Module 26: Space & the Solar System

Planets, distances, and cosmic scale

Part A · the Sun -- the star at the centre
The Sun -- our star

Diameter

1,392,700 km -- 109× Earth's diameter

Mass

1.989 × 10³⁰ kg -- 333,000× Earth's mass

Surface temperature

~5,500°C (corona: 1–3 million °C -- hotter than surface, still unexplained)

Distance from Earth

~150 million km = 1 AU. Light travel time: 8 min 20 sec.

Composition

~74% hydrogen, ~25% helium, 1% heavier elements

Age / remaining life

4.6 billion years old. ~5 billion years of hydrogen fuel remaining.

The Sun contains 99.86% of all mass in the solar system. Its gravity holds everything from Mercury to the Oort Cloud (~2 light-years away). The Sun is a G-type main-sequence star -- perfectly average by stellar standards, which is fortunate: massive stars burn fast and go supernova.
The Sun's internal layers
Core 0–25% of radius · ~15 million °C
Nuclear fusion occurs here: 4 hydrogen nuclei fuse into 1 helium nucleus, releasing enormous energy as gamma rays. The core fuses ~620 million tonnes of hydrogen per second. Density is ~150 g/cm³ -- 150× water.
Radiative zone 25–70% of radius · ~7 million °C
Energy from the core travels outward as photons, but the plasma is so dense that photons are constantly absorbed and re-emitted -- a single photon takes 100,000–170,000 years to cross this zone. This is why sunlight you see today was "created" at the Sun's core over 100,000 years ago.
Convective zone 70–100% of radius · ~2 million → 5,500°C
Heat is transported by convection -- hot plasma rises, cools at the surface, sinks back down in giant cells. Granules (convection cells ~1,000 km wide) are visible at the surface, each lasting ~10 minutes. The Sun's surface (photosphere) is the visible "surface" we see from Earth.
Photosphere 500 km thick · ~5,500°C
The visible surface. Sunspots are cooler regions (~3,800°C) where intense magnetic fields suppress convection -- they appear dark only by contrast. Sunspot activity follows an 11-year cycle that affects space weather on Earth.
Chromosphere & Corona Above surface · up to 3 million °C
The chromosphere (pink during solar eclipses) extends ~2,000 km above the photosphere. The corona -- the Sun's wispy outer atmosphere -- extends millions of km and is inexplicably hotter than the surface. The solar wind originates here: a stream of charged particles that fills the solar system and drives auroras on Earth.
The Sun in context -- stellar classification (Morgan–Keenan)
O-type -- Blue supergiant (e.g. Rigel)
50× Sun's mass, 300,000× luminosity. Burns fuel in just millions of years. Ends as a supernova.
30,000–50,000 K
B-type -- Blue-white (e.g. Spica)
2–16× Sun's mass. Very bright, short-lived. Responsible for much of a galaxy's UV output.
10,000–30,000 K
A-type -- White (e.g. Sirius, Vega)
1.4–2× Sun's mass. Sirius is the brightest star in our night sky. Too short-lived for complex life to evolve.
7,500–10,000 K
F-type -- Yellow-white (e.g. Procyon)
~1.2× Sun's mass. Slightly hotter and shorter-lived than the Sun. Some are in habitable zone candidates.
6,000–7,500 K
G-type -- Yellow dwarf ← The Sun (also: Alpha Centauri A)
~1× solar mass. Long-lived (~10 billion years). Stable output. Our Sun is 4.6 Gyr old, halfway through its life. Ideal for complex life.
5,200–6,000 K
K-type -- Orange dwarf (e.g. Epsilon Eridani)
0.5–0.8× Sun's mass. Dimmer but very long-lived. Increasingly considered top candidates for life-hosting systems.
3,700–5,200 K
M-type -- Red dwarf (e.g. Proxima Centauri)
Most common star type (~75% of all stars). 0.08–0.5× solar mass. Extremely long-lived (trillions of years). Prone to intense flares that may sterilise nearby planets.
2,400–3,700 K
Part B · the planets -- interactive explorer
Scale visualisation -- relative planet sizes (not to orbital distance scale)
Mer
Ven
Ear
Mar
belt
Jupiter
Saturn (rings not shown)
Uranus
Neptune
Inner planets (Mercury–Mars) shown at 10px per Earth diameter. Gas giants scaled at ~1/11th for fit. If Jupiter were truly to scale relative to Earth above, it would be 1,120px wide.
Planetary comparison -- diameter relative to Earth
Bar width proportional to diameter. Earth = 12,742 km baseline.
Part C · beyond the planets -- the outer solar system

Asteroid belt

Between Mars and Jupiter (~2.2–3.2 AU)

Millions of rocky objects, but total mass only ~4% of Earth's Moon. Despite depictions in films, space between asteroids averages hundreds of thousands of km -- the Voyager probes passed through without incident. Ceres (diameter 940 km) is the largest and is classified as a dwarf planet.

