante lo esperaba en su oficina. era sólo una excusa. por fin, fuimos a unas tiendas cerca de la universidad porque yo quería comprar unos cassettes. luego vinimos aquí al hotel

porque yo había invitado a jorge y a angela a nadar. pero yo no nadé con ellos. ¿qué hacía yo mientras ellos nadaban? ¿mamá? raquel: mientras ellos nadaban yo hablaba por teléfono. primero, llamé a mi madre. yo le conté de mi opinión sobre jorge y angela. ¿y qué me dijo ella? así es mi mamá. y tenía razón. cuando yo intenté hablar con angela sobre lo del teatro

¿qué pasó? se enfadó conmigo. ¿por qué no te gusta jorge a ti? angela, no te enfades conmigo. no he dicho nada. pues dime entonces por qué te opones a eso del teatro. ibasta con eso de oponerme! no te pongas tan defensiva. mira, si quieres que te diga la verdad... iajái lo sabía. igual que mi abuela. iolvídalo! mi madre tiene razón. no me deben importar los asuntos de otros. bueno, tendré que hablar con ella más tarde. también tuve una conversación con arturo. ¿y qué creen uds.? ¿estaba arturo contento durante la conversación? arturo, eres imposible. lo sé.

pero es parte de mi encanto, ¿no? yo creo que sí. creo que arturo estaba muy contento. y yo en este momento también estoy contenta. arturo va a visitar méxico dentro de dos días. bueno. sólo hay un problema ahora. no podemos comunicarnos por teléfono con el hermano de angela. nunca está en casa. ¿dónde estará este roberto castillo? al día siguiente raquel y angela se van de la bella isla de puerto rico. jorge y angela vienen al hotel para recoger a raquel. angela... yo sé que nos acabamos de conocer.

ojalá me perdones por lo de ayer. raquel, tienes que comprender. todo el mundo dice cosas de jorge que me irritan. mi abuela, mis amigas en el banco y ahora tú. ¿hay algo que yo no vea? eso es todo. debemos irnos. hombre: iangela! angela... me alegro mucho de encontrarte. ¿qué pasa, tío? estás muy preocupado. tienes que ir directamente a ver a tu hermano cuando llegues a méxico. ¿cómo? no comprendo. sucedió un accidente... en la excavación. ¿qué pasó? su hermano tuvo un accidente en la excavación.

captioned by the caption center wgbh educational foundation

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>> most of us learned at an early age how an apple falling from a tree inspired isaac newton to describe how the universe behaves by certain predictable rules. but what about when the universe doesn't behave so... [ thunder rumbling ] predictably?

can mathematics explain the often unpredictable behavior of the physical world, everything from the weather to the way a baseball travels through the air? welcome to chaos theory. >> jake's fastball's coming in at about 94. >> yep. >> an object at rest will remain at rest... >> unless acted upon by an external and unbalanced force. newton on your mind again? >> yep. i've always been partial to his first law of motion. >> uh-huh. a lot of forces act on a baseball: gravity, friction, turbulence. >> turbulence? >> mm-hmm. knuckleball.

some things you just can't predict. [ bat cracks ] >> still, every action has a reaction. >> pops and red are discussing an age-old dilemma: why in nature some things, like a baseball, can behave both predictably and unpredictably. and it's an exploration that began in earnest and one that used mathematics with isaac newton and his apple in the late 17th century. newton's revelation about gravity led him to define a set of rules about how the physical world operated, which he published in 1687. his laws were, in fact, so precise that they seemed to describe the world as perfectly balanced, behaving like clockwork. newton's laws would influence all the sciences, as well as the arts, religion, and philosophy, for centuries to come, essentially framing how civilized man understands the universe. the philosophical movement that

arose from newton's mathematical concepts came to be called determinism, the belief that future events are necessitated by past and present events, in combination with the laws of nature. now, some scholars even took this one step further, suggesting that once the initial conditions of the universe were set, the rest of history was inevitable. this is one of those examples where a little bit of mathematics in the wrong hands can be dangerous. but on the other hand, the ideas that there's a clockwork universe or that there's a regularity to the world as described by newton's laws is in fact something that we know to be true for much of physical phenomena. so, with his three laws of motion -- the laws of inertia, acceleration, and reciprocal actions -- newton was the first to mathematically describe how an object's motion through space and time can be calculated by adding up the infinitesimal changes in its path. in other words, newton showed us how to use mathematics to

