Audited ·Last updated 29 Jul 2026·4 citations·Tier 2·0 uses

Apparent Magnitude & Brightness Ratio Calculator

How many times brighter is one star than another? Convert between magnitude difference and flux ratio on the Pogson scale, and combine two magnitudes.

Apparent Magnitude Calculator

What do you want to find?
The reference object, used in both modes. The scale runs backwards — smaller is brighter. Default is SIMBAD's V = −1.46 for Sirius.
Used when comparing two magnitudes. Must be in the SAME photometric band as object 1. Default is SIMBAD's V = 0.03 for Vega.
Used when converting a ratio back to magnitudes. How many times more flux object 1 delivers than object 2. Must be greater than zero; values below 1 mean object 1 is the fainter one.
Brightness ratio F₁ / F₂
3.9446
10^(0.4 × Δm). How many times more flux object 1 delivers than object 2. Dimensionless.
Magnitude difference Δm = m₂ − m₁
1.49
Apparent magnitude of object 1
-1.46
Apparent magnitude of object 2
0.03
Extra flux from object 1 (%)
294.4573
Combined magnitude of the pair
-1.7053
Flux factor of one magnitude
2.5119
How to read this result
Object 1 (magnitude -1.46) is the brighter of the two — remember the scale runs backwards, so the smaller magnitude wins. It delivers 3.94457 times the flux of object 2. These figures are valid only if both magnitudes were measured in the SAME photometric band, because the zero point cancels out of a ratio only within one band. The combined magnitude assumes the two sources are blended into one unresolved measurement and that their fluxes simply add; it models no extinction.

Background.

"Sirius is magnitude −1.46 and Vega is magnitude 0.03" is a statement most people can read but few can feel. How much brighter is that, actually? This calculator answers exactly that: give it two apparent magnitudes and it tells you the ratio of the light they deliver, or give it a brightness ratio and it tells you how many magnitudes that is. It also combines two magnitudes into the single value a photometer would report if it could not separate them.

The scale is logarithmic and it runs backwards, which is why the arithmetic is not obvious. Norman Pogson formalised the inherited Greek ranking in 1856 by fixing five magnitudes as exactly a hundredfold difference in brightness. That makes one magnitude a factor of 100^(1/5) = 2.5118864315 — usually quoted as 2.512 — and it forces the minus sign in the definition, m = −2.5 log₁₀(flux) + constant, so that brighter objects keep the small numbers they had inherited. ESA's education material states the same property directly: "the difference between each step on the scale is equal to a decrease in brightness of 2.512 and (2.512)⁵ = 100".

The practical formulas follow immediately. The ratio of two fluxes is F₁/F₂ = 10^(0.4(m₂ − m₁)), and the difference of two magnitudes is Δm = 2.5 log₁₀(F₁/F₂). Notice that no zero point appears in either: because both are built from a difference or a ratio, whatever constant defines the photometric system cancels exactly. That is what lets this page work in the V band, in Gaia's G band, in bolometric magnitudes or in anything else — provided both magnitudes come from the same band. Mix a V magnitude with a bolometric one and the cancellation is invalid, the answer is silently wrong, and no arithmetic can detect it. The result note says so on every calculation.

The combined-magnitude output answers a different and genuinely useful question: what does a close pair look like when a photometer cannot resolve them? Fluxes add, magnitudes do not, so you have to convert down to flux, add, and convert back: m_total = −2.5 log₁₀(10^(−0.4m₁) + 10^(−0.4m₂)). Two identical stars blend to 2.5 log₁₀(2) = 0.753 magnitudes brighter than either alone — not one magnitude, and certainly not the sum of the two. This assumes the fluxes simply add, which holds for incoherent sources in the same band, and it models no extinction.

One limit worth naming before you use the number: apparent magnitude describes what reaches you, not what the object emits. Two stars with the same apparent magnitude can differ by orders of magnitude in real output if one is far more distant, and interstellar dust dims things further along the way. If you want intrinsic brightness, you need the distance modulus and an absolute magnitude — that is the stellar magnitude calculator — or a luminosity in watts, which is the luminosity calculator. This page compares what you see, and only what you see.

