PhysSandbox
Classical MechanicsWaves & SoundElectricity & MagnetismOptics & LightGravity & OrbitsLabs
🌙Astronomy & The Sky🌡️Thermodynamics🌍Biophysics, Fluids & Geoscience📐Math Visualization🔧Engineering🧪Chemistry

More from Astronomy & The Sky

Other simulators in this category — or see all 51.

View category →
NewSchool

Exoplanet Transit (limb darkening u₁, u₂)

Quadratic limb-darkened disk; grid-integrated F(t); TESS-like solar preset vs uniform-disk page.

Launch Simulator
NewUniversity / research

Sphere of Influence (Hill)

r_H ≈ a (m/3M)^(1/3): schematic secondary orbit and Hill radius vs masses and a.

Launch Simulator
NewSchool

Measuring c (ToF toy)

c ≈ 2D/Δt round-trip; schematic path + Fizeau/Foucault context.

Launch Simulator
NewUniversity / research

GPS & Relativity

Weak-field + SR clock drift estimates vs altitude and orbital speed.

Launch Simulator
NewSchool

Nuclear Binding Curve

Qualitative B/A vs A with fusion/fission context.

Launch Simulator
NewSchool

Seasons & Axial Tilt

Obliquity ~23.4°: declination model vs day of year and noon sun altitude at latitude.

Launch Simulator
PhysSandbox

Interactive physics, chemistry, and engineering simulators for students, teachers, and curious minds.

Physics

  • Classical Mechanics
  • Waves & Sound
  • Electricity & Magnetism

Science

  • Optics & Light
  • Gravity & Orbits