Dwarf planets

Pluto, Eris, Ceres, Makemake, Haumea

Pluto (reclassified in 2006) orbits at ~39 AU, takes 248 years per orbit, has 5 moons including Charon (half its size). Eris is slightly larger than Pluto -- its discovery triggered the dwarf planet debate. IAU definition: orbits the Sun, roughly spherical, but has NOT cleared its orbital neighbourhood.

Kuiper Belt

30–50 AU -- beyond Neptune

A disc of icy objects, the remnants of solar system formation. Contains Pluto, Eris, and thousands of other objects. Short-period comets originate here (those with orbital periods under 200 years). 20× wider than the asteroid belt but 20–200× more massive.

Oort Cloud

~2,000–100,000 AU -- the edge of the solar system

A vast spherical shell of icy bodies surrounding the solar system. Long-period comets (orbital periods thousands to millions of years) originate here. Never been directly observed -- inferred from comet trajectories. Its outer edge (~100,000 AU = ~1.6 light-years) is roughly halfway to the nearest star.

Part D · Earth's Moon -- everything worth knowing

Distance from Earth

384,400 km

Light: 1.3 sec. Varies: 356,500 (perigee) to 406,700 km (apogee)

Diameter

3,474 km

27% of Earth's. Largest moon relative to its planet (except Charon/Pluto)

Orbital period

27.3 days

Sidereal (relative to stars). Lunar month (new moon to new moon): 29.5 days

Rotation period

27.3 days

Same as orbital period -- tidally locked. We always see the same face.