predict an object's motion from instant to instant, given such quantities as acceleration, mass, and gravitational pull. newton's ideas were revolutionary, an entirely new way of thinking about the universe. after all, he showed us how we can use the mathematics of differential equations to predict the future. differential equations as a mathematical crystal ball. let's look at a simple example. suppose we have an object x traveling around an object y solely under the influence of gravity. then we know exactly where x will be in space 10 seconds or even 10,000 years from now. newton's theory efficiently described the interactions of what we would call a two-body system, answering the question: what occurs when the forces of two masses affect each other? now, we see the power of these ideas some 200 years later with the advent of more powerful telescopes. at that time, astronomers

noticed that some planets were not following the perfect, newtonian elliptical orbits, especially the planet uranus, so they theorized that its orbit must have been upset by some other body, and then using differential calculus, they were able to actually calculate the orbit of an unknown orb. the mathematicians said, "point your telescope here and you will find it." and so, in 1846, there it was. neptune became the first planet to be discovered based on mathematical prediction rather than mere observation. the late 19th century was, in fact, alive with such scientific triumphs, and royal prizes were offered for solutions to the most challenging mathematical problems. one such challenge was introduced by the king of sweden in 1888. he offered a prize to anyone who could solve the so-called three-body problem. in layman's terms, the king asked, "does newton's two-body solution, the simple elliptical motions of a single planet

around a massive sun, can we do the similar prediction for more than two bodies?" one of the greatest mathematicians and scientists of all time took up the king's challenge: jules henri poincare. now, poincare tried to find a closed-form solution to the famous problem, using those differential equations. again, essentially looking for a formula like one for an ellipse to describe the motion of several planets all under the influence of gravity. although poincare didn't succeed, he came close enough that the king awarded him the prize anyway, because his explorations had made a significant contribution to classical mechanics, besides adding a lot of mathematics. however, when a referee asked for a clarification, poincare discovered an error, and the great mathematician went back to the drawing board. unable to solve the problem as it was originally posed, poincare made up his own: will

the solar system always stay together or will it fall apart? what poincare discovered was that for more than two bodies, certain initial conditions could lead to chaos. you see, with two bodies and newton's equations, basically only two things could happen. either the two objects could move apart to infinity, essentially like a meteor passing by the planet, or we could get the familiar old periodic solutions of one planet orbiting around another one. and most importantly, changing the starting position slightly wouldn't change the behavior. but add some more objects to the situation, and suddenly all bets were off. other wild, non-periodic behaviors could happen, and moreover, slight cnges in the starting positions could have very different long-term effects, although roughly, the bodies would still move in approximately the same region of space. poincare's discovery was astounding, but even more, the way in which he made this discovery was at least as important as the discovery

itself. his epiphany was that the system of equations could be approached visually. to understand what poincare did, we have to understand a bit more about the problem. in classical mechanics, an object's position is recorded using its location in three dimensions: the so-called x, y, and z coordinates. when that object is moving, its velocity along each of these axes is also noted: velocity x, velocity y, and velocity z. when a second object is added to the system, six more variables must now be calculated. as additional objects are added, tracking all of the variables can be completely unwieldy, especially if the calculations are difficult. still like clockwork, just a lot of moving parts. what mathematicians call a deterministic dynamical system. what poincare saw was that if we look beyond the numbers that govern the orbits of the planet, we would find that the entire system could be viewed as a

single point moving through a multidimensional space of very high dimension. we now call this "phase space." and what the picture told him was that the system as a whole would behave unpredictably, like a leaf floating down a stream. poincare's revelations put a crack in the foundation of newton's clockwork universe and paved the way to a theory of chaos. but no one would really explain the unpredictability that poincare's calculations hinted at until midway through the 20th century, when one man stumbled on an explanation while using computers to examine a problem much more complex than three bodies moving through phase space: weather patterns on the planet earth. [ thunder rumbles ] at m.i.t. in the early 1960s, dr. edward lorenz built a simplified mathematical model of the way air moves in the earth's atmosphere. working with a 12-variable computerized weaer model, lorenz repeated a calculation

