yego.me
💡 Stop wasting time. Read Youtube instead of watch. Download Chrome Extension

Physics: Are we forever trapped in the arrow of time? | Sabine Hossenfelder


3m read
·Nov 3, 2024

We need some way to explain why people only get older and not younger. But we have this big mystery in the foundations of physics because if we look at the laws for the microscopic constituents, like elementary particles, they work the same way forward in time as they do backward in time.

But the problem is we think that everything around us—us, worlds, plants, and so on and so forth—is made of those particles bouncing off each other. But we don't experience our reality as being the same forward in time and backward in time. Eggs break, but they don't unbreak. If we drop a pebble into water, you see the water splash out and the pebble sinks. People only get older but not younger.

So where does it come from if the laws work the same forward and backward? The answer to this question is that it's not just the laws themselves that matter, but it's also how the individual particles are arranged. So despite the fundamental laws of nature having this symmetry between forward in time and backward in time, we ourselves have this experience that forward in time is very different from backward in time.

And this experience is what we call the arrow of time. And we need an explanation for it. The most common explanation that physicists put forward for it is entropy increase. And entropy is a measure for the number of microstates in each macrostate. What we mean by this is that things become more and more disorderly over time.

They break, but they don't unbreak. This explains part of the reason for why the direction forward in time looks different than the direction backward in time because entropy only increases in one direction of time. Mathematically, with our equation, we can run the movie backward, but it won't look the same.

So we've said entropy always increases, and this explains why the future's different from the past. But it brings up a new problem because entropy can only increase if it was small to begin with. Indeed, the entropy must have been very small in the beginning of the universe; otherwise, we wouldn't be here today.

So what does the arrow of time have to do with us aging? At first sight, you could say, well, that's all about biology; it's all about cell processes. There are lots of scientists who are trying really hard to slow down the process of aging, and now you physicists come and try to tell them it's not possible.

It's certainly true that there are cell processes that determine how we age, and it's really, really complicated. And I admit that I'm totally not competent to talk about it. I'm just a physicist. But it is possible to fend off entropy increase for some amount of time in a particular part of a system.

For example, there are certain creatures, like types of lobsters or maybe trees, that can keep entropy increase very low for a certain amount of time at the expense of increasing entropy elsewhere. Some species are better at this than others. Maybe in the future, we'll be able to slow down aging.

Maybe we'll be able to live 100,000 years or maybe a billion years. But you can't do it for the entire universe. So entropy will eventually increase, and it'll get us in the end. This brings up the question: is this how the universe will end?

This question has captured the imagination of a lot of science fiction writers. The most famous example might be Isaac Asimov. In his short story, "The Last Question," Isaac Asimov envisions a man asking a computer—today we might say an artificial intelligence—if there's any way to stop the entropy from increasing in the universe.

For a long time, billions of years, the answer of this computer and its more sophisticated later versions is that it has incomplete information for an answer. At the very end, when all the stars have burned out and the only beings that remain are completely disembodied consciousnesses that float through the universe, the computer finishes the calculation and says, "Let there be light."

So how will it end? For me, the answer is we don't really know.

More Articles

View All
Principles for Success “Be Radically Open-Minded” | Episode 7
Principles for Success: An Ultra Mini-Series Adventure in 30 Minutes and in Eight Episodes Episode 7: Be Radically Open-Minded Taking risks and occasionally being ruined wasn’t acceptable, and neither was not taking risks and not having exceptional resu…
What is Dark Matter and Dark Energy?
Matter, as we know it: atoms, stars and galaxies, planets and trees, rocks and us. This matter accounts for less than 5% of the known universe. About 25% is dark matter; and 70% is dark energy, both of which are invisible. This is kind of strange because …
Common denominators: 1/2 and 1/3 | Math | 4th grade | Khan Academy
You have two fractions: 1⁄4 and 5⁄6, and you want to rewrite them so they have the same denominator and have whole number numerators. What numbers could you use for the denominator? So here’s our fractions: 1⁄4 and 5⁄6, and we want to rewrite these fract…
Warren Buffett: "Rule #1: Never lose money. Rule #2: Never forget rule #1."
Warren Buffett: The first rule of investment is: Don’t lose. And the second rule of investment is: Don’t forget the first rule. And that’s all the rules there are. I mean, if you buy things for far below what they’re worth, and you buy a group of them, yo…
How to Use Khan Academy's Free Courses for Texas Teachers and Students
To share valuable free resources with you today that I believe will not only benefit your students but also lighten your load as you manage the many decisions and tasks that come along with teaching nowadays. I really truly appreciate everything that you …
Worked example: finite geometric series (sigma notation) | High School Math | Khan Academy
Let’s take, let’s do some examples where we’re finding the sums of finite geometric series, and let’s just remind ourselves in a previous video we derived the formula where the sum of the first n terms is equal to our first term times 1 minus our common r…