X-ray Binary Luminosity Calculator

Compute X-ray binary luminosity from mass accretion rate and radiative efficiency, or from the Eddington fraction. Classifies BH, NS, ULX, and AGN sources.

💫 X-ray Binary Luminosity Calculator
Compact Object Mass M (M☉)
M☉
Compact Object Radius R (km)
km
Radiative Efficiency η (0 to 1)
fraction
Mass Accretion Rate (M☉/yr)
M☉/yr
Compact Object Mass (M☉)
M☉
Eddington Fraction L/LEdd
× LEdd
Accretion Luminosity
Eddington Luminosity
Eddington Ratio
Eddington Accretion Rate
Luminosity in L☉
Source Classification
Actual Luminosity
Eddington Luminosity
Required Mdot (eta=0.1)
Eddington Mdot (eta=0.1)
Luminosity in L☉
Source Classification

💫 What is an X-ray Binary Luminosity Calculator?

An X-ray binary (XRB) is a stellar system in which a compact object -- a neutron star or black hole -- accretes matter from a companion star, releasing gravitational potential energy primarily as X-ray emission. As material falls from the donor star through an accretion disk onto the compact object, it releases energy at a rate governed by the simple formula L = eta * Mdot * c^2, where eta is the radiative efficiency, Mdot is the mass accretion rate, and c is the speed of light. This process is the most efficient known way to extract energy from matter short of matter-antimatter annihilation, making X-ray binaries among the most luminous persistent X-ray sources in the universe.

The radiative efficiency eta encodes the depth of the gravitational potential well. For a non-spinning (Schwarzschild) black hole, the innermost stable circular orbit (ISCO) sits at 6 GM/c^2, and infalling matter releases eta ~ 5.7% of its rest-mass energy. For a maximally spinning (Kerr) black hole, the ISCO shrinks to 1.24 GM/c^2 and eta reaches ~42%. Neutron stars, with their hard surfaces at roughly 10 km, have eta ~ 15-25% because all kinetic energy thermalizes at the surface. This difference in efficiency makes NSs more luminous per unit mass accretion rate than Schwarzschild BHs.

The Eddington luminosity sets the natural luminosity scale for any compact accretor. At L_Edd = 4*pi*G*M*m_p*c/sigma_T, radiation pressure on free electrons exactly balances gravity, limiting spherically symmetric accretion. Sources exceeding L_Edd include ultraluminous X-ray sources (ULXs), which may represent super-Eddington disk accretion with powerful outflows, beamed emission, or intermediate-mass black holes. This calculator handles all regimes from quiescent LMXBs (0.001 L_Edd) to hyperluminous X-ray sources (1000 L_Edd).

Famous examples include Cygnus X-1, the first confirmed stellar black hole (21.2 M_sun), accreting from a supergiant companion at about 2% Eddington in its hard state; Sco X-1, the first extrasolar X-ray source discovered (1962), a neutron star LMXB near its Eddington limit; and Her X-1, an X-ray pulsar with strong pulsations revealing its 1.4 M_sun neutron star accretor. Load these presets to explore real observed parameters and compare them to theoretical predictions.

📐 Formula

Lacc  =  η × Ṁ × c²
Lacc = accretion luminosity (W)
η = radiative efficiency (0.057 for Schwarzschild BH, 0.20 for NS, up to 0.42 for Kerr BH)
= mass accretion rate (kg/s)
c = speed of light = 2.998 × 108 m/s
LEdd  =  4πGM mpc / σT  ≈  1.26 × 1031 (M/M) W
M = compact object mass | mp = proton mass = 1.673 × 10−27 kg
σT = Thomson cross-section = 6.652 × 10−29
Edd = LEdd / (ηc²)  —  mass rate at Eddington luminosity
Example: Cygnus X-1: M = 21.2 M⊙, η = 0.057, Ṁ = 2×10−6 M⊙/yr → L ≈ 4.6 × 1030 W ≈ 0.03 LEdd

📖 How to Use This Calculator

Steps

1
Select mode - Use Accretion Rate mode to input the physical mass transfer rate and efficiency. Use Eddington Fraction mode to specify luminosity as a multiple of L_Edd, useful when the Eddington fraction is known from spectral fitting.
2
Enter compact object parameters - For accretion mode: mass in solar masses, radius in km (use ISCO radius for BH), radiative efficiency eta, and mass accretion rate in M_sun/yr (scientific notation like 2e-6 is accepted).
3
Use a preset - Click Cygnus X-1 (BH HMXB), Her X-1 (NS X-ray pulsar), Sco X-1 (NS LMXB near Eddington), or M33 X-7 (extragalactic massive BH) to load real observed parameters.
4
Read the results - Get accretion luminosity in watts and solar luminosities, Eddington luminosity, Eddington ratio, Eddington accretion rate, and automatic classification as BH XRB, NS LMXB, ULX, or sub-Eddington accretor.

