Latest / Talking Science / The Cosmic Distance Ladder – How We Measure the Universe
Transcript
- 0:00So picture yourself for a second standing right
- 0:02on the edge of a wide, just incredibly deep river
- 0:06gorge. Okay, I'm picturing it. And you're looking
- 0:08out and there is this specific tree on the far
- 0:11bank. You really want to know exactly how far
- 0:14away that tree is. Right. But there's a massive
- 0:16problem. You can't just walk across and pace
- 0:19it out, right? And you can't, like, stretch a
- 0:22tape measure over open air and 100 meters of
- 0:24rushing water? Obviously not. You are completely
- 0:27stuck on your side of the cliff. Welcome to our
- 0:30deep dive for today, by the way. I'm your host,
- 0:32and today we're looking at an article about how
- 0:35human beings actually measure the vastness of
- 0:37the universe. And I'm your resident astronomy
- 0:40expert. Yeah, that feeling of being stuck on
- 0:43one side of an uncrossable gap. That is the exact
- 0:46position humanity is in every single time we
- 0:49look up at the night sky. Because we want to
- 0:50know how big the universe is. Exactly. We want
- 0:53to know how far away things are. But we are permanently
- 0:55stranded on Earth. We just we can't stretch a
- 0:58tape measure to the stars. But if you know just
- 1:01a little bit of geometry, you don't actually
- 1:03need to cross that gorge. You can just walk a
- 1:06short measured distance along your own side of
- 1:09the cliff. Right, which we would call a baseline.
- 1:11Right. So you measure the angle to the tree from
- 1:13the start of your walk. Then you walk, say, 10
- 1:16paces. And you measure the angle to the tree
- 1:19from the end of your walk. Suddenly you have
- 1:21a triangle. And simple trigonometry hands you
- 1:24the distance across the water. No crossing required.
- 1:27It's so cool. It really is. And that simple geometric
- 1:30trick, using a known baseline and a couple of
- 1:34angles to find a distance you can't measure directly,
- 1:37that is the seed of one of the greatest achievements
- 1:40in modern astronomy. Which is what they call
- 1:42the cosmic distance ladder, right? Yeah, exactly.
- 1:44It's the exact system astronomers use to figure
- 1:47out the distance to almost everything in the
- 1:48cosmos. From, you know... our own moon out to
- 1:52galaxies so ancient their light has been traveling
- 1:54toward us since before the earth even formed
- 1:56wow okay let's unpack this because climbing that
- 1:59ladder is basically our mission for this deep
- 2:02dive if you want to understand how we measure
- 2:04the universe without prior astronomy knowledge
- 2:06you really have to understand this ladder and
- 2:09it really is a ladder Because no single measurement
- 2:12method works at every scale of the universe.
- 2:14You literally have to climb rung by rung. Right.
- 2:17Each new technique you use is calibrated against
- 2:20the one right below it, which lets you reach
- 2:22further and further out. Exactly. I mean, if
- 2:24everything relies on the step below it, we have
- 2:26a chicken and egg problem. To measure the tree
- 2:28across the gorge, I had to walk 10 paces. I had
- 2:31to, like, establish a physical baseline. If we
- 2:34are stuck on Earth... How do we get that very
- 2:37first baseline to start measuring space? Well,
- 2:40we just bounce a signal off our neighbors. Wait,
- 2:42really? Yeah. The absolute bottom run of the
- 2:45ladder doesn't rely on starlight at all. It relies
- 2:47on radar. Oh, like air traffic control. Exactly
- 2:50like that. We use the exact same basic mechanism,
- 2:54but astronomers aim it at solid planets within
- 2:57our solar system. You send out a burst of radio
- 3:00waves into space toward Venus or Mars, and you
- 3:03just wait for the echo to return to Earth. So
- 3:05we are just timing the echo. Yep, because we
- 3:08know how fast radio waves travel. They travel
- 3:10at the speed of light, which is a fixed universal
- 3:12constant. It never changes. Okay, so if I send
- 3:15a radio burst to Venus and it takes exactly,
- 3:18say, four minutes for the echo to hit my receiver,
- 3:21I can just do the simple math to figure out the
- 3:23total distance of that round trip. Right. And
- 3:25because these measurements are direct and physical,
- 3:28they give us these rock solid distances within
- 3:30our own solar system. Like we can measure the
- 3:33distance to Venus down to a matter of meters.