involving a numerical representation of a slightly shifting wind condition. to save computation time, he began the simulation in the middle of its course but entered the data by rounding off the original six-digit variables to just three digits, an adjustment of just one one-thousandth from the original setting. but to his surprise, the weather that the computer predicted on this new run, using these slightly different intermediate values, was completely different than his earlier simulations. lorenz expected that the miniscule difference would have practically no effect. by iterating this slightly altered calculation, lorenz realized that minute variations in the initial values in his weather model could result in widely divergent weather patterns. remember, newton showed how an object's motion through space could be predicted by calculating the infinitesimal changes in its path. now lorenz was showing that for certain equations, an infinitesimal change in the data could end in a highly

unpredictable result. that's what we mean by sensitive dependence on initial conditions: the error, the distance between the two trajectories, grows exponentially fast. the fact that small changes in initial conditions produce large changes in the long-term outcome is the trademark of a chaotic system, and it's called "sensitivity to initial conditions," or "sensitive dependence." and this process of iteration can be thought of as an amplifier, or a mechanism that reveals the sensitive dependence. using the computer, which made it possible to rapidly repeat and accumulate the infinitesimally small changes over and over again, lorenz was able to actually chart this sensitivity. the resulting graph, called the lorenz attractor, is in fact a phase-space representation of this simplified model of the weather. the graph's similarity to the shape of a butterfly caught on as a way to illustrate the concept of "sensitive

dependence." so it's a magical coincidence that we explain this by sometimes saying that a butterfly flapping its wings in china might cause an infinitesimal change in wind current that could lead to a hurricane in florida several months later: the butterfly effect. >> first butterfly of the season. kind of warms your heart, don't you think? hey, did i ever tell you about how chaos theory's connected to heart dynamics? >> think it's going to rain? >> feels humid, all right. good air for a knuckleball. >> that wouldn't have anything to do with turbulence, would it? >> well, a ball that spins, say, a fastball, if thrown correct, can take a more predictable, uh, newtonian path as it moves through the air. >> but a ball that doesn't spin? >> well, that's where celestial mechanics meets chaos theory.

>> baseball and mathematics, two great american pastimes. so we're here today with steve strogatz, author of the book nonlinear dynamics in chaos and also a professor of theoretical and applied mechanics at cornell university. and steve's going to help us make sense out of chaos on the baseball field. steve, ready? >> hey, you know, your friends pops and red are having a pretty interesting conversation out there. >> they're quite the grizzled old philosophers. >> so the thing about a knuckleball, you know, is that the pitcher grips it with two fingers in this flat part here. and the trick is to throw it so that it has very little spin. and what happens then is that the airflow around the pitch starts to create vortices, little whirlpools of air behind the ball. >> so it's actually almost pushing the ball forward, right? >> yeah, sort of pushing. well, i mean, mainly the ball has its own inertia carrying it forward, but these whirlpools do, if they're in the wake of a knuckleball, sort of push it around in a funny and unpredictable way, whereas a fastball, which would have much

more spin, has a much more predictable wake and it leads to a pitch that's more predictable, except of course it's fast. >> i mean, so a wake, so just like a boat moving through the water, you see something behind it, and that's the wake. and that's exactly what this is doing in the air. and depending on whether or not it's spinning, you get different wake patterns in the back, is that right? >> that's right. and so the chaotic wake behind the knuckleball is more turbulent and it makes the pitch less predictable in the sense that the next time the pitcher throws it, even if he just changes the angle a little bit of release or the speed, it'll end up looking like a totally different pitch. >> so that's an example of this sensitive dependence on initial conditions that we're going to be hearing about. >> right, it's chaos at work on the baseball field. just a tiny change in the pitch makes a big change by the time it crosses the plate. >> these slight changes with the knuckleball are going to affect, well, very different paths that still end up at home plate, or somewhere around home plate. >> right. yeah, that's the idea. and so what we want to try to understand a little better is how is it that something that starts like a tiny difference,

how can those tiny differences get amplified and grow and grow exponentially fast, leading to very different outcomes? and so it seems like one way that we might want to look at it is what we're showing here on the screen now. we could take a look at just doing this with numbers, okay? >> very, very simple numerical examples... >> yeah, just the number line that you've been using. right. so let's just focus on numbers, and we'll do a certain operation on the numbers, which is to -- >> so just numbers between 0 and 1. we only have that piece of the line. >> yeah, so not the whole number line. just start from 0 to 1 and pick some number in there. let's say .632. >> okay. >> okay, and you could imagine that there's more digits after that if you want, but let's just -- .632. and then we multiply by 10. this is the operation we're going to do. and so then we would get the number 6.32. and what i want to do next is an operation that a mathematician calls "mod 1," which means just drop off the number before the decimal point.