Tidal locking -- why one face only
Earth's gravity created tidal bulges in the Moon's crust. These bulges created a drag that gradually slowed the Moon's rotation over billions of years until rotation period exactly matched orbital period. Now perfectly synchronised -- the far side ("dark side" is a misnomer -- it gets as much sunlight as the near side, just never faces us) was unseen until Soviet Luna 3 photographed it in 1959.
Tides -- the Moon's gravitational pull
The Moon's gravity pulls Earth's oceans (and to a tiny extent, land) toward it. As Earth rotates, different points pass through this tidal bulge -- creating high and low tides (~2 per day). The Sun also creates tides (~46% the strength). When Sun, Moon, and Earth align (new/full moon): spring tides (highest). When at right angles: neap tides (lowest range).
The 8 lunar phases -- one complete cycle = 29.5 days
New Moon
Day 0 -- invisible.
Waxing crescent
Days 1–6. Right side lit.
First quarter
Day 7. Right half lit.
Waxing gibbous
Days 8–13. Mostly lit.
Full Moon
Day 14–15. Fully lit.
Waning gibbous
Days 16–21. Left side lit.
Last quarter
Day 22. Left half lit.
Waning crescent
Days 23–29. Sliver left.
The Moon's movement through space is complex: It orbits Earth (27.3 days). Earth + Moon orbit the Sun together (365.25 days). The Moon's path around the Sun is always convex -- it always curves toward the Sun, never loops backward, despite appearances. The Moon is also very slowly drifting away from Earth at ~3.8 cm/year (measured by laser retroreflectors left by Apollo missions).
Part E · Earth's atmosphere -- the five layers
From the ground to space -- altitude and what happens at each level
Exosphere 700 km to ~10,000 km
The outermost layer -- atmosphere so thin it merges imperceptibly into interplanetary space. Molecules can escape Earth's gravity. Satellites in very high orbits (GPS: ~20,200 km) orbit here. No weather phenomena. Temperature "definition" breaks down -- molecules travel huge distances between collisions.
Thermosphere 80–700 km
ISS orbits here (~400 km). Temperature rises dramatically with altitude (up to 2,500°C) -- but air is so thin there are almost no molecules to transfer heat. Auroras (Northern/Southern Lights) occur here -- solar wind particles excite atmospheric atoms. Re-entry vehicles experience intense heating here from air compression.
Mesosphere 50–80 km
Temperature drops to −90°C at the mesopause (top) -- coldest natural temperature on Earth. Most meteors burn up here (friction with air molecules). Noctilucent clouds form near the top at ~82 km -- rare, beautiful electric-blue clouds of ice crystals, only visible at twilight. Too high for aircraft, too low for satellites -- the "ignorosphere."
Stratosphere 12–50 km
Contains the ozone layer (~15–35 km) which absorbs UV radiation -- essential for life on Earth. Temperature increases with altitude here (the opposite of the troposphere) because ozone absorbs UV energy. Very dry, no weather. Commercial aircraft fly at ~10–12 km (just below/at the tropopause). Concorde flew at ~18 km in the lower stratosphere. Weather balloons reach ~30–40 km.
Troposphere 0–12 km (8 km at poles, 16 km at equator)
All weather happens here. Contains ~75% of the atmosphere's mass and ~99% of its water vapour. Temperature decreases ~6.5°C per km. Mount Everest (8,849 m) is near the top. Beyond the tropopause (the boundary), temperature stops falling -- this inversion "caps" convection and prevents weather systems from penetrating into the stratosphere.
The Kármán line (100 km) is the internationally recognised boundary of space -- the point where the atmosphere is too thin for aircraft to generate lift and orbital mechanics take over.
Part F · key space distances -- the numbers you need
Distances from Earth's surface -- drag to explore
Part G · the universe's composition -- what everything is made of
Composition of the observable universe
Observable Universe
Dark energy -- 68%
Dark matter -- 27%
Ordinary matter -- 5%
Of that 5% ordinary matter…
Intergalactic gas
~72%
Intragalactic gas & dust
~18%
Stars
~8%
Everything else
(planets, you, etc.)
<1%
Everything you can see, touch, and measure -- all galaxies, stars, planets, people, and light -- accounts for just ~5% of the universe's total energy content. Dark matter doesn't interact with light (we detect it only via gravity). Dark energy is the name given to the force driving the universe's accelerating expansion. Both are among the deepest unsolved problems in physics.
The cosmic calendar -- if the universe's age were one year
Carl Sagan's concept: compress 13.8 billion years into 1 calendar year. Each second = ~437 years.
Jan 1
Big Bang -- the universe begins
13.8 billion years ago. Time, space, and all matter created. Temperature: 10³² K. Cosmic inflation expands the universe by a factor of 10²⁶ in a fraction of a second.
Jan 22
First stars ignite
~13.5 billion years ago. Population III stars -- enormous, metal-free, extremely short-lived. Their explosions seeded the universe with heavier elements forged in stellar cores.
Mar 16
Milky Way begins to form
~12 billion years ago. The Milky Way is relatively old as galaxies go -- it has been assembling via mergers for most of cosmic history. Its central supermassive black hole (Sagittarius A*, 4 million solar masses) likely formed early.
Sep 2
Sun and solar system form
