Math + Cosmic Scales Survival Kit
January 23, 2026
By the end of this lecture, you will be able to:
Don’t panic about the equations!
Today I’ll show you examples using formulas we haven’t covered yet. You’re not expected to understand them fully — we’ll learn each one properly when its topic comes up.
For now, focus on the method, not the formula.
Think of it like watching a cooking demo before you have all the ingredients. You’re learning the technique — the details come later.
If the Sun were a cantaloupe in San Francisco…
…Earth would be a pinhead 15 meters away.
The nearest star? Another cantaloupe in Hawaii.
Math as a telescope 🔭
In ASTR 101, numbers aren’t decoration — they’re how we turn points of light into physical reality.
Four survival tools 🧰
A few anchor distances (order-of-magnitude is enough today):
| Scale | Distance | Light travel time |
|---|---|---|
| Earth–Moon | \(3.84\times10^8\,\text{m}\) | \(\sim 1.3\,\text{s}\) |
| 1 AU (Earth–Sun) | \(1.50\times10^{11}\,\text{m}\) | \(\sim 8.3\,\text{min}\) |
| 1 light-year (ly) | \(9.46\times10^{15}\,\text{m}\) | 1 year |
| 1 parsec (pc) | \(3.09\times10^{16}\,\text{m}\) | \(\sim 3.26\,\text{yr}\) |
The key idea
Distance and time mix in astronomy because information travels at a finite speed.
We don’t see things as they are. We see them as they were.
Common trap
A light-year is a distance, not a time — even though “year” is in the name. It’s how far light travels in one year: about 9.5 trillion km.
Light is the fastest thing in the universe. Nothing can travel faster.
\[c = 300{,}000\,\text{km/s} = 3 \times 10^8\,\text{m/s}\]
Every galaxy in this image is a time capsule. The light we see left millions to billions of years ago — we’re seeing them as they were, not as they are.
A light-year is a distance, not a time — even though “year” is in the name.
It’s how far light travels in one year:
\[1\,\text{ly} \approx 9.5 \times 10^{15}\,\text{m}\]
That’s about 9.5 trillion kilometers.
Why use light-years?
“Proxima Centauri is \(4 \times 10^{16}\) m away” is painful.
“4.2 light-years” is memorable.
Because light takes time to travel, looking far away = looking back in time.
| Object | Distance | You see it as it was… |
|---|---|---|
| Moon | 1.3 light-sec | 1.3 seconds ago |
| Sun | 8.3 light-min | 8.3 minutes ago |
| Proxima Centauri | 4.2 ly | 4.2 years ago |
| Andromeda Galaxy | 2.5 Mly | 2.5 million years ago |
Mind-bending implication
The further we look, the further back in time we see.
The most distant galaxies show us the universe as it was billions of years ago.
These cosmic scales are why we need a math survival kit:
These aren’t abstract math exercises. They’re the tools that let us decode the universe.
Each step on this ladder is a factor of 10.
From your desk to the edge of the observable universe takes about 27 steps.
The mnemonic
(555)-711-2555 encodes the multipliers at each scale jump. Astronomers really do use phone-number tricks to navigate cosmic scales!
Light takes about 8.3 minutes to travel 1 AU.
Tool 1: Scientific Notation
Because the universe refuses to be written out in longhand
A number written as
\[a\times 10^n\]
means:
Big number
\(300{,}000{,}000\,\text{m/s} = 3.0\times10^8\,\text{m/s}\)
Small number
\(0.000000001\,\text{s} = 1.0\times10^{-9}\,\text{s}\)
Direction rule
Why this works
Exponents are a shorthand for repeated multiplication. Adding exponents = multiplying powers of ten: \(10^3 \times 10^2 = 10^{3+2} = 10^5\).
What is \((3 \times 10^5)(4 \times 10^3)\)?
| Prefix | Symbol | Factor |
|---|---|---|
| tera | T | \(10^{12}\) |
| giga | G | \(10^{9}\) |
| mega | M | \(10^{6}\) |
| kilo | k | \(10^{3}\) |
| milli | m | \(10^{-3}\) |
| micro | \(\mu\) | \(10^{-6}\) |
| nano | n | \(10^{-9}\) |
When exact arithmetic is annoying, estimate on purpose.