What is apparent magnitude calculator?

Apparent magnitude, m, is the logarithmic measure of how bright a celestial object appears from Earth. It combines the object's real output, its distance, and any dimming along the way into one number, and it is what a telescope actually measures. The scale is inverted — the brightest objects have the most negative values — because it descends from a Greek ranking in which the brightest stars were "of the first magnitude" and the faintest visible ones "of the sixth".

Pogson's 1856 convention fixed that inherited ranking to an exact ratio: five magnitudes is exactly a factor of 100 in flux, so one magnitude is 100^(1/5) = 2.5118864315. From this everything on this page follows. The flux ratio of two objects is F₁/F₂ = 10^(0.4(m₂ − m₁)); the magnitude difference for a known flux ratio is Δm = 2.5 log₁₀(F₁/F₂); and the blended magnitude of an unresolved pair is m_total = −2.5 log₁₀(10^(−0.4m₁) + 10^(−0.4m₂)).

Because all three are ratios or differences, the photometric zero point cancels and none of them needs one. The IAU did fix exact zero points in 2015 (Resolution B2) for the bolometric scale specifically — m_bol = 0 at an irradiance of 2.518021002 × 10⁻⁸ W m⁻² — but those are needed only to convert a magnitude into a physical flux, which this page deliberately does not do. What it needs from the IAU definition is just the −2.5 log₁₀ form.

What apparent magnitude is not: it is not absolute magnitude (which is the apparent magnitude at 10 parsecs), it is not luminosity (total power in watts), and it is not comparable across photometric bands. All three of those distinctions cause real errors, and all three are handled by other pages here rather than fudged into this one.

How to use this calculator.

  1. Pick your direction: two magnitudes to a brightness ratio, or a brightness ratio to a magnitude difference.
  2. Enter the magnitude of the reference object as object 1. Both modes need it.
  3. Enter the second magnitude, or the flux ratio, depending on your chosen mode.
  4. Check that both magnitudes come from the same photometric band. This is the one error the calculator cannot catch for you.
  5. Read the brightness ratio, the percentage, and — if you are dealing with an unresolved pair — the combined magnitude.

The formula.

F₁ ⁄ F₂ = 10^(0.4 (m₂ − m₁)) · Δm = 2.5 log₁₀(F₁ ⁄ F₂) · m_total = −2.5 log₁₀(10^(−0.4m₁) + 10^(−0.4m₂))

Start from the definition m = −2.5 log₁₀(F) + C, where C is the photometric zero point of whatever system you are in. Subtract two of them and C vanishes: m₂ − m₁ = −2.5 log₁₀(F₂/F₁) = 2.5 log₁₀(F₁/F₂). Exponentiating gives F₁/F₂ = 10^(0.4(m₂ − m₁)), which is the first formula on this page, and rearranging gives Δm = 2.5 log₁₀(F₁/F₂), which is the second. The disappearance of C is not a convenience — it is the reason this page is band-agnostic, and it is also precisely why the two magnitudes must come from the same band, since two different C values do not cancel.

The sign is the part that trips people. Δm is defined here as m₂ − m₁, so a positive Δm means object 2 has the larger magnitude, which on an inverted scale means object 2 is the fainter one and object 1 is brighter. Sirius at −1.46 and Vega at 0.03 give Δm = +1.49 and a ratio of 3.94, meaning Sirius delivers 3.94 times Vega's flux. Swap the inputs and Δm becomes −1.49 and the ratio becomes 1/3.94 = 0.2535 — the calculator does exactly that, and a test asserts it.

The combined magnitude cannot be done in magnitude space at all, because magnitudes are logarithms and light adds linearly. Each magnitude is converted to a relative flux with 10^(−0.4m), the two fluxes are added, and the sum is converted back with −2.5 log₁₀. For two identical sources the answer is m − 2.5 log₁₀(2) = m − 0.7525749892: doubling the light is three quarters of a magnitude, not one. For Sirius and Vega the blend is −1.7053219872, brighter than Sirius alone but by only a quarter of a magnitude, because Vega contributes about a fifth of the combined light.