- 3:35That's insane. Down to meters. Yeah. But if we
- 3:38connect this to the bigger picture, the real
- 3:40power of this radar trick isn't just knowing
- 3:42where Venus is. If we map out the distances to
- 3:45the other planets, we can use the laws of gravity
- 3:48to perfectly calculate the exact size of the
- 3:51Earth's orbit around the sun. OK, I see. So we
- 3:54use. the radar to figure out the distance from
- 3:56the earth to the sun and i know there's a technical
- 3:58term for that right yeah that specific distance
- 4:01is called an astronomical unit you got it And
- 4:04so that single number, that astronomical unit,
- 4:07that becomes the baseline for the next rung up
- 4:10on our ladder. Yes. We use the entire Earth's
- 4:13orbit to recreate your trick at the River Gorge.
- 4:16Which brings to mind a trick a lot of us played
- 4:18with as kids. Oh, the finger trick. Yeah, the
- 4:21finger trick. If you're listening, you can do
- 4:22this right now. If you hold your finger up right
- 4:24in front of your face and you close one eye.
- 4:27and then open and close the other eye, your finger
- 4:29seems to jump left and right against the background
- 4:31of the room. It's a great analogy. And the closer
- 4:34your figure is to your face, the bigger that
- 4:36apparent jump is. Right. And astronomers call
- 4:39that apparent shift parallax. It happens anytime
- 4:42you view the same object from two slightly different
- 4:45positions. For your finger, the two positions
- 4:47are your left eye and your right eye. And for
- 4:50a star. For a star, astronomers use the Earth's
- 4:53orbit. they look at a nearby star in january
- 4:56then they wait six months until july by july
- 5:01the earth has traveled hundreds of millions of
- 5:03kilometers to the complete opposite side of the
- 5:05sun so january is one eye and july is the other
- 5:09eye exactly and the background of the room is
- 5:11the field of much more distant essentially fixed
- 5:14stars when they look at the target star again
- 5:17in july it appears to have shifted slightly against
- 5:21that background. Wow. And because the radar measurements
- 5:24gave us the exact diameter of the Earth's orbit,
- 5:26we know the exact length of our baseline. We
- 5:29measure the angle of the star's shift, and geometry
- 5:32hands us the distance to the star. It's incredibly
- 5:35elegant. Because you don't need to know anything
- 5:37about the star itself. You don't need to know
- 5:39how bright it is or how hot it is. It's just
- 5:41pure math. It's just triangles, yeah. But stepping
- 5:43back for a sec, when you look at the sheer scale
- 5:46of what they're trying to measure, it seems kind
- 5:48of impossible. The shift they're looking for
- 5:50isn't like a finger jumping across a wall. It
- 5:52is staggeringly small. It is very, very small.
- 5:55The source mentions we are talking about a fraction
- 5:57of an arc second. To put that into human terms
- 5:59for you listening. Observing that shift is roughly
- 6:02equivalent to trying to measure the width of
- 6:04a single human hair viewed from several kilometers
- 6:07away. Yeah, it's wild to think about. Trying
- 6:10to do that from the surface of the Earth, looking
- 6:12up through our blurry, turbulent atmosphere,
- 6:15it seems like a nightmare. And it was, was a
- 6:17massive limiting factor for a long time. The
- 6:20atmosphere constantly distorts the light, which
- 6:22meant we could only use parallax for a few thousand
- 6:24of the very closest stars. To get past the blur,
- 6:28you have to leave the atmosphere. So in 2013,
- 6:31the European Space Agency launched a space observatory
- 6:34called Gaia. Oh, I've heard of Gaia. Yeah. By
- 6:37operating in the vacuum of space, Gaia has been
- 6:39able to precisely map the positions and parallax
- 6:41shifts of well over a billion stars. It pushed
- 6:45reliable geometric measurements out from a tiny
- 6:47local bubble to distances of many thousands of
- 6:50light years. A billion stars. That is just, I
- 6:54mean, that's incredible. But even with Gaia.