so a 6.32 would then become just .32. >> mod 1. >> okay, now what i want to do is compare that to what would have happened if we had originally started with .633, making only a difference in the one-thousandth place, right? i mean, in science, normally if you have something that's good to three digits, you'd say that's pretty good. >> i'm done. >> yeah, so but watch what happens if we do our operation on .633. then we multiply by 10, we get .33. >> right. we multiply by 10, we lop off the integer. >> yes, but that differs from our original number, not in the thousandths place, but now in the hundredths place. we've amplified the error, the difference, by 10. >> right. >> okay, and if we did this one more time... >> so we're doing both of them. we multiply them both by 10, we lop off the integer, and now we compare. and now they differ just in the tenths place, so there's another multiple of 10 in the error. >> yeah. so that's the thing that -- the difference between these two outcomes is growing by a factor of 10. it's growing exponentially fast as we go forward in time.

and that's what happens in chaotic systems. but you might think -- and so this is the other interesting point, why we need the mod -- that the error, if it kept growing exponentially, that would be like one of the baseball pitches going out of the stadium. that doesn't happen here because the mod keeps things bounded to always lie between 0 and 1. >> right, always on our little segment here. >> yeah, always stays in our segment eventually. so things can get far apart, but not too far apart, and that's what we see in chaotic systems, too. >> so this an interesting point, that, again, people think of chaos as, you know, totally unpredictable, uncontrollable. >> yeah, that's right. and the way that mathematicians use chaos, it may be not the best word for the subject in a way, because what we should think of is that there's a whole spectrum of disorder. if we keep sort of like raising the heat, you know, to wilder and wilder behavior, then you would start to see something like turbulence, where it's complicated not just in time, like chaos, but also in space. there's a counterpart to the turbulence that arises in living things -- it would really be a matter of life and death -- which is complicated behavior in

your own heart in space and time, that we call fibrillation. >> so fibrillation is actually turbulence in my heart. >> it's a kind of electrical turbulence. instead of the organized, rhythmic flow of electricity that triggers the ventricles to beat properly in sync, you find that you start to get a -- something like electrical vortices, electrical whirlpools on the heart causing different parts to beat at different times. you get uncoordinated beating, and no blood gets pumped. and you're -- when people die suddenly in, you know, a matter of minutes from cardiac arrest, that's what's happening at the electrical level. so mathematicians nowadays are just starting to work with cardiologists to try to figure out this most deadly arrhythmia, using modern-day versions of chaos theory, the cutting edge of chaos. >> i see. so a nice -- i mean, a beautiful and important intersection of mathematics and medicine. well, steve, thanks a lot. this has been a really exciting tour of chaos in all sorts of different venues, and i appreciate the tour. >> sure. thanks, my pleasure. >> so now we're going to look a little bit more closely at the

use of chaos in cardiac dynamics. when mathematicians talk about chaos theory, what they're talking about is "mild/wild," poised between metronome regularity and the craziness of turbulence. scientists have begun to explore chaos for such practical applications as the treatment of heart disease. chaos is giving us a lot of new insight into heart dynamics, helping us understand the arrhythmias that can, in the worst cases, lead to sudden cardiac death. more than 300,000 people in the united states die of cardiac arrest every year. most attacks are brought about by an abrupt change from rhythmic pumping of the heart muscle to spasmodic convulsions. scientists discovered that the unstable palpitations known as cardiac fibrillation are a form of chaos. like all chaotic occurrences, it isn't completely random. the heart can become arrhythmic because of stress, an injury, or some abnormality in the muscle tissue. the electronic impulses of the heart begin rotating in a kind