Rounding stage: no intermediate rounding. All arithmetic runs at 40 significant digits in a private decimal context, and rounding happens once at the return boundary — magnitudes to ten decimal places, ratios and percentages to twelve significant digits (a ratio can legitimately be 10⁻²⁰ or 10²⁰, which decimal-place rounding would destroy). The brighter/fainter/equal decision is made on the unrounded magnitude difference, so the exactly-equal case is deterministic.

Invalid-domain behaviour: a flux ratio of zero or below raises a field error, since the logarithm has no value there and negative brightness has no physical reading. Magnitudes outside −60 to +70 raise an error, as does a flux ratio outside 10⁻⁴⁰ to 10⁴⁰, because beyond those the derived quantities exceed what a double can hold; for scale, the Sun is about −26.8 and the faintest objects Hubble has detected are around +31, so the supported range is far wider than astronomy uses.

A worked example.

Example

Sirius and Vega are the two brightest stars in the northern sky, and both V magnitudes come from SIMBAD: Sirius (α CMa) at −1.46 and Vega (α Lyr) at 0.03. The magnitude difference is Δm = 0.03 − (−1.46) = 1.49. It is positive, which on the inverted scale means object 1 — Sirius — is the brighter one. The brightness ratio is F₁/F₂ = 10^(0.4 × 1.49) = 10^0.596 = 3.9445730208. Sirius delivers 3.94 times the visual flux of Vega, or 294.46% more. Less than a magnitude and a half of separation is already a factor of nearly four in light — that is how compressed the magnitude scale is. Blended together, as an instrument that could not resolve them would see, they give m_total = −2.5 log₁₀(10^(0.584) + 10^(−0.012)) = −2.5 log₁₀(3.83709 + 0.97275) = −1.7053219872. Adding Vega's light to Sirius brightens the pair by only 0.245 magnitudes, because Vega contributes about a fifth of the total. A sanity check with the scale's own defining property: setting the two magnitudes to 0 and 5 gives a ratio of exactly 100, and setting them to 0 and 1 gives exactly 2.5118864315. Both are what ESA states the Pogson scale must do, and both are asserted as tests. A scope note on this specific example: SIMBAD's V magnitudes for both stars carry quality flag C with no quoted uncertainty, and Vega's 0.03 is itself a measured value, not the exact 0.00 that the historical Vega-based magnitude system was supposed to assign it. Modern photometric systems no longer define Vega as exactly zero, which is why the catalogue value is 0.03 rather than 0. The ratio computed here is exactly what those two catalogue numbers imply, no more.

magnitude20.03
magnitude1-1.46
solve ForbrightnessRatio

Frequently asked questions.