4.6 billion years ago. A giant molecular cloud collapses. The Sun ignites. Planets form from the protoplanetary disc within ~100 million years. Earth's Moon forms from a giant impact with a Mars-sized body (the "Theia" hypothesis) within the first ~50 million years.
Sep 14
First life on Earth appears
~4 billion years ago. Microbial life (likely chemosynthetic bacteria) in ancient oceans. Life appeared remarkably quickly after Earth cooled enough to have liquid water -- within the first ~500 million years.
Dec 17
Cambrian explosion
540 million years ago. Multicellular animal life diversifies explosively. Most major animal body plans appear in the fossil record within ~20 million years.
Dec 25
Dinosaurs go extinct (K-Pg event)
66 million years ago. Chicxulub impactor (~10 km diameter) hits the Yucatán Peninsula. 75% of all species extinct. Mammals diversify into the vacated ecological niches.
Dec 31
11:59:59
All of recorded human history
The last ~10,000 years (agriculture, writing, all civilisations, the entire scientific enterprise) occupies the final 23 seconds of the cosmic year. Modern Homo sapiens (~300,000 years old) appears at 11:58:43 pm. You exist in the final fraction of a second.
Part H · landmark space missions -- 10 missions that changed everything
Part I · SpaceX -- the private space revolution
Founded 2002 by Elon Musk with $100 million of his own capital
SpaceX entered an industry dominated by governments and legacy contractors, with the explicit goal of making humanity multiplanetary. Its core innovation was vertical integration (building almost everything in-house) and reusability -- the two factors that have driven launch costs from ~$50,000/kg (Space Shuttle) toward a target of <$100/kg with Starship. As of 2025, SpaceX conducts more orbital launches per year than all other countries combined.
Launch vehicles
Key missions & programmes
Part J · interactive calculators -- from other modules
Module 07 · Time & Scale
Your age on other planets
Enter your birthdate and see how old you'd be if you'd lived on Mars, Jupiter, or any other planet.
Module 01 · Weight & Mass
Your weight across the solar system
See how many kilograms you'd register on the surface of every planet and the Moon, scaled by surface gravity.
Part K · beyond the solar system -- stars, galaxies, and the cosmos
Our nearest stellar neighbours
4.24 ly
Proxima Centauri -- the closest star to the Sun
A red dwarf (M-type) only 0.12% as luminous as the Sun. Hosts Proxima b, a potentially rocky planet in the habitable zone. However, red dwarfs emit intense flares that could strip away atmospheres. Part of the Alpha Centauri triple system. At current spacecraft speeds (~17 km/s) it would take ~73,000 years to reach.
4.37 ly
Alpha Centauri A & B -- the two bright companions
A binary pair (G-type and K-type) orbiting each other every 80 years. Alpha Centauri A is nearly identical to our Sun. The brightest star in the southern sky (Rigil Kentaurus). Breakthrough Starshot aims to send a laser-propelled probe there at 20% the speed of light -- arrival in ~20 years.
5.96 ly
Barnard's Star -- the fastest-moving star in the sky
A red dwarf moving at such high apparent speed across the sky that its position measurably shifts within a human lifetime. It will become our closest neighbour in ~10,000 years. Has a candidate super-Earth Barnard's Star b (contested). Its rapid motion was used historically to calculate its distance precisely.
8.58 ly
Sirius -- the brightest star in the night sky
A white A-type star 2.1× the Sun's mass and 25× its luminosity. Has a white dwarf companion (Sirius B) -- what remains after a star more massive than the Sun exhausted its fuel. Despite being the brightest star as seen from Earth, it is not particularly special; it just happens to be relatively close.
10.5 ly
Epsilon Eridani -- one of the youngest nearby stars
Only ~800 million years old (vs the Sun's 4.6 billion). Has a confirmed planet (Epsilon Eridani b) and a debris disc similar to a young solar system. Featured extensively in science fiction -- the destination of humanity's first interstellar colony ship in Arthur C. Clarke's novels.
The Milky Way -- our galaxy in numbers
Scale
100,000–120,000 light-years diameter. ~1,000 light-years thick at the disc. Our Sun sits in the Orion Arm, ~26,000 light-years from the galactic centre.
Contents
100–400 billion stars. Estimated 100 billion planets. Central supermassive black hole: Sagittarius A* (~4 million solar masses). Dark matter halo extends ~260,000 light-years.
Structure
A barred spiral galaxy. The bar at the centre (~27,000 ly long) channels gas into the core. Four main spiral arms. Orbits its own centre once every ~225 million years (one "galactic year" = 225 Myr).
Our motion
The Sun orbits the galactic centre at ~230 km/s. The Milky Way itself moves at ~630 km/s toward the Great Attractor. The entire Local Group is also falling toward the Virgo Supercluster.
Milky Way cross-section -- our position
Centre
0 ly
Sagittarius
Arm
Sun ☉
26,000 ly
Perseus
Arm
Edge
60,000 ly
The Sun is not at the centre -- it sits in a relatively quiet suburban region of one of the Milky Way's minor spiral arms. This is likely important for life: the galactic centre is a violent environment of intense radiation, frequent supernovae, and gravitational disruption.
Types of galaxies -- from spirals to ellipticals
Exoplanets -- planets beyond the Solar System
As of 2025, over 5,700 exoplanets have been confirmed. The methods used to find them reveal how different -- and how common -- planetary systems are.
The cosmic distance ladder -- how we measure the universe
