A star can be characterized as a system driven far from equilibrium by a steady flow of energy through it. The energy comes from both nuclear and gravitational potential energy, which is slowly converted into starlight in a range of frequencies. The starlight then illuminates the surfaces of planets, like ours, driving them into far-from-equilibrium states of their own.
This is an example of a general principle: Flows of energy through open systems tend to drive them to states of higher organization. (“Open systems,” recall, are any bounded systems that can exchange energy with their surroundings.) We can call this the principle of driven self-organization. If the principle of sufficient reason is the paramount explanatory principle in nature and the identity of the indiscernibles her prince, the principle of driven self-organization is the good angel who does the detailed work in myriads of stars and galaxies to ensure a diverse, complex universe.
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A ubiquitous feature of such self-organizing systems is that they are stabilized by feedback mechanisms. Any living thing is an intricate network of feedback processes that regulate, channel, and stabilize the flows of energy and material through it.
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Patterns in space and time are formed when different feedback mechanisms compete to control a system. When a positive-feedback mechanism competes with a negative-feedback mechanism but they act on different scales, you may get patterns in space.
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[O]ur present universe is characterized by structure and complexity on a wide range of scales, from the organization of molecules in living cells to the organization of galaxies into clusters. There is a hierarchy of self-organizing systems, driven by energy flows and stabilized and shaped by feedback processes.
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What do we see when we look back? We see a universe evolving from less to more structured, from equilibrium to complexity.
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[I]f we consider the solar system as an isolated system, the fact that parts of it are undergoing self-organization is compatible with an overall increase of its entropy. The system as a whole is trying to come to equilibrium and will increase its entropy where it can. The second law is doing its best to drive the solar system to equilibrium, but as long as there’s a big star radiating hot photons into cold space, that equilibrium is postponed. While it’s postponed, molecules can ride the energy flow to greater and greater states of organization and complexity. And stars burn for billions of years, so there’s lots of time for complexity to proliferate. The existence of stars has much to do with why the universe is far from equilibrium almost 14 billion years after its formation.
But why are there stars? If the universe must tend toward entropy and disorder, how is it that stars, which drive the universe away from equilibrium, are ubiquitous? To put this another way: If the universe is to be Leibnizian, something like stars must exist. What features of the laws of nature guarantee that they do?
The physics of stars relies on two unusual features of the laws of nature. The first is incredibly fine tuning in the parameters that govern physics. These fine tunings include the masses of the elementary particles and the strengths of the four forces. They make nuclear fusion possible, so the hydrogen gas comprising a star does not behave as it would in the absence of nuclear forces. Rather than just moving around randomly, the hydrogen atoms jammed together at the center of a star can interact in a new way. They fuse to make helium and a few other light elements. It’s as if you were trapped in a cell, day after day, in the same boring equilibrium. Every hour is like every other. Then all of a sudden a door opens where there was none before, and you escape into a whole new world. The laws of thermodynamics applied to generic atoms would never predict nuclear fusion and the possibilities it gives rise to.
The second unusual feature has to do with the behavior of systems held together by the force of gravity. Very simply, gravity subverts our naïve ideas about thermodynamics.
An everyday observation, which is also a consequence of the second law of thermodynamics, is that heat flows from hotter bodies to colder bodies. Ice melts. Water on the stove boils. Heat stops flowing when the temperature of the two bodies is the same; they have reached the state of equilibrium. Normally when we take energy out of a body, its temperature goes down, and when we put energy into a body, it heats up. So when heat flows from a hotter body to a colder body, the latter heats up and the former cools down. This goes on until they’re at the same temperature. This is why the air in a room is at a single temperature. If it weren’t, energy would flow from the warmer side to the cooler until they reached a common temperature.
This behavior makes the system in equilibrium stable against the effects of small fluctuations. Suppose, by a small fluctuation, one side of a room became a bit warmer than the other. Energy would flow from the warm side, cooling it, to the cooler side, warming it, so that soon the temperature is uniform again. Most systems work in this intuitive way. But not all.