- 6:56In space, there has to be a physical limit to
- 6:59this, right? Yeah. The universe is massive. Yeah,
- 7:01there absolutely is a limit. Because if a star
- 7:04is millions of light years away, the angle of
- 7:07that shift eventually becomes so infinitesimally
- 7:10small that no telescope could ever measure it.
- 7:13The geometry math just breaks down. We need a
- 7:16new rung. We do. When geometry runs out, we have
- 7:19to start judging distance by brightness. Which
- 7:21means we run into the campfire problem. The campfire
- 7:23problem, exactly. Imagine you are standing in
- 7:26a dark field at night and you see a light in
- 7:28the distance. How do you know if you are looking
- 7:30at a massive bonfire 10 miles away or like a
- 7:34tiny matchstick just one mile away? You don't.
- 7:37Right, they might look exactly the same brightness
- 7:39to your naked eye. In astronomy, the solution
- 7:42to that campfire problem is finding what we call
- 7:44a standard candle. A standard candle, okay. Yeah,
- 7:47the whole trick of a standard candle is finding
- 7:49an object in space where we somehow already know
- 7:51its true intrinsic brightness. If we know exactly
- 7:54how many watts of light a star is pumping out
- 7:57and we measure how dim it appears from Earth,
- 7:59the laws of physics tell us exactly how far that
- 8:01light had to travel to fade by that amount. I
- 8:04see. But getting that intrinsic brightness is
- 8:06the hard part, isn't it? We can't just fly out
- 8:09to a star to check its wattage. How do we know
- 8:12the true brightness of a star we've never been
- 8:14to? Well, the breakthrough came from a rather
- 8:16unassuming type of star known as a Cepheid variable.
- 8:20It's named after the constellation Cepheus, where
- 8:22an early one was spotted. Okay, a Cepheid variable.
- 8:25What does it do? A Cepheid isn't a static star
- 8:28like our Sun. It rhythmically brightens and dims
- 8:31over a period of days or weeks. It is literally
- 8:34pulsating. Its outer layers physically expand
- 8:38and contract. Oh, wow. So it's basically a giant.
- 8:41cosmic blinking light. Pretty much. And the way
- 8:44we cracked the code on these blinking lights
- 8:45goes back to an astronomer named Henrietta Leavitt
- 8:48at the Harvard College Observatory in the early
- 8:5020th century. Right. She was studying photographs
- 8:52of thousands of these pulsating cepheid stars
- 8:55in a specific cluster called the Small Magellanic
- 8:58Cloud. And her choice to study that specific
- 9:01cloud, that is the brilliant part. And unlocked
- 9:03everything. Because the small Magellanic cloud
- 9:06is a dwarf galaxy orbiting our own. So since
- 9:09all the stars Leavitt was studying were packed
- 9:11together in that one distinct cloud, she could
- 9:14safely assume they were all roughly the exact
- 9:16same distance from Earth. Oh. Which isolates
- 9:20the variable. Oh, exactly. If she sees two blinking
- 9:24stars in that cloud and one looks brighter than
- 9:27the other, she knows it isn't because it's closer
- 9:29to Earth. It has to be genuinely intrinsically
- 9:32brighter. Right, and she realized the rhythm
- 9:34tells you the brightness. She discovered a mathematically
- 9:37consistent rule called the period -luminosity
- 9:40relationship. Basically, the longer a cepheid
- 9:43takes to pulsate, The slower its blinking rhythm,
- 9:46the more intrinsically luminous the star actually
- 9:49is. So a slow blink means a massive bright star.