Astronomers cannot use a single method for all distances. Instead they build a hierarchy of overlapping techniques, each calibrated against the one below it.
Radar ranging Up to ~2 AU
Bouncing radio waves off nearby planets and measuring the round-trip time gives exact distances in the inner Solar System. Used to calibrate the Astronomical Unit precisely to within metres.
Stellar parallax Up to ~10,000 light-years
As Earth orbits the Sun, nearby stars appear to shift slightly against background stars. The angle of shift reveals distance geometrically. The Gaia spacecraft measured parallax for over 1 billion stars with extraordinary precision.
Cepheid variable stars Up to ~100 million light-years
Cepheid stars pulsate with a period precisely linked to their intrinsic luminosity. Measure the period, know the true brightness, compare to apparent brightness, and you have the distance. Henrietta Swan Leavitt discovered this relationship in 1908, unlocking the scale of the universe.
Type Ia supernovae Up to ~10 billion light-years
White dwarf stars that explode after accreting enough mass always reach the same intrinsic peak brightness -- a "standard candle." This allowed astronomers to discover in 1998 that the expansion of the universe is accelerating (earning a Nobel Prize in 2011), implying the existence of dark energy.
Cosmic Microwave Background / Hubble's Law Billions of light-years
The universe's expansion means distant galaxies are redshifted in proportion to their distance (Hubble's Law: v = H₀ x d). The CMB maps the entire observable universe as it was 380,000 years after the Big Bang. Together these fix the universe's age at 13.8 billion years and size at 93 billion light-years (diameter of the observable universe).
Part K (i) · black holes -- in detail
What is a black hole?
A black hole is a region of spacetime where gravity is so extreme that nothing -- not even light -- can escape once it crosses the event horizon. They are not "vacuum cleaners" that suck in matter from afar; at any distance beyond the event horizon, a black hole's gravity is no different from any other object of the same mass. Their power lies in their compactness.
Formation
Stellar black holes form when a massive star (more than ~20-25 solar masses) exhausts its nuclear fuel. The core collapses in a fraction of a second -- no longer able to support its own weight -- while the outer layers explode as a supernova. The collapsed core, if massive enough, becomes a black hole rather than a neutron star.
Schwarzschild radius
Every mass has a theoretical Schwarzschild radius: compress that mass within this radius and it becomes a black hole. For the Sun: ~3 km. For Earth: ~9 mm. For a human body: ~10⁻²⁵ m (far smaller than an atomic nucleus). The radius scales linearly with mass.
Types of black holes
Stellar-mass
~3 to ~100 solar masses
Formed from dying massive stars. Thousands exist in the Milky Way. The first confirmed: Cygnus X-1 (1972). Detectable via X-ray emissions from accreting material.
Intermediate-mass
100 to ~100,000 solar masses
Long theorised but hard to confirm. First strong evidence found in globular clusters and dwarf galaxy nuclei. The "missing link" between stellar and supermassive black holes.
Supermassive
1 million to 66 billion solar masses
Found at the centres of almost all large galaxies. Our own: Sagittarius A* (4 million solar masses). The largest known: TON 618 (66 billion solar masses). How they form remains an open question.
Primordial (theoretical)
Any mass -- even sub-gram
Hypothetical black holes formed from density fluctuations in the very early universe, before stars existed. Could explain dark matter. Searched for via gravitational lensing -- none confirmed yet.
Anatomy of a black hole -- layers from outside in
Click a region to learn more. Distances shown are for a stellar black hole of ~10 solar masses (Schwarzschild radius ~30 km).
Accretion disc / jets Thousands to millions of km out
Inner accretion disc ~300–3,000 km
ISCO -- innermost stable circular orbit ~90 km (3× rs)
Photon sphere ~45 km (1.5× rs)
★ Event horizon ~30 km (rs)
Ergosphere (rotating BH only) Inside EH for Kerr BH
Singularity (theoretical) r = 0 (mathematically)
Select a region above to explore it
Each zone of a black hole has radically different physics. The event horizon is where Einstein's general relativity predicts a "point of no return" for in-falling matter and light.
Milestones in black hole observation
1915
Einstein's general relativity predicts extreme spacetime curvature
Karl Schwarzschild derived the first exact solution to Einstein's field equations within weeks of their publication -- describing the geometry of spacetime around a point mass. He found the mathematical feature we now call the event horizon, though the physical interpretation took decades.
1972
Cygnus X-1 -- first strong black hole candidate confirmed
An X-ray binary system in which a compact invisible object (too massive for a neutron star) accretes material from a companion star, emitting X-rays. Stephen Hawking famously bet Kip Thorne in 1974 that it was NOT a black hole -- and conceded in 1990.
2015
First gravitational wave detection -- LIGO hears two black holes merge
The merger of two stellar black holes (29 and 36 solar masses) 1.3 billion light-years away was detected as a spacetime ripple lasting 0.2 seconds. The signal matched general relativity's prediction perfectly. This opened gravitational wave astronomy as an entirely new way to observe the universe.