OoM is not “sloppy.” It’s a controlled approximation for staying in the right cosmic zip code.
Tool 2: Units & Conversions
Units are the meaning of a number
A physical quantity = a number + a unit
✓ Physical quantities
✗ Not physical quantities
The unit is not optional. Without it, the number is meaningless.
A physical constant is a number that nature gives us — it doesn’t change.
Why do constants matter?
They’re conversion factors between different physical quantities. The speed of light \(c\) converts between distance and time. That’s why light-years work!
Units are human choices:
Dimensions are the type of quantity:
Examples:
Why mention dimensions?
Not to do a full “dimension analysis” unit…but because unit mistakes are the #1 avoidable error in astronomy problems.
A conversion factor is an equality written as a fraction.
Example:
\[1\,\text{m} \leftrightarrow 100\,\text{cm}\]
so you can use
\[\frac{100\,\text{cm}}{1\,\text{m}}=1 \quad \text{or} \quad \frac{1\,\text{m}}{100\,\text{cm}}=1.\]
Write what you’re given.
Multiply by conversion factors arranged so units cancel.
Check that your final units match what you wanted.
Selection rule
Put the unit you want to remove in the denominator.
\[1000\,\text{min}\times\frac{1\,\text{hr}}{60\,\text{min}} = \frac{1000}{60}\,\text{hr}\approx 16.7\,\text{hr}\]
Sanity check: hours are bigger units than minutes, so the number should get smaller. ✓
A) Convert \(60\,\text{mph}\) to \(\text{m/s}\).
B) Convert \(0.5^\circ\) to arcseconds.
(Use: \(1\,\text{mile}=1.6\,\text{km}\), \(1\,\text{hr}=3600\,\text{s}\), \(1^\circ=60\,\text{arcmin}\), \(1\,\text{arcmin}=60\,\text{arcsec}\).)
Quick vocab: angular units
Astronomers measure tiny angles in arcminutes (1/60 of a degree) and arcseconds (1/60 of an arcminute). The Moon is about 30 arcmin wide; a star’s disk is less than 0.05 arcsec.
When a unit is squared or cubed, the conversion factor gets squared/cubed too.
The trap: Students often write
\[1\,\text{m}^3 = 100\,\text{cm}^3\] ❌
Why it’s wrong: You’re converting each dimension.
The right way:
\[1\,\text{m} = 100\,\text{cm}\]
\[1\,\text{m}^3 = (1\,\text{m})^3 = (100\,\text{cm})^3\]
\[= 100^3\,\text{cm}^3 = 10^6\,\text{cm}^3\] ✓
Rule: When converting \(\text{m}^n\), raise the conversion factor to the \(n\)th power too.
Pro tip: Parentheses are your best friend — wrap the number and unit together: \((100\,\text{cm})^3\), not \(100\,\text{cm}^3\).
Physics has only three base dimensions: length \([L]\), mass \([M]\), time \([T]\).
Everything else is built from combinations:
The building principle
Complex quantities are just base dimensions multiplied and divided. If you know the recipe, you can always check your work.
| Quantity | Dimension | SI Unit | Named Unit |
|---|---|---|---|
| Length | \([L]\) | m | meter |
| Mass | \([M]\) | kg | kilogram |
| Time | \([T]\) | s | second |
| Velocity | \([L][T]^{-1}\) | m/s | — |
| Acceleration | \([L][T]^{-2}\) | m/s² | — |
| Force | \([M][L][T]^{-2}\) | kg·m/s² | Newton (N) |
| Energy | \([M][L]^2[T]^{-2}\) | kg·m²/s² | Joule (J) |
| Power | \([M][L]^2[T]^{-3}\) | kg·m²/s³ | Watt (W) |
| Pressure | \([M][L]^{-1}[T]^{-2}\) | kg/(m·s²) | Pascal (Pa) |
Named units are shortcuts. A Newton is just kg·m/s². A Joule is just kg·m²/s². If a unit looks unfamiliar, rewrite it in base units!