- 9:53A fast blink means a smaller, dimmer star. That
- 9:56is such an elegant key to the universe. It's
- 9:58beautiful physics. But how do we put it on the
- 10:01ladder? Like, we know the rule now, but we still
- 10:03need a hard distance to calibrate it. We use
- 10:05the rung below. Astronomers looked for cepheid
- 10:08variables that were close enough to Earth that
- 10:10we could measure their distance using the parallax
- 10:12geometry we just talked about. The parallax gave
- 10:14us the exact distance. Knowing the exact distance
- 10:17allowed us to calculate the exact intrinsic brightness
- 10:20of those nearby cepheids. And that calibrated
- 10:24Henrietta Leavitt's rule. Wow. And once it's
- 10:27calibrated, parallax doesn't matter anymore.
- 10:29Not at all. We can look deep into space, find
- 10:31a completely new cepheid. Time its blink, use
- 10:34leave its math to find its true brightness and
- 10:37just calculate the distance. And this was the
- 10:39exact tool Edwin Hubble used in the 1920s to
- 10:43change our entire understanding of reality. It
- 10:45really was. Because before Hubble, people saw
- 10:48these fuzzy patches of light in the night sky
- 10:50and assumed they were just gas clouds inside
- 10:52the Milky Way. They thought the Milky Way was
- 10:55the entire universe. Which is funny to think
- 10:57about now. Right. But Hubble found cepheids inside
- 11:00those fuzzy patches, timed their blanks, and
- 11:03realized those patches were entirely separate
- 11:05galaxies, located millions of light years away.
- 11:07The universe got unimaginably bigger overnight.
- 11:10It was a profound paradigm shift. But just like
- 11:14with parallax, Cepheids eventually hit a wall.
- 11:17As we try to measure galaxies billions of light
- 11:20years away, individual pulsating stars just fade
- 11:24from view. Too far away to see the blink. Exactly.
- 11:27Even our best telescopes can't pick out a single
- 11:29Cepheid in a galaxy halfway across the observable
- 11:32universe. So we need a brighter candle. We need
- 11:34an explosion. Yes, we do. Which brings us to
- 11:37the next rung on the ladder. A specific kind
- 11:39of stellar detonation called a Type Ia supernova.
- 11:43Right. And these are some of the most violent
- 11:45events in the cosmos. A Type Ia supernova starts
- 11:48with a white dwarf. Okay, remind me what a white
- 11:51dwarf is. A white dwarf is essentially the dense,
- 11:54compact corpse of a star that was once similar
- 11:56to our sun. Imagine this dense white dwarf is
- 11:59locked in a tight orbit with a normal living
- 12:01companion star. Because the white dwarf has such
- 12:04intense gravity, it starts siphoning gas off
- 12:07its companion. Oh man, so it acts like a cosmic
- 12:09vampire just constantly feeding off the other
- 12:11star? That's a good way to picture it. But it
- 12:14can't just gorge itself forever, right? A star's
- 12:17core can only support so much weight. before
- 12:21gravity crushes it exactly there is a very specific
- 12:24physical threshold as the white dwarf pulls more
- 12:27and more gas onto itself its mass increases eventually
- 12:30it approaches a critical mass limit and then
- 12:33what the moment it hits that exact threshold
- 12:36the core can no longer support its own weight
- 12:39The white dwarf collapses inward, triggering
- 12:41a runaway thermonuclear explosion. The entire
- 12:44star detonates. The whole thing. And because
- 12:46that detonation is triggered at the exact same
- 12:48mass limit every single time, the resulting explosion
- 12:51is almost exactly the same size every single
- 12:53time. Right. The physics dictate that the bomb
- 12:55always has the exact same yield. It creates a
- 12:58thermonuclear flashbulb so bright it can briefly
- 13:01outshine an entire galaxy of 100 billion stars.
