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Earth Is Almost 20 Galactic Years Old
The Sun takes approximately 230 million years to orbit the Milky Way. In its 4.54-billion-year history, Earth has completed roughly 20 Galactic orbits.
- Orbit 1: Earth and Moon form.
- Orbit 2: LUCA, our last universal common ancestor, may have lived around 4.2 billion years ago.
- Orbit 5: Ancient microbial life.
- Orbit 10: Great Oxidation Event.
- Orbit 13: Early eukaryotic cells.
- Orbit 18: Cambrian explosion.
- Orbit 19: First dinosaurs.
- Orbit 20: Dinosaur extinction, evolution of humans, and the present day.
Human civilization occupies only a tiny fraction of Earth's twentieth journey around the Milky Way.
Nearly 20 Galactic years. One remarkable planetary history.
We often picture the Sun motionless at the centre of the Solar System. But the Sun moves too.
Every planet gravitationally influences the Sun. Jupiter's mass alone shifts the Sun–Jupiter barycentre beyond the Sun's visible surface. The entire Solar System has a constantly moving centre of mass called the Solar System Barycentre.
The Sun and planets move around this shared centre of mass. Sometimes the barycentre lies inside the Sun; sometimes it lies in empty space beyond its surface.
This is the same gravitational reflex motion astronomers use to detect giant exoplanets around distant stars.
The Sun is not fixed at the centre. It is part of the orbital dance.
The Sun is not travelling through empty space. As it orbits the Milky Way, it moves through the local interstellar medium, while continuously releasing a stream of charged particles called the solar wind. This magnetized wind pushes against the surrounding interstellar environment, creating an enormous bubble around the Sun and its planets: the heliosphere.
The solar wind travels outward at hundreds of kilometres per second. Far beyond Neptune, it encounters the pressure of the interstellar medium and slows abruptly at the termination shock. It then flows through a turbulent region called the heliosheath, before reaching the heliopause, where the solar wind's outward pressure is balanced by the surrounding interstellar pressure. Beyond this boundary, neutral hydrogen can accumulate in a region known as the hydrogen wall. The heliosphere may also have an extended tail, although its precise shape remains an active area of research.
Only two spacecraft have directly crossed the heliopause. Voyager 1 crossed in August 2012 at approximately 122 AU, and Voyager 2 followed in November 2018 at approximately 119 AU. By November 2026, they had travelled roughly 172 AU and 144 AU from the Sun, respectively. Their measurements provide our first direct observations of the boundary between the Sun's plasma environment and interstellar space.
The heliosphere does not stop every galactic cosmic ray, but it does reduce the number reaching the inner Solar System. It is a dynamic magnetic environment that helps shape the radiation conditions around our planetary neighbourhood.
Happy Birthday Dr Carl Sagan ✍️
92 years ago today, the universe produced a man who would spend his life helping us understand it.
Carl Sagan didn't just study the cosmos. He gave it to us.
The scientist;
He helped show that Venus is a runaway greenhouse world, a warning written in the clouds of our nearest neighbour. He studied the seasonal changes on Mars and the hazy organic chemistry of Titan, and he played key roles in the Mariner, Viking, Voyager and Galileo missions.
The messenger;
He helped compose humanity's first messages to the stars: the Pioneer plaques and the Voyager Golden Record. Two golden discs carrying our music, our languages and our greetings are still drifting beyond the Sun's reach. They may outlast every city on Earth.
The conscience;
In 1990 he persuaded NASA to turn Voyager 1 around for one last look home. From 6 billion kilometres away, Earth appeared as a single pale blue pixel suspended in a sunbeam. That image changed how we see ourselves. Every border, every war, every human story fits inside that tiny dot.
The teacher;
"Cosmos" carried science into hundreds of millions of homes. "The Dragons of Eden" won a Pulitzer Prize. "The Demon-Haunted World" handed us a candle in the dark: scepticism, evidence and wonder, held together.
The guardian of our future;
He warned the world about nuclear winter and climate change long before most were listening. He believed our survival depends on wisdom keeping pace with our technology, and that reaching for the stars and caring for our home planet are the same act of love.
His greatest gift;
He taught us that science is not cold. It is the most profound way we have of feeling at home in the universe. We are made of star-stuff, and through us the cosmos has begun to understand itself.
Thank you, Carl, for looking up and taking all of us with you.
The pale blue dot still remembers you.
In 2012, the Large Hadron Collider found the Higgs boson. In the fourteen years since, it has found nothing else new. Was it a failure?
Before the LHC switched on, many physicists expected more. The Higgs mass is fragile: quantum effects should push it to enormous values unless something cancels them. The favourite candidate, supersymmetry, predicted a family of new particles close to the Higgs. The LHC searched for them. They weren't there.
Now Europe must decide what comes next. In May 2026, the CERN Council recommended a 91-kilometre ring, the Future Circular Collider. It would first collide electrons with positrons to measure the Higgs with extreme precision, then perhaps later host a proton collider at far higher energy. Governments decide whether to build it around 2028.
Critics say the old prediction rested on a sense that nature should look "natural", an aesthetic preference rather than evidence, so a bigger machine guarantees nothing. Supporters reply that measuring the Higgs precisely is guaranteed knowledge, and that only experiment can say where new physics hides.
Underneath is an older question: when you look carefully and find nothing, have you failed, or have you learned something true about nature?
What Does a Quantum Particle's Wavefunction Look Like?
A quantum wavefunction is not simply an ordinary wave oscillating up and down. It is a complex-valued mathematical function. Its real and imaginary parts can be visualized as two perpendicular oscillations, forming a rotating helix when plotted together. This is a representation of quantum phase, not the physical shape of a particle.