💡 Example Calculations

Example 1 - Cygnus X-1 (Black Hole HMXB)

M = 21.2 M☉, R = 50 km (ISCO), η = 0.057, Ṁ = 2.5×10⁻⁸ M☉/yr

1
Convert accretion rate: 2.5 × 10−8 M⊙/yr = 2.5 × 10−8 × 1.989 × 1030 / 3.156 × 107 = 1.58 × 1015 kg/s
2
Accretion luminosity: L = 0.057 × 1.58 × 1015 × (2.998 × 108)2 = 8.07 × 1030 W
3
Eddington luminosity: LEdd = 4pi × G × 21.2 M⊙ × mp × c / σT = 2.67 × 1032 W; Cygnus X-1 is sub-Eddington at ~3% LEdd in its hard state
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Example 2 - Sco X-1 (Neutron Star LMXB near Eddington)

M = 1.4 M☉, R = 10 km, η = 0.20, Ṁ = 10⁻⁸ M☉/yr

1
High efficiency (eta = 0.20) for NS: deep potential well and surface boundary layer add energy to the disk luminosity alone
2
Accretion luminosity: L = 0.20 × (10−8 × 1.989 × 1030 / 3.156 × 107) × c2 = 3.6 × 1029 W
3
Eddington luminosity for 1.4 M⊙: LEdd = 1.76 × 1031 W; Sco X-1 operates at about 0.02 LEdd (bright persistent LMXB)
L ≈ 3.6 × 1029 W | LEdd = 1.76 × 1031 W | fEdd0.02 | NS LMXB / HMXB
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Example 3 - ULX Source (Super-Eddington BH)

M = 10 M☉, Eddington fraction = 10 × L_Edd

1
Eddington luminosity: LEdd = 4pi × G × 10 M⊙ × mp × c / σT = 1.26 × 1032 W
2
Actual luminosity at 10 LEdd: L = 10 × 1.26 × 1032 = 1.26 × 1033 W = 3.3 × 106 L⊙
3
Required Mdot (eta = 0.1): 1.4 × 10−6 M⊙/yr — super-Eddington accretion likely drives powerful outflows and beaming
L = 1.26 × 1033 W | 3.3 × 106 L⊙ | Ultraluminous X-ray Source (ULX)
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❓ Frequently Asked Questions