of spiral wave. this rotating disturbance can travel, its chaotic impulses circulating through the heart tissue. it may also break up into a small number of added spiral waves, all rotating and diverging, causing the system to destabilize. by using the math of chaos, researchers were able to calculate how to give small electrical pulses to test animals, and then, eventually, humans. these pulses induced premature beats which cardiologists were able to use to coerce the heart tissue back into a healthy rhythm. scientists have yet to utilize chaos in specific medical applications, but perhaps the theory will someday lead to better anti-arrhythmia drugs, gentler defibrillators, and other beneficial technologies. beyond heart dynamics and computer animation, scientists and mathematicians use chaos to explore evolutionary biology, economics, population growth, artificial intelligence, gaming and probability, even making

more efficient fuel injectors. buperhaps one of the most interesting explorations is one that takes us again into outer space. >> the interplanetary superhighway is a network of ultra-low-energy orbits generated by the five lagrange points that connect the entire solar system, and it explains how things can move back and forth using chaotic dynamics. i'm martin lo. i work as a mission designer in designing trajectories for space missions at jpl. the very specific branch of mathematics that we use to study the interplanetary superhighway is called dynamical systems theory. it gives us a very different picture of the solar system. instead of just isolated planets in near-circular orbits around the sun, this interplanetary

superhighway concept says that all the planets, the moons, the asteroid belts, the comets, the kuiper belt, they're all actually dynamically connected and linked. so even though you don't see the orbits connecting them, there's a web underneath. lagrange points are what i call the seeds of the interplanetary superhighway. they're locations where all the forces, the gravitational forces, are balanced with the rotational forces so that if you put a particle there, it would just remain there. but if you just have the slightest motion on it -- breathing on it would cause it to drift away. it's as if you were starting on street number one and then you go down, it will take you to one place, but if you start on street number two, not only will it take you to a different place, but it'll be actually to another city. so in our case, it could be

actually to another planet. starting from these lagrange points, or the equilibrium points, they generate families of periodic orbits. so these are orbits that close on themselves, and they surround the lagrange points and they get bigger, bigger, and bigger. and what happens, these are very special types of periodic orbits that are very sensitive, or people call them unstable. but this sensitive dependence is really the definition of chaos. the very first mission that used this type of very sensitive orbits, and it was called the isee-3, international sun-earth explorer 3, was launched in 1978. by using the sensitive dependence on slight changes, it was able to reorient itself, move away from the l1 lagrange point, and actually go to follow -- to study a comet.

and so it's this type of sensitivity and energy savings that makes these orbits very, very powerful. here we are in the jpl space museum, and behind me is a life-size model of the galileo spacecraft. what's really exciting for me is that even though the original design used very classical theories to come up with the trajectory, we now can show that it's actually following the pathways of the interplanetary superhighway. in terms of the future research on the concept of the interplanetary superhighway, there's really two sides. from the scientific point of view, by understanding these pathways and mapping them out, it will help us to understand how solar systems form, how the transport of material that builds life comes to the earth. on a second vein that's more practical for humans is that it will help us to find ways to fly

cheaply from a to b. it might help us to deflect, detect, and even perhaps capture rogue asteroids that might otherwise hit the earth. >> do you see that? >> you mean that shooting star? >> yeah, beautiful. >> could have come all the way out from the kuiper belt, caught the interplanetary superhighway. >> i know, i know. you and your lagrange tubes. bunch of convoluted mathematical mumbo jumbo, if you ask me. chaos theory. [ thunder rumbles ] give me old isaac newton anytime. >> you know, i don't think the weather has anything to do with clockwork. >> you wouldn't be suggesting that we're going to get rained out on account of some butterfly flapping its wings in china, would you? >> you mean the butterfly effect? nah. [ thunder rumbles ]

>> a butterfly flapping its wings in china causing a hurricane over florida might be a stretch, but mathematically, well, as we've seen, anything's possible. and maybe that butterfly is the right metaphor for mathematics and mathematicians. small discoveries over time as well as the big ones, amplified through history, done by some of the greatest thinkers of all time: pythagoras to euclid, newton, poincare, lorenz, and countless others wse journeys travel amazing intellectual trajectories through history. and with chaos, we've just begun to explore the unpredictable, on our way to perhaps discovering other superhighways of knowledge that might someday lead us to the end of the unknown. captions by lns captioning portland, oregon www.lnscaptioning.com

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