For a free, non-relativistic particle, the dispersion relation is ω(k) = ℏk²/2m. Its wavepacket travels at the group velocity, twice the phase velocity. Because different momentum components travel at different speeds, a localized Gaussian wavepacket spreads over time: σ(t) = σ₀√[1 + (t/τd)²].
This mathematics has experimental foundations. Electron diffraction, C₆₀ fullerene interference and ultracold atomic gases demonstrate the wave nature and evolution of quantum matter. What we observe experimentally are interference patterns and probability distributions, not the wavefunction itself.
How big is the black hole in M87?
In 2019, the Event Horizon Telescope measured its mass at 6.5 billion Suns (EHT Collaboration, ApJL 875, L6). Its event horizon works out to about 38 billion km across, roughly 1.5 light-days.
For scale: our whole planetary neighbourhood, Neptune and Pluto included, would sit comfortably inside it. Voyager 1 has been flying for 49 years and is only now approaching a distance of one light-day from Earth. It would still be crossing.
And it doesn't sit quietly. Its surroundings launch a jet visible for 5,000 light-years, first spotted in 1918 by Heber Curtis as "a curious straight ray". Its physical nature only began to become clear decades later.
Horizon size assumes no spin; rotation changes its size and geometry. Disk and jet shapes are illustrative.
A ball can move along a straight path, yet someone watching from a rotating platform may see it follow a curve. The difference is not in the ball's motion, but in the reference frame used to observe it.
In this visualization, the red trajectory represents motion in an inertial frame, while the blue curve illustrates how that same motion appears to an observer rotating with the platform. In the rotating frame, the apparent acceleration includes Coriolis and centrifugal effects. The Coriolis acceleration depends on both the platform's angular velocity and the object's velocity relative to it.
The same principle operates on Earth. Because our planet rotates, moving air and ocean currents experience Coriolis deflection, helping shape large-scale atmospheric circulation. What appears to be a sideways acceleration can arise simply because the observer is rotating.
Light has no rest mass, yet gravity can bend its path. The remarkable part is that light can follow the straightest possible path through spacetime while appearing to curve around a massive object.
Just as a glass lens bends light through refraction, a massive body bends light through a fundamentally different mechanism: the curvature of spacetime. In General Relativity, light follows paths called null geodesics. Both the geometry of space and the behavior of time contribute to its deflection, revealing how gravity changes the paths along which light travels.
Two pure qubit states pointing in opposite directions on the Bloch sphere are perfectly distinguishable by an appropriate measurement. States whose Bloch vectors are separated by a right angle have a different relationship: prepare one, then measure in a basis containing the other, and that outcome occurs with 50% probability.
The equation P = (1 + cos θ)/2 connects this probability to the angle between their Bloch vectors. Identical directions give probability one; opposite directions give zero. The sphere represents quantum states, rather than positions in space. Its geometry tells us how preparation and measurement fit together, turning the angle between two arrows into an experimentally testable prediction.
A square wave can emerge from the sum of smooth circular motions. By projecting odd Fourier harmonics (n = 1, 3, 5, …) onto the real axis, their combined oscillations gradually approximate the sharp transitions of a square wave.
Each added harmonic brings the waveform closer to its ideal shape. The sound you hear is generated directly from the same mathematical sum, S_N(t), turning Fourier's mathematics into an audible signal.
Richard Feynman on the Beauty of the Stars✍️.
Does knowing what the stars are made of take away their beauty? Feynman thought the opposite. On a desert night he saw the same stars as any poet, and felt them, but he also knew his eye was catching light that had left them a million years before. To him the scientific picture made the sky bigger, not smaller.
Gravity creates five special locations in the Sun–Earth system where a small object can maintain the same position relative to both bodies as they orbit.
These are called Lagrange points. L1, L2, and L3 lie along the Sun–Earth line, while L4 and L5 form equilateral triangles with them. In the rotating reference frame, gravity and the centrifugal effect balance at these locations.
The James Webb Space Telescope orbits around L2 rather than remaining exactly at the point. This geometry allows it to stay near Earth while maintaining a favorable position for observing the universe.
A rotating complex number becomes a helix when time is represented as a third dimension. Viewed from two perpendicular directions, the same motion reveals sine and cosine.
This is Euler’s formula made geometrical, e^(iωt) = cos(ωt) + i sin(ωt).
Why can't we predict the future forever, even when the laws of physics are exact?
Imagine 1,000 double pendulums starting with angular differences as small as 0.0001°. Initially, their motions appear identical. But as time passes, tiny differences grow rapidly, eventually producing completely different trajectories.
This is deterministic chaos. Through sensitive dependence on initial conditions, small uncertainties can grow approximately as e^(λt), where λ is the Lyapunov exponent. The equations remain deterministic, but long-term prediction becomes practically impossible.
In the final lecture of his 1964 Cornell series, Richard Feynman raised an interesting question. It went something like this: how can we study just one small part of nature, discover a mathematical law, and then use it to predict what happens in places we have never explored?
What fascinated him was that observations made within a limited region could tell us something about the unknown. Near the end of the lecture, Feynman acknowledged that he did not know why this was possible. His answer was philosophical rather than scientific. He thought it might have something to do with the simplicity and beauty of nature. For Feynman, the remarkable thing was not merely that we could discover physical laws, but that these laws could reveal something about parts of nature we had never observed.
What happens if chaos continues for billions of years?
Surprisingly, some systems can eventually return arbitrarily close to their initial states, no matter how unpredictable their motion becomes.
Poincaré's Recurrence Theorem establishes this for almost all trajectories in bounded, measure-preserving systems. Related quantum recurrences can occur under suitable conditions.
If the universe itself is a finite, isolated quantum system, similar recurrences might occur over unimaginably long timescales. But this remains theoretical, and whether the universe satisfies those conditions is unknown.