Tool 3: The Ratio Method
Compare systems without calculator misery
The hard way: Calculate Jupiter’s surface gravity.
The ratio way: Compare Jupiter to Earth.
The pattern
If \(A = k B^n\), then comparing two cases:
\[\frac{A_2}{A_1}=\left(\frac{B_2}{B_1}\right)^n\]
The constant \(k\) cancels!
What this says: Ratios let you compare systems using only the relationship between quantities — no need to look up constants.
| Scaling | Meaning | Where it shows up |
|---|---|---|
| \(\propto R^2\) | area grows fast | telescope area, surface area |
| \(\propto R^3\) | volume grows very fast | planet volumes, “how many Earths” |
| \(\propto 1/r^2\) | inverse-square | brightness, gravity |
Problem: The Keck telescope has a 10-meter diameter mirror. The Hubble Space Telescope has a 2.4-meter diameter mirror. How much more light can Keck collect?
Setup: Light-collecting area scales as \(A \propto D^2\) (area of a circle)
Ratio method: \[\frac{A_\text{Keck}}{A_\text{Hubble}} = \left(\frac{D_\text{Keck}}{D_\text{Hubble}}\right)^2 = \left(\frac{10}{2.4}\right)^2 \approx (4.2)^2 \approx 17\]
Answer: Keck collects about 17× more light than Hubble — no need to calculate actual areas!
The Sun’s radius is about 109× Earth’s radius. How many Earths fit inside the Sun?
Using \(V \propto R^3\), what is \(V_\odot / V_\oplus\)?
What we measure: Brightness ratio of two stars (same apparent brightness)
What physics says: Inverse-square law means equal brightness at different distances implies different luminosities
What we conclude: A star 10× further away but equally bright must be 100× more luminous
The ratio shortcut
\(\frac{L_2}{L_1} = \left(\frac{d_2}{d_1}\right)^2 = 10^2 = 100\)
If you move twice as far from a light source:
\[\text{brightness}\propto \frac{1}{d^2}\]
Watch the flip!
Because brightness is inversely proportional to \(d^2\), the ratio flips:
\[\frac{B_2}{B_1}=\left(\frac{d_1}{d_2}\right)^2\]
Astronomers call this flux — energy per second per area (W/m²).
Example: Twice as far → \(\dfrac{B_2}{B_1}=\left(\dfrac{1}{2}\right)^2=\dfrac{1}{4}\) the brightness.
Problem: Mars orbits at 1.5 AU from the Sun. Earth orbits at 1 AU. How does the intensity of sunlight on Mars compare to Earth?
Setup: Sunlight intensity follows the inverse-square law: \(I \propto 1/d^2\)
Ratio method: \[\frac{I_\text{Mars}}{I_\text{Earth}} = \left(\frac{d_\text{Earth}}{d_\text{Mars}}\right)^2 = \left(\frac{1}{1.5}\right)^2 = \left(\frac{2}{3}\right)^2 = \frac{4}{9} \approx 0.44\]
Answer: Mars receives only 44% as much sunlight as Earth — less than half!
This is why solar panels on Mars rovers need to be so large. (Mars is cold mostly because its thin atmosphere can’t trap heat — but less sunlight doesn’t help!)
What we measure: Brightness (flux \(F\)) — how much light arrives at our detector (W/m²)
What physics says: Inverse-square law relates flux, luminosity, and distance:
\[F = \frac{L}{4\pi d^2}\]
where \(L\) = luminosity (total power output, in Watts) and \(d\) = distance
What we conclude: If we know a star’s true luminosity \(L\) and measure its flux \(F\), we can solve for distance \(d\)
The inference chain
Observable (\(F\)) → Model (inverse-square) → Physical property (\(d\))
Tool 4: Rate Problems
Change per time is basically the universe’s favorite sentence structure
Most rate problems are one equation with three rearrangements:
\[\text{amount} = \text{rate}\times\text{time}\]
Astronomy examples
What this says: If you know any two of these, you can find the third. This single pattern solves most “how far/fast/long” questions.