2019
First image of a black hole's shadow -- M87*
The Event Horizon Telescope (a planet-sized radio array) imaged the shadow of M87* -- a 6.5 billion solar mass black hole 55 million light-years away. The glowing ring of superheated gas matched theoretical predictions. In 2022, the same team imaged Sagittarius A*, the Milky Way's own central black hole.
Ongoing
Hawking radiation -- still undetected but theoretically critical
In 1974, Stephen Hawking showed that black holes must slowly emit thermal radiation due to quantum effects near the event horizon -- eventually evaporating entirely. For stellar black holes, the temperature is ~60 nanokelvin, undetectable in practice (cooler than the CMB), but the principle has profound implications for the "information paradox": what happens to the information about everything that fell in?
Part K (ii) · wormholes -- in detail
What is a wormhole?
A wormhole (formally: an Einstein-Rosen bridge) is a hypothetical tunnel through spacetime connecting two separate points in space or time. While they emerge from valid mathematics in general relativity, no wormhole has ever been observed, and enormous physical obstacles exist to their creation or traversability. They are not science fiction -- they are legitimate solutions to Einstein's equations -- but whether they can exist in nature remains one of physics' open questions.
Key distinction: All wormholes that appear in Einstein's equations are fundamentally unstable and non-traversable in their basic form. Making them traversable requires "exotic matter" with negative energy density -- a form of matter that may not exist, or may only exist in tiny quantities via the Casimir effect.
Anatomy of a traversable wormhole (Thorne-Morris model, 1988)
The Morris-Thorne wormhole is the physicists' favourite toy model -- mathematically well-defined, physically informative. Toggle each section to understand what the theory actually says.
🌌
Mouth A -- entry point (e.g. our region of space)
Appears as a spherical opening suspended in space. To a distant observer it would look like a warped, lensed image of wherever the other mouth is -- you would see the other end of the universe as if looking through a glass sphere. Tidal forces near the mouth are theoretically kept survivable for a sufficiently large wormhole.
⏱️
The throat -- minimum radius
The narrowest point of the tunnel. This is where time dilation is most extreme. For a traversable wormhole, the throat must remain open -- held apart by something. Gravity alone would collapse it instantly. The transit time through the throat can, in theory, be made shorter than the light-travel time between the two mouths in normal space -- this is what makes wormholes potentially useful for faster-than-light travel (or closed timelike curves).
⚛️
Exotic matter requirement -- the fatal obstacle
To keep the throat open, the wormhole requires "exotic matter" -- material with negative energy density that threads the throat and exerts a repulsive gravitational effect. The Casimir effect (a quantum phenomenon) demonstrates that negative energy densities are physically possible in tiny amounts, but the quantities required for a macroscopic wormhole are astronomically large. This is the central reason physicists believe traversable wormholes are probably impossible in practice, even if allowed in theory.
🌠
Mouth B -- exit point (another location or time)
Could in principle be anywhere in the same spacetime: billions of light-years away, or in a different region of the same galaxy. More provocatively, general relativity also permits the two mouths to be connected to different times -- a wormhole whose mouths are moved at relativistic speeds relative to each other (or placed in different gravitational potentials) would experience different rates of time, creating a potential time machine. This is what led Kip Thorne to publish the 1988 wormhole paper: a graduate student asked if time machines were possible, and the answer turned out to be: yes, IF wormholes exist AND can be traversed.
Types of wormholes -- from Einstein-Rosen to ER=EPR
Wormhole vs. black hole -- key differences
Black hole
One-way. Once you cross the event horizon, you cannot leave -- not even information can escape. General relativity predicts a singularity at the centre where density becomes infinite and current physics breaks down. Black holes are confirmed to exist via multiple independent lines of evidence. They destroy information (possibly -- this is the "information paradox").
Wormhole
Hypothetically two-way (if traversable). Both mouths have horizons in the non-traversable Schwarzschild case, but a traversable wormhole requires the exotic matter to prevent horizon formation. Information is preserved -- it exits the other mouth. Wormholes have never been observed. The ER=EPR conjecture (2013, Maldacena and Susskind) proposes that quantum entanglement and wormholes may be the same phenomenon -- connecting quantum mechanics and general relativity in a profound way.
The chronology protection conjecture: Stephen Hawking proposed that the laws of physics conspire to prevent wormholes from being used as time machines -- quantum fluctuations near the wormhole throat would build up catastrophically, destroying the wormhole before it could be exploited for backwards time travel. This remains unproven but is consistent with our observation that we have not been visited by time travellers.
Part L · Q&A