What is an X-ray binary?+
An X-ray binary (XRB) is a two-star system where a compact object (neutron star or black hole) accretes matter from a companion star. As matter falls through an accretion disk and releases gravitational energy, it heats to millions of degrees and radiates primarily in X-rays. XRBs are classified as HMXBs (companion mass above ~10 M_sun, wind accretion) or LMXBs (companion below ~2 M_sun, Roche-lobe overflow), and include transient and persistent sources.
What is the formula for accretion luminosity?+
Accretion luminosity is L = eta * Mdot * c^2, where eta is the radiative efficiency and Mdot is the mass accretion rate. Typical values: eta = 0.057 for a Schwarzschild BH (ISCO at 6 rg), eta = 0.15 to 0.25 for neutron stars (surface boundary layer included), eta up to 0.42 for maximally spinning Kerr BH (ISCO at 1.24 rg). This formula makes accretion the most efficient non-nuclear energy source known.
What is the Eddington luminosity and why does it matter?+
The Eddington luminosity L_Edd = 4*pi*G*M*m_p*c/sigma_T is the luminosity at which radiation pressure equals gravity for spherically symmetric electron scattering. It scales linearly with mass: L_Edd ~ 1.26 x 10^31 * (M/M_sun) W. Exceeding L_Edd halts spherically symmetric infall. However, disk geometry, magnetic support, and beaming allow super-Eddington emission in ULXs and are studied in detail with modern X-ray observatories.
What is radiative efficiency and what values are expected?+
Radiative efficiency eta is the fraction of accreted rest-mass energy emitted as radiation. For Schwarzschild BH: eta = 1 - sqrt(1 - 2/3 * rs/r_ISCO) where rs is the Schwarzschild radius. For r_ISCO = 6rs, eta ~ 0.057 (5.7%). For maximally spinning Kerr BH, r_ISCO ~ 1.24rs gives eta ~ 0.42 (42%). For neutron stars with hard surfaces, eta ~ GM/(Rc^2) + disk contribution ~ 0.15 to 0.25. Radiatively inefficient accretion flows (ADAFs) at very low Mdot have eta approaching zero.
What are high-mass vs low-mass X-ray binaries?+
HMXBs have early-type OB companion stars (M above ~10 M_sun) that fill their Roche lobe or drive strong winds. Examples: Cygnus X-1, Vela X-1, 4U 0115+63. Mass transfer is driven by stellar winds or Roche-lobe overflow. LMXBs have late-type companions (M below ~2 M_sun, typically K or M stars) filling their Roche lobes. Mass transfer is slower and accretion is disk-dominated. Examples: Sco X-1, 4U 1820-30, XTE J1550-564. LMXBs dominate the bright persistent XRB population.
What are ultraluminous X-ray sources?+
ULXs are X-ray point sources with luminosity above ~10^33 W (10^39 erg/s), exceeding L_Edd for a 10 M_sun BH. They are found in nearby galaxies, typically off-nucleus. Proposed explanations: (1) super-Eddington accretion onto stellar-mass BHs (10 to 100 M_sun) with funnel beaming and radiative-wind driven columns; (2) intermediate-mass BHs (100 to 10^5 M_sun); (3) strongly magnetized neutron stars where the cyclotron resonance scattering increases effective L_Edd. Multiple mechanisms likely contribute across the ULX population.
How is Cygnus X-1 classified and what are its parameters?+
Cygnus X-1 is a HMXB with a confirmed black hole (mass 21.2 M_sun, measured from the orbital motion of its companion HDE 226868). It accretes primarily from the strong stellar wind of the 41 M_sun O-supergiant companion at about 2 x 10^-6 M_sun/yr. In its hard state it radiates at ~2% Eddington with a power-law X-ray spectrum. In its softer state the spectrum peaks in the UV/soft X-ray, consistent with a hotter thermal disk extending closer to the BH. It alternates between hard and soft spectral states on timescales of months.
What is the relationship between X-ray luminosity and mass transfer rate in LMXBs?+
In a persistent LMXB, the X-ray luminosity directly tracks the mass transfer rate through L = eta*Mdot*c^2. For a NS LMXB near Eddington (Mdot ~ 10^-8 M_sun/yr, eta ~ 0.2), L ~ 3.5 x 10^29 W ~ 10^5 L_sun. Transient LMXBs undergo outbursts triggered by the thermal-viscous disk instability model (DIM): at low Mdot the disk is cold and neutral; when it heats past the hydrogen ionization threshold (~6,500 K), viscosity jumps and a large disk reservoir drains rapidly, producing an X-ray outburst lasting weeks to months.
What X-ray telescopes observe XRBs?+
Current major observatories: Chandra (0.5-10 keV, subarcsecond imaging), XMM-Newton (0.15-15 keV, high throughput), NuSTAR (3-79 keV, first hard X-ray focusing telescope), NICER (0.2-12 keV, microsecond timing for NS). Historical: UHURU (first systematic survey, discovered Cygnus X-1 in 1964), EXOSAT, Ginga, ROSAT, RXTE (energetic X-ray transient survey), Swift (GRB + transient monitoring). Planned: eXTP, STROBE-X (timing and spectroscopy of NS/BH systems).
How does XRB accretion compare to AGN accretion?+
Both are powered by L = eta*Mdot*c^2, but scales differ by 10^6 to 10^9 in mass. A typical stellar BH XRB (10 M_sun) at Eddington luminosity emits ~10^32 W. A Seyfert galaxy AGN (10^8 M_sun) at 10% Eddington emits ~10^38 W. Because XRB variability timescales are seconds to months while AGN timescales are years to millennia, XRBs allow study of the complete spectral-state cycle within a human lifetime, making them the best laboratories for understanding AGN disk physics.

What is an X-ray binary?

An X-ray binary (XRB) is a two-star system in which one component is a compact object (neutron star or black hole) that accretes matter from its companion star. As material falls onto the compact object, gravitational potential energy is released as X-ray emission. XRBs are among the brightest X-ray sources in the sky and are divided by companion type: high-mass X-ray binaries (HMXBs) with OB supergiant donors, and low-mass X-ray binaries (LMXBs) with Roche-lobe-filling late-type companions.

What is the formula for accretion luminosity?

Accretion luminosity is L = eta * Mdot * c^2, where eta is the radiative efficiency (fraction of rest-mass energy radiated), Mdot is the mass accretion rate in kg/s, and c is the speed of light. This is derived from the gravitational potential energy released as material falls from infinity onto the compact object surface or innermost stable orbit. For a neutron star of mass M and radius R, the Newtonian estimate gives eta ~ GM/(Rc^2) ~ 0.2 for R = 10 km.

What is the Eddington luminosity and why is it important?