How many times brighter is a magnitude 1 star than a magnitude 6 star?
Exactly 100 times. That is the definition of the modern scale: Pogson fixed five magnitudes as exactly a hundredfold difference in brightness in 1856, which is why one magnitude is 100^(1/5) = 2.5118864315 and five steps of it multiply to exactly 100. ESA states the same thing as "(2.512)⁵ = 100". This calculator reproduces both figures exactly rather than approximately.
Why is a smaller magnitude brighter?
Because the scale is a formalisation of a two-thousand-year-old ranking rather than a measurement designed from scratch. Hipparchus called the brightest stars "first magnitude" and the faintest naked-eye ones "sixth". When Pogson put that ranking on a logarithmic footing he preserved the ordering, which required a minus sign: m = −2.5 log₁₀(flux) + constant. Objects brighter than "first magnitude" then need negative numbers, which is how Sirius ends up at −1.46 and the Sun at about −26.8.
What is the formula for the brightness ratio between two magnitudes?
F₁/F₂ = 10^(0.4 × (m₂ − m₁)). Going the other way, Δm = 2.5 log₁₀(F₁/F₂). No zero point appears in either, because it cancels out of a ratio — which is exactly why both magnitudes have to be measured in the same photometric band for the cancellation to be legitimate.
Can I compare a V magnitude with a Gaia G magnitude?
Not directly, and this is the one mistake the calculator cannot catch. Different bands have different zero points and sample different parts of the spectrum, so the constant that vanishes from a same-band ratio does not vanish from a cross-band one. The resulting number will look perfectly reasonable and will be wrong by an amount that depends on the stars' colours. Convert to a common band first, using a published colour transformation for the specific catalogues involved.
How do I combine the magnitudes of two stars?
You cannot add or average magnitudes — light adds, logarithms do not. Convert each to a relative flux with 10^(−0.4m), add those, then convert back with −2.5 log₁₀. Two identical stars come out 2.5 log₁₀(2) = 0.753 magnitudes brighter than one, not one magnitude brighter. Sirius and Vega blended give −1.705, only 0.245 magnitudes brighter than Sirius alone. This calculator reports the combined magnitude on every calculation.
Isn't Vega defined as magnitude zero?
It used to be the anchor of the visual magnitude system, and "Vega magnitudes" is still standard terminology, but modern photometric systems do not define it as exactly 0.00. SIMBAD lists Vega at V = 0.03, and that measured value is what this page's default uses. Vega is also a rapid rotator seen nearly pole-on and is slightly variable, which is part of why the field moved to systems anchored on physical flux densities instead. If you see 0.00 quoted, it is a legacy convention rather than a measurement.
Does a brighter apparent magnitude mean a more luminous star?
No — that is the single biggest misreading of apparent magnitude. It tells you how much light arrives, which mixes the object's real output with its distance and with any dust in between. Sirius outshines almost everything in our sky mainly because it is 2.6 parsecs away; move it to 10 parsecs and it would be an ordinary magnitude 1.43 star. For intrinsic brightness you want absolute magnitude, from the stellar magnitude calculator, or luminosity in watts, from the luminosity calculator.
What does the percentage output mean?
It is (F₁/F₂ − 1) × 100 — how much extra flux object 1 delivers relative to object 2, expressed as a percentage. Sirius against Vega gives 294.46%, meaning Sirius delivers nearly three times as much light again on top of Vega's. When object 1 is the fainter one the percentage goes negative: a magnitude 6 object compared with a magnitude 1 object gives −99%, because it delivers only one hundredth of the flux.

References& sources.

  1. [1]European Space Agency, Science & Technology education resource, "Stellar Distances" (retrieved 2026-07-29). States the defining property of the Pogson scale: "a magnitude 1 star is 100 times brighter than a magnitude 6 star" because "the difference between each step on the scale is equal to a decrease in brightness of 2.512 and (2.512)⁵ = 100". Also defines apparent versus absolute magnitude. Independent of the IAU documents below; open access.
  2. [2]Mamajek, E. E., et al. (2015), "IAU 2015 Resolution B2 on Recommended Zero Points for the Absolute and Apparent Bolometric Magnitude Scales", arXiv:1510.06262 (retrieved 2026-07-29). Fixes the −2.5 log₁₀ form of the magnitude definition with exact zero points (m_bol = −2.5 log₁₀(f/f₀), f₀ = 2.518021002 × 10⁻⁸ W m⁻²). This page needs only the functional form, since every quantity it returns is a ratio in which the zero point cancels. Open-access preprint of an adopted IAU resolution.
  3. [3]SIMBAD astronomical database (CDS, Strasbourg), objects "Sirius" (alf CMa, V = −1.46) and "Vega" (alf Lyr, V = 0.03), both from reference 2002yCat.2237....0D with quality flag C and no quoted uncertainty. Retrieved 2026-07-29. The two inputs to the worked example. Independent data centre; open access.
  4. [4]Pogson, N. R. (1856), "Magnitudes of Thirty-six of the Minor Planets for the First Day of each Month of the Year 1857", Monthly Notices of the Royal Astronomical Society 17, 12. The paper that proposed fixing a light ratio of 100^(1/5) per magnitude, giving the modern m = −2.5 log I scale. Bibliographic reference only — the 1856 volume is an archival scan and was not machine-readable at the time of writing; the scale's defining property is verified here against the ESA citation above rather than against the original.

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