1. Venus is closer to Earth than Mars, yet Mars has been visited by more spacecraft. Why is Mars a better destination for exploration?

Venus is hellish in ways Mars is not. Venus's surface temperature is ~465°C -- hot enough to melt lead -- due to an extreme greenhouse effect. The atmosphere is 90× denser than Earth's (equivalent to 900m underwater) and composed of carbon dioxide with sulphuric acid clouds. Every spacecraft that has landed on Venus has been destroyed within 2 hours by the pressure and heat. Mars, while cold (avg −63°C) and with a very thin atmosphere (1% of Earth's), is survivable for robotic missions. Rovers (Curiosity, Perseverance) have operated for years. Mars also has evidence of ancient water (dried riverbeds, polar ice caps) making it interesting for life-detection. There are also serious proposals for human missions to Mars. A human mission to Venus would require floating in the upper atmosphere -- the surface is inaccessible with current technology.

2. Why does the Moon always show the same face to Earth, and what would you see if you stood on the far side?

Tidal locking: Earth's gravity created tidal bulges in the Moon's solid crust. The gravitational pull on these bulges created a torque that gradually slowed the Moon's rotation over billions of years until its rotation period exactly equalled its orbital period (27.3 days). At that point, the same face perpetually points toward Earth -- the system is in its lowest energy state, and there's no longer a torque to change it. From the far side of the Moon, you would never see Earth -- it would always be below your horizon. You would see the stars and Sun in a completely black sky (no atmosphere means no scattered light). The far side has a much more heavily cratered surface -- the near side's mare (dark volcanic plains) are largely absent. China's Chang'e 4 became the first mission to land on the far side in January 2019. Communication requires a relay satellite positioned at the Earth-Moon L2 Lagrange point because the Moon itself blocks direct radio contact.

3. If you were on the ISS (400 km altitude), would you experience weightlessness because you're "far from Earth's gravity"?

No -- this is one of the most common misconceptions in space science. At 400 km altitude, Earth's gravity is still about 88–89% of its surface value. You feel weightless on the ISS not because gravity is weak, but because you are in continuous freefall. The ISS (and everything in it) is falling toward Earth at the same rate -- but moving horizontally fast enough (~27,600 km/h) that Earth's curved surface keeps falling away beneath it at the same rate it falls toward Earth. This is what an orbit is: perpetual freefall in which you miss the ground because you're moving sideways so fast. Astronauts experience microgravity because every object in the ISS -- the station itself, their bodies, their breakfast -- is all falling at exactly the same rate. There is no relative gravitational force between them. True weightlessness (absence of gravity) doesn't exist in the solar system -- gravity has infinite range, just diminishing with distance.

4. Saturn has rings -- why doesn't every gas giant? And what are the rings actually made of?

All four gas giants actually have rings -- but Saturn's are uniquely prominent and bright. Jupiter, Uranus, and Neptune all have ring systems, but they are faint and dark (composed of dust and dark rocky material). Saturn's rings are made primarily of water ice particles ranging from tiny grains to chunks several metres across -- and ice is highly reflective (albedo ~0.9 vs dark rocky material's ~0.05). This is why Saturn's rings are brilliant white and visible from Earth with a basic telescope while the other planets' rings are nearly invisible. The rings likely formed from the tidal disruption of an icy moon (or captured comet) that came within Saturn's Roche limit -- the distance at which tidal forces overcome an object's self-gravity. Saturn's rings are only ~10–100 metres thick despite being 282,000 km wide -- if scaled to the thickness of a sheet of paper, the rings would be several kilometres across. Saturn's rings are also surprisingly young -- estimated at only 10–100 million years old, meaning dinosaurs existed before Saturn had its current ring system.

5. How far away is the nearest star, and how does that distance put the solar system's scale in perspective?

Proxima Centauri is 4.24 light-years away -- ~40 trillion km, or ~268,000 AU. To put this in perspective: if you shrank the Sun to the size of a grapefruit (13 cm), Earth would be a grain of sand 14 metres away, Jupiter a marble 73 metres away, and Neptune a pea 440 metres away. The Oort Cloud's outer edge would be about 50 km away. Proxima Centauri, at the same scale, would be 3,800 km away -- roughly the distance from London to New York. The nearest star is as far from our solar system as a different continent is from another, while our entire solar system (planets) fits on a football pitch. The Voyager 1 probe, launched in 1977 and travelling at ~17 km/s (the fastest human-made object at the time), is currently ~24 billion km from Earth -- which sounds enormous but is only ~0.000025% of the way to Proxima Centauri. At its current speed, it would take ~73,000 years to reach there (it's not heading that direction).