Imagine there’s a gas that works the other way, cooling down when you add energy to it and heating up when you take energy away. This may seem counterintuitive, but there are such gases. They have to be unstable. Suppose you start off with all of this kind of gas in a room at the same temperature. A little fluctuation moves a bit of energy from the left side to the right. Then the left side heats up, while the right side cools down. This causes more energy to flow from the left side, the hot side, to the cold side. As it does, the left side won’t cool down; rather, it gets even hotter. And as more energy flows into the cool right side, that side gets even cooler. Soon you have a runaway instability, in which the two sides of the room are driven to continually increase their temperature difference.
Now let’s look at just the hot side and repeat the scenario. Suppose another fluctuation appears, cooling the center of the hot side a bit. The same phenomenon acts as positive feedback to further cool the center and further heat the region around it. As time goes on, the little fluctuation grows into a feature. This can happen again and again. Soon you have a complex pattern of cold and hot regions.
A system that works this way naturally drives itself to form complex patterns. It’s hard to predict where such systems will end up, because there are a huge number of heterogeneous, patterned configurations it might evolve toward. We call these anti-thermodynamic systems. The second law still operates in them, but because putting energy into a region cools it down, the state in which the gas is uniformly distributed is highly unstable.
Systems held together by gravity behave in this crazy way. Stars, solar systems, galaxies, and black holes are all anti-thermodynamic. They cool down when you put energy into them. This means that all these systems are unstable. The instabilities drive them away from uniformity and stimulate the formation of patterns in space and time.
This has a lot to do with why the universe is not in equilibrium 13.7 billion years after its origin. The increasing structure and complexity that characterize the universe’s history are largely explained by the fact that the gravitationally-bound systems filling it, from clusters of galaxies to stars, are anti-thermodynamic.
It’s easy to understand why such systems are anti-thermodynamic. Two basic features differentiate gravity from the other forces: The gravitational force is (1) long-range and (2) universally attractive. Consider a planet in orbit around a star. If you put energy in, it will move to an orbit farther from the star, where it moves slower. So putting energy in decreases the speed of the planet, and this lowers the system’s temperature — because temperature is just the average speed of things in the system. Conversely, if you take energy out of the solar system, the planet must respond by falling closer to the star, where it moves faster. Hence, taking energy out heats up the system.
We can compare this with the behavior of an atom, which is held together by the electric force between charges. Like gravity, the electric force acts over long distances, but it differs by being attractive only between opposite charges. A positively-charged proton will attract a negatively-charged electron, but once the electron is bound to the proton the resulting atom has no net charge. The force is said to saturate, and the atom does not attract any other particles to it. A solar system works the opposite way, because when a star attracts some planets, the resulting system is even more attractive to passing bodies than the star alone would have been. So here’s another instability — a gravitationally-bound system will attract still more bodies to it.
This anti-thermodynamic behavior manifests itself in the devolution of star clusters. If a star cluster were to act thermodynamically, it would reach equilibrium — in this case, a state in which all its stars had the same average speed and stayed clustered forever. Instead, what happens is that a star cluster slowly dissipates. This happens in an interesting way. Every once in a while a star comes close to a double star — that is, two stars in orbit around each other. A close approach can result in a narrower orbit for the double star. This orbital shrinking releases energy, which is imparted to the third star. The third star now has enough energy to escape the cluster, and it begins a journey off into space. After a long time, little is left of the star cluster except some double stars in close orbits and a cloud of fast-moving stars streaming away from the cluster.
This does not contradict the second law, only a naïve interpretation of it. The law that entropy should usually increase just codifies the truism that the more ways there are for something to happen, the more likely it is that it will. Normal thermodynamic systems end up in the single, boring state of uniform equilibrium; gravitationally-bound, anti-thermodynamic systems end up in one of a large number of highly heterogeneous states.
So the fact that our universe is interesting has a threefold explanation: The principle of driven self-organization acts over a myriad of subsystems and scales, from the molecular to the galactic, evolving them to states of ever increasing complexity. The engines driving that process are the stars, which exist because of a combination of the fine tuning of the fundamental laws and the anti-thermodynamic nature of gravity. But these forces can produce a universe filled with stars and galaxies only if the initial conditions of the universe are strongly time-asymmetric.