- 13:05And because they are phenomenally bright and
- 13:07incredibly consistent, Type Ia supernovae are
- 13:09the ultimate standard candles. We can spot them
- 13:12in galaxies billions of light years away, far
- 13:14beyond the reach of any individual cepheid star.
- 13:16But wait, so what does this all mean for the
- 13:19latter? Every rung has to connect. We know the
- 13:22supernova explodes at a specific mass, but we
- 13:26don't automatically know its exact brightness
- 13:28in watts. True. We have to calibrate the flashbulb.
- 13:31which means we have to wait for a type E supernova
- 13:34to go off in a galaxy that is close enough to
- 13:37us that we can also measure the Cepheid variables
- 13:40in that same galaxy. And that is the defining
- 13:43vulnerability of the entire cosmic distance ladder.
- 13:46The supernovae are calibrated by the Cepheids.
- 13:49The Cepheids are calibrated by parallax. Parallax
- 13:52is calibrated by radar. Nothing stands alone.
- 13:55It's a house of cards. Basically. If we made
- 13:57a tiny math error decades ago calculating the
- 13:59distance to Venus with radar, that error propagates
- 14:03up. It corrupts the parallax, which corrupts
- 14:05the cepheids, which means our entire map of the
- 14:07deep universe is wrong. Tell me cosmologists
- 14:10don't just rely on this one single fragile ladder.
- 14:13Oh, they don't. That house of cards scenario
- 14:14keeps scientists away at night. I bet. So they
- 14:17build independent backup methods to cross -check
- 14:19the wrongs. For instance, there is a principle
- 14:21called the Tully -Fisher relation. What's that?
- 14:23This rule links how fast an entire spiral galaxy
- 14:26is spinning to how intrinsically bright the whole
- 14:30galaxy is. If you can measure the rotation speed,
- 14:33you can estimate the galaxy's brightness and
- 14:35therefore its distance without needing to isolate
- 14:38individual stars at all. Okay, that makes me
- 14:41feel better. And there is another backup called
- 14:42the tip of the red giant branch. The tip of the
- 14:45red giant branch? Yeah. This looks at populations
- 14:48of aging stars. Right before an old star undergoes
- 14:52a specific internal change in how it burns helium,
- 14:55it hits a very sharp, predictable peak in brightness.
- 14:59That peak acts as an alternative standard candle.
- 15:03Ah, I see. Because these backup rungs generally
- 15:06agree with the suffades and the supernovae, astronomers
- 15:08have a high degree of confidence that the latter
- 15:11is fundamentally sound. That's reassuring. So
- 15:14we have our ladder. We can measure out to the
- 15:16deepest reaches of space. But what if we want
- 15:18to measure the expansion of the space itself?
- 15:21Then we need a new trick. Right. And to do that,
- 15:23we have to look at how light behaves when an
- 15:25object is moving away from us. If you are standing
- 15:29on a sidewalk and an ambulance speeds past you,
- 15:32the pitch of the siren Sounds higher as it approaches
- 15:35and then visibly drops to a lower pitch as it
- 15:38speeds away. The Doppler effect. Yeah, the Doppler
- 15:41effect. The sound waves get stretched out as
- 15:43the vehicle recedes. And light does the exact
- 15:45same thing. When a galaxy is moving away from
- 15:47us, the light waves it emits get stretched out.
- 15:50In the visible spectrum of light, longer wavelengths
- 15:53look red. Okay. So as the light stretches, its
- 15:56color shifts toward the red end of the spectrum.
- 15:59Astronomers call this redshift. Redshift. And
- 16:01in the 1920s, Edwin Hubble. the same guy who
- 16:04used cepheids to discover other galaxies, he
- 16:06started measuring the redshift of those galaxies.