Problem: How far does light travel in one year? (In meters)
Step 1: Identify the rate equation
\[\text{distance} = \text{speed} \times \text{time}\]
Step 2: Gather your values
But wait — the units don’t match! We need time in seconds.
Step 3: Convert 1 year → seconds
\[1\,\text{yr} \times \frac{365\,\text{days}}{1\,\text{yr}} \times \frac{24\,\text{hr}}{1\,\text{day}} \times \frac{3600\,\text{s}}{1\,\text{hr}}\]
\[= 365 \times 24 \times 3600\,\text{s}\]
\[\approx 3.15 \times 10^7\,\text{s}\]
Step 4: Multiply using scientific notation
\[1\,\text{ly} = c \times t = (3 \times 10^8\,\text{m/s}) \times (3.15 \times 10^7\,\text{s})\]
Scientific notation multiplication rule
Multiply coefficients, add exponents: \((a \times 10^m) \times (b \times 10^n) = (a \times b) \times 10^{m+n}\)
\[= (3 \times 3.15) \times 10^{8+7}\,\text{m}\] \[= 9.45 \times 10^{15}\,\text{m}\]
Answer: \(1\,\text{ly} \approx 9.5 \times 10^{15}\,\text{m}\) (about 9.5 trillion kilometers)
What we measure: Distance to a galaxy (in light-years)
What physics says: Light travels at \(c = 3 \times 10^8\) m/s (finite speed)
What we conclude: A galaxy 2.5 million light-years away → we see it as it was 2.5 million years ago
Distance is a time machine. The further we look, the further back in time we see.
Earth moves around the Sun at about \(29.8\,\text{km/s}\).
How far does Earth travel in one minute? (Answer in meters.)
The decoding ritual
For any quantitative astronomy question:
| Unit | What it’s good for | Useful fact |
|---|---|---|
| AU | solar system distances | \(1\,\text{AU}\approx 1.50\times10^{11}\,\text{m}\) |
| ly | “how far light goes” | \(1\,\text{ly}\approx 9.46\times10^{15}\,\text{m}\) |
| pc | star/galaxy distances | \(1\,\text{pc}\approx 3.09\times10^{16}\,\text{m}\approx 3.26\,\text{ly}\) |
Recognition, not retention
You don’t need to memorize formulas. You need to recognize patterns:
When you see a big number or a scaling question, you’ll know which tool to reach for.
If you move twice as far from a light source, brightness becomes…
Step 1: Multiply the coefficients \[3 \times 4 = 12\]
Step 2: Add the exponents \[10^5 \times 10^3 = 10^{5+3} = 10^8\]
Step 3: Combine \[12 \times 10^8\]
Step 4: Normalize (coefficient should be between 1 and 10) \[12 \times 10^8 = 1.2 \times 10^9\]
\[60 \frac{\text{mile}}{\text{hr}}\times\frac{1.6\,\text{km}}{1\,\text{mile}}\times\frac{1000\,\text{m}}{1\,\text{km}}\times\frac{1\,\text{hr}}{3600\,\text{s}}\approx 26.7\,\text{m/s}\]
\[0.5^\circ\times\frac{60\,\text{arcmin}}{1^\circ}\times\frac{60\,\text{arcsec}}{1\,\text{arcmin}}=1800\,\text{arcsec}\]
\[109^3 \approx (1.09\times10^2)^3 = 1.09^3\times10^6\approx 1.3\times10^6.\]
So the Sun’s volume is about 1.3 million Earth volumes.
\[29.8\,\text{km/s} = 2.98\times10^4\,\text{m/s}\]
One minute is \(60\,\text{s}\), so
\[\text{distance}=vt=(2.98\times10^4\,\text{m/s})(60\,\text{s})\approx 1.79\times10^6\,\text{m}.\]
That’s about 1800 km in one minute.

ASTR 101 • Lecture 2