The Eddington luminosity L_Edd = 4*pi*G*M*m_p*c / sigma_T is the maximum luminosity at which radiation pressure on free electrons exactly balances gravitational attraction. For spherically symmetric accretion of hydrogen plasma, L_Edd ~ 1.3 x 10^31 * (M/M_sun) watts. Sources exceeding L_Edd cannot maintain steady spherical accretion, though super-Eddington emission is observed in ULXs via beamed, disk-driven, or magnetically dominated flows.

What is radiative efficiency eta and what values are expected?

Radiative efficiency eta is the fraction of accreted rest-mass energy (Mdot*c^2) that emerges as radiation rather than falling into the compact object or being advected. For Schwarzschild BHs (non-spinning), the ISCO is at 6 GM/c^2 and eta ~ 0.057. For maximally spinning Kerr BHs, the ISCO is at 1.24 GM/c^2 and eta ~ 0.42. Neutron stars with solid surfaces retain all infalling kinetic energy as heat, giving eta typically 0.15 to 0.25. Advection-dominated accretion flows (ADAFs) at low Mdot can have very low effective eta.

What is the Eddington accretion rate?

The Eddington accretion rate is the mass transfer rate at which accretion at efficiency eta produces exactly L_Edd: Mdot_Edd = L_Edd/(eta*c^2) = 4*pi*G*M*m_p/(eta*sigma_T*c). For a 10 M_sun BH with eta = 0.1, Mdot_Edd ~ 1.4 x 10^-7 M_sun/yr. This is a characteristic rate used to normalize observed accretion rates and compare across source types.

What are high-mass vs low-mass X-ray binaries?

High-mass X-ray binaries (HMXBs) have companion stars more massive than about 10 M_sun, typically OB supergiants or Be stars. The compact object accretes from the stellar wind. Examples: Cygnus X-1 (BH + O supergiant), Vela X-1 (NS + B supergiant). Low-mass X-ray binaries (LMXBs) have companions below about 2 M_sun, typically K or M stars filling their Roche lobe. Accretion is through an accretion disk. Examples: Sco X-1, Her X-1, XTE J1550-564.

What are ultraluminous X-ray sources (ULXs)?

ULXs are off-nucleus X-ray point sources with luminosity above ~10^33 W (10^39 erg/s), exceeding the Eddington limit for a 10 M_sun BH. They are found in nearby galaxies and may represent super-Eddington accretion onto stellar-mass compact objects (with beamed, wind-confined emission), intermediate-mass black holes (100 to 100,000 M_sun), or highly magnetized neutron stars (pulsating ULXs, where the strong B-field modifies the Eddington limit).

How is X-ray luminosity related to mass transfer rate in LMXBs?

In an LMXB, the donor star fills its Roche lobe and transfers mass through the L1 Lagrange point at a rate set by the companion's evolutionary state. The accretion disk channels this material onto the compact object. The X-ray luminosity directly tracks the mass transfer rate through L = eta*Mdot*c^2. Transient LMXBs show outbursts when disk instability triggers a sudden increase in Mdot, while persistent LMXBs (like Sco X-1) maintain steady accretion.

What X-ray missions observe these sources?

Key X-ray observatories include: Chandra (subarcsecond imaging, 0.5-10 keV), XMM-Newton (high throughput, 0.15-15 keV), NuSTAR (hard X-ray focusing, 3-79 keV), NICER (neutron star timing, 0.2-12 keV), and eROSITA (all-sky survey). Historical missions include UHURU (first systematic X-ray survey, discovered Cygnus X-1), EXOSAT, ROSAT, RXTE, and Swift. Together they have catalogued thousands of X-ray binaries in the Milky Way and nearby galaxies.

What is the difference between an XRB and an AGN?

Both X-ray binaries and active galactic nuclei (AGN) are powered by accretion onto compact objects, but the scales differ by 10^6 to 10^9. A typical XRB has a stellar-mass BH (3 to 100 M_sun) and X-ray luminosity of 10^30 to 10^32 W. An AGN harbors a supermassive BH (10^6 to 10^10 M_sun) with bolometric luminosity up to 10^40 W. The same physics (L = eta*Mdot*c^2, L_Edd = 4pi*G*M*m_p*c/sigma_T) governs both, making XRBs useful laboratories for understanding AGN on human timescales.

What is Cygnus X-1 and why is it important?

Cygnus X-1 was discovered in 1964 and became the first source widely identified as a black hole (dynamical mass measurement via orbital motion of its companion HDE 226868 showed M > 3 M_sun). The BH mass is now measured at 21.2 M_sun. It is a HMXB accreting from the stellar wind of a 41 M_sun O-type supergiant at a rate of about 2 x 10^-6 M_sun/yr. In its hard state it radiates at about 2% Eddington as a bright X-ray source detectable with simple instruments.