- 16:08He was a busy guy. Seriously. He compared how
- 16:10far away a galaxy was to how stretched out its
- 16:13light was, and he found a direct link. He discovered
- 16:16what we now call Hubble's Law. The further away
- 16:19a galaxy is from us, the faster it is receding.
- 16:22To visualize why this is happening, imagine taking
- 16:25a deflated balloon and drawing a bunch of dots
- 16:27all over it with a marker. Each dot represents
- 16:30a galaxy. Now start blowing up the balloon. As
- 16:34the rubber expands, every single dot gets further
- 16:37away from every other dot. The dots aren't actively
- 16:41crawling across the surface. The rubber itself
- 16:43is stretching, carrying the dots with it. That
- 16:46is what space is doing. It is expanding in all
- 16:49directions. And because Hubble's law ties distance
- 16:52directly to redshift, it becomes a powerful tool.
- 16:55If you can measure how stretched out a galaxy's
- 16:58light is, you instantly know how fast it is moving
- 17:00and roughly how far away it is. Which sets up
- 17:03one of the biggest plot twists in modern physics.
- 17:06Oh, yeah, this is a big one. In the late 1990s,
- 17:08teams of astronomers were using our ultimate
- 17:10standard candles, the type Ia supernovae, to
- 17:14measure distances to very remote galaxies. But
- 17:17the data came back weird. The distant supernovae
- 17:20were noticeably dimmer than they should have
- 17:21been. And everyone at the time assumed the expansion
- 17:24of the universe was either coasting at a steady
- 17:27speed or gradually slowing down due to the inward
- 17:30pull of gravity. But the math didn't lie. The
- 17:33supernovae were dimmer. But if they're dimmer
- 17:35than expected, it means they're further away
- 17:37than expected. Yes. What's fascinating here is
- 17:41the only way the math works is if the expansion
- 17:43of the universe isn't slowing down. It is actively
- 17:46accelerating. Space is stretching faster and
- 17:49faster every single day. It's like throwing a
- 17:52baseball up into the air. And instead of slowing
- 17:54down and falling back to Earth, it suddenly rockets
- 17:56upward into the sky. It defies gravity. Exactly.
- 17:59This discovery proved there must be a mysterious
- 18:02force driving this acceleration, a force we now
- 18:05call dark energy. And the astronomers who figured
- 18:08this out won a Nobel Prize, all because they
- 18:11trusted the upper rungs of the distance ladder
- 18:12enough to spot a discrepancy. And that brings
- 18:16us to the ultimate prize in cosmology, the Hubble
- 18:19Constant. The Hubble Constant. OK. Yeah, this
- 18:22is a specific number that represents the exact
- 18:24rate at which the universe is expanding today.
- 18:27If we can pin down the precise value of the Hubble
- 18:31constant, we can run the clock backwards to calculate
- 18:34the exact age of the universe. Oh, wow. And we
- 18:37can run the clock forwards to predict its ultimate
- 18:39fate. Okay, here's where it gets really interesting.
- 18:42This is the great mystery we promised at the
- 18:44start of this deep dive. We currently have two
- 18:47independent ways to measure the Hubble constant.
- 18:51And they refuse to agree. They stubbornly refuse.
- 18:54And this conflict has been tearing at the astrophysics
- 18:56community for a decade. Let's look at the two
- 18:59methods. First, you have the local or late universe
- 19:03method. Right, which is everything we just talked
- 19:05about. Building the ladder from the ground up.
- 19:07Radar, parallax, cepheid, supernovae. Exactly.
- 19:10Measuring the redshift of galaxies directly around
- 19:12us. Teams have refined this ladder to a razor
- 19:15sharp edge. And then you have the second method.