6. What is the "Fermi Paradox" and why does the scale of the universe make it so puzzling?

The Fermi Paradox is physicist Enrico Fermi's famous question: "Where is everybody?" Given the universe contains ~2 trillion galaxies, each with ~100–400 billion stars, many with planetary systems, and the universe is 13.8 billion years old -- there has been ample time and space for intelligent civilisations to arise, spread, and make themselves detectable. Even at 1% of the speed of light (far slower than theoretical limits), a civilisation could colonise the entire Milky Way in ~10 million years -- a blink of cosmic time. Yet we detect nothing: no signals, no megastructures, no visitors. Proposed resolutions include: (1) The Great Filter -- some evolutionary step is extraordinarily rare, and either we have already passed it (life, eukaryotes, multicellular life, intelligence -- take your pick), or it lies ahead of us; (2) The civilisation lifetimes hypothesis -- intelligent civilisations self-destruct before going interstellar; (3) The "Dark Forest" hypothesis -- civilisations deliberately hide; (4) We simply haven't looked hard or long enough. The silence of the cosmos is one of the deepest unsolved questions in all of science.

7. If you fell into a black hole, would you notice crossing the event horizon? What would actually happen to you?

For a sufficiently large black hole, you would feel nothing special at the moment of crossing the event horizon. There is no physical surface, no wall, no flash of light -- just empty space. The event horizon is a mathematical boundary defined by the escape velocity equalling the speed of light. A local observer falling freely through it experiences no discontinuity. This is a consequence of the equivalence principle: freefall locally feels the same as being in empty space. However, two things would eventually kill you. First, tidal forces: as you approach the singularity, the difference in gravitational pull between your head and feet grows without limit, stretching you lengthwise and compressing you sideways -- physicists call this "spaghettification." For a stellar-mass black hole (~10 solar masses, Schwarzschild radius ~30 km), tidal forces at the event horizon are already fatal. For a supermassive black hole like M87* (6.5 billion solar masses, horizon radius ~19 billion km), tidal forces at the horizon are negligible -- you would cross it comfortably and only be torn apart much closer to the singularity. Second, time: once inside, every possible future path in spacetime leads to the singularity. You cannot escape, turn around, or send a message out. From a distant observer's perspective, you would appear to slow down asymptotically, growing redder and dimmer, never quite reaching the horizon -- frozen in time. The two perspectives are both physically valid and irreconcilable from the outside.

8. Traversable wormholes are mathematically permitted by general relativity -- so why do physicists think they almost certainly cannot exist in practice?

There are several compounding obstacles, each of which alone would likely be fatal. First, exotic matter: keeping a wormhole throat open requires material with negative energy density -- something that pushes outward against gravity rather than inward. The Casimir effect (a quantum vacuum phenomenon) demonstrates that negative energy densities are physically real in tiny amounts, but the quantities needed to stabilise a wormhole of traversable size would be astronomically large, possibly exceeding the total mass-energy of the observable universe for any useful wormhole. Second, stability: even if exotic matter were available, wormholes are dynamically unstable. Any small perturbation -- a single photon passing through -- causes the throat to collapse on a timescale far shorter than the crossing time. Third, Hawking's chronology protection conjecture: if a wormhole were stabilised, moving its two mouths to different gravitational potentials or at relativistic speeds relative to each other would create a time machine. Hawking argued that quantum vacuum fluctuations would build up in a feedback loop at the moment a closed timelike curve (time loop) became possible, delivering enough energy to destroy the wormhole before it could be used. This has not been proven rigorously but is consistent with the absence of time travellers. Fourth, the ER=EPR conjecture suggests that the wormholes that do exist in nature (connecting entangled black holes) are non-traversable by construction -- the quantum information link and the spacetime tunnel are real, but sending a signal through requires a process that is equivalent to faster-than-light communication, which quantum mechanics independently forbids. The mathematical existence of wormholes in general relativity is therefore considered a feature of the theory's geometry rather than a blueprint for construction.