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Space · Subtopic 1 of 5

Standard Candles

A star's luminosity LL is the total power it radiates. At distance dd, that power spreads over a sphere of area 4πd24\pi d^2, so the radiant flux intensity received is F=L4πd2F=\dfrac L{4\pi d^2}. A standard candle is an object whose luminosity is known, such as a Cepheid variable star or a type Ia supernova. Measuring its flux then gives its distance: d=L4πFd=\sqrt{\dfrac L{4\pi F}}.

Cambridge 9702 Paper 4Edexcel YPH11 WPH15AQA 7408 Paper 3B≈ 30 minRevision 5 · updated 2026-10-27
Section 1 of 14

Learning objectives

  • Define luminosity and radiant flux intensity.
  • Use the inverse square law F=L4πd2F=\dfrac L{4\pi d^2}.
  • Explain what a standard candle is and give examples.
  • Use standard candles to find distances to galaxies.
Pause and think

Two stars look equally bright in the sky. Are they the same distance away?

Section 2 of 14

Core idea

Start hereHow far is a street light?

If you know a street lamp is 100 W, you can judge its distance by how dim it looks. Astronomers do the same with stars of known power: standard candles.

The big idea

F=L4πd2F=\frac L{4\pi d^2}. Known LL + measured FF → distance.

1. Inverse-square law

Light spreads over a sphere of area 4πd²
d2d: same light over 4× the area
At twice the distance, the same power covers four times the area: a quarter of the flux.
F=L4πd2F=\frac L{4\pi d^2}
where
FF
radiant flux intensity (W m⁻²).
LL
luminosity (W).
Worked exampleThe solar constant

L=3.83×1026L=3.83\times10^{26} W, d=1.5×1011d=1.5\times10^{11} m.

Goal
FF at Earth.
Strategy
Formula.
  1. 4π(1.5×1011)2=2.83×1023 m24\pi(1.5\times10^{11})^2=2.83\times10^{23}\text{ m}^2
    Sphere area.
  2. F=1.36×103 W m−2F=1.36\times10^3\text{ W m}^{-2}
    Divide.
Answer1.361.36 kW m−2^{-2}.
✓ CheckMatches the measured solar constant ✓.

2. Finding distance

Flux from a star against distance
10203040500.20.40.60.810distance (light-years)flux (relative)F = L / 4πd²
Knowing LL and measuring FF: d=L4πFd=\sqrt{\dfrac{L}{4\pi F}}.
Worked exampleA Cepheid

L=1.0×1030L=1.0\times10^{30} W, F=2.0×10−12F=2.0\times10^{-12} W m−2^{-2}.

Goal
dd.
Strategy
d=L4πFd=\sqrt{\frac L{4\pi F}}.
  1. 4πF=2.51×10−114\pi F=2.51\times10^{-11}
    Denominator.
  2. d=10302.51×10−11=2.0×1020 md=\sqrt{\frac{10^{30}}{2.51\times10^{-11}}}=2.0\times10^{20}\text{ m}
    Square root.
Answer2.0×10202.0\times10^{20} m (~21 000 light-years).
✓ CheckWithin our galaxy's scale ✓.
Common misconceptionForgetting the square root d∝L/Fd\propto\sqrt{L/F}.
Pause and think

Two standard candles?

Summary

  • F=L/(4πd2)F=L/(4\pi d^2).
  • Known LL → distance.
Key words
Luminosity
Total power emitted.
HistoryLeavitt's law. In 19121912 Henrietta Swan Leavitt, working as a "computer" at Harvard measuring photographic plates, discovered that brighter Cepheids pulse more slowly. Edwin Hubble later used her relationship to show that the Andromeda "nebula" was a separate galaxy far beyond the Milky Way.
Fun factBrighter than a galaxy. A type Ia supernova can briefly outshine its entire host galaxy of 100100 billion stars. Astronomers in 19981998 used them to discover that the expansion of the universe is speeding up, earning a Nobel Prize.
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