- 19:18The top -down early universe approach. This method
- 19:21completely ignores the latter. Instead, it looks
- 19:23at the cosmic microwave background. What is that
- 19:25exactly? When the universe was born in the Big
- 19:28Bang, it was incredibly hot and dense. About
- 19:31380 ,000 years later, it cooled just enough for
- 19:34the first atoms to form, and light was finally
- 19:37able to travel freely through space. So it's
- 19:40the literal afterglow of the Big Bang, the oldest
- 19:42light in existence. Yes. We use space satellites
- 19:45like ESA's Planck satellite to map the tiny microscopic
- 19:49temperature variations in that ancient radiation.
- 19:52By looking at the physics of that baby universe,
- 19:54scientists can plug that data into our standard
- 19:57model of cosmic evolution, mathematically run
- 20:00the clock forward 13 .8 billion years, and predict
- 20:03exactly what the Hubble constant should be today.
- 20:06Okay, so we have a bottom -up measurement using
- 20:08exploding stars today and a top -down measurement
- 20:11calculating forward from the oldest light. in
- 20:13existence. Both methods have been checked, double
- 20:16checked and triple checked by the smartest people
- 20:17on Earth. They have. But when you compare the
- 20:19final numbers, they don't match. They disagree
- 20:22by about 10 percent. Ten percent. Yeah. And in
- 20:24the world of precision cosmology, a 10 percent
- 20:27gap is a massive, statistically significant chasm.
- 20:30It is well outside the margin of error for either
- 20:33team. This discrepancy is known as the Hubble
- 20:36tension. The Hubble tension. So who messed up?
- 20:39There has to be a math hair somewhere, right?
- 20:41Maybe a smudge on a telescope lens or like a
- 20:44flaw in how we calibrate the cepheid variables.
- 20:47I mean, it could be. A lot of scientists are
- 20:50desperately hunting for a hidden human error
- 20:52or systematic bias in the instruments. But there
- 20:55is another alternative, and it is what cosmologists
- 20:58are taking very seriously right now. What if
- 21:00nobody messed up? Right. What if both measurements
- 21:03are perfectly correct? The bottom -up ladder
- 21:05is accurately measuring the universe today. The
- 21:08top -down calculation is accurately measuring
- 21:10the baby universe. Okay, but if both are true,
- 21:13it means our standard model of the universe is
- 21:15broken. It means we are missing a completely
- 21:18new piece of physics. There is a hidden ingredient
- 21:20out there, perhaps something we don't understand
- 21:22about how dark energy behaves over time, that
- 21:25we haven't discovered yet. Man, that is wild.
- 21:28So to bring this all together for you listening,
- 21:30we started this journey... just trying to figure
- 21:33out how to measure a tree across a river gorge.
- 21:36And look where we ended up. Right. We built a
- 21:38ladder of geometry and pulsating stars and exploding
- 21:41white dwarfs, and we ended up standing at the
- 21:44absolute edge of known physics. From bouncing
- 21:47radar off Venus to mapping the oldest light in
- 21:50existence, the cosmic distance ladder is the
- 21:53ultimate detective story. It really is a living,
- 21:56breathing mystery. And this Hubble tension isn't
- 21:59a failure of science. It's a thrilling reminder
- 22:01that the universe still has massive fundamental
- 22:05secrets waiting to be uncovered in the dark.
- 22:07The book of physics is far from finished. It
- 22:10really is far from finished. And I want to leave
- 22:12you with one final thought to mull over today,
- 22:13building on that massive cliffhanger. If both
- 22:17of these measurements, the baby universe and
- 22:19the modern universe, are completely accurate,
- 22:21what if the hidden ingredient we are missing
- 22:23is that the fundamental laws of physics themselves
- 22:25have actually changed over the last 13 billion
- 22:27years? Ooh, I love that. What if the universe's
- 22:30measuring stick is actively evolving along with
- 22:33the universe itself? It definitely makes you
- 22:35look at that rushing river gorge in a whole new
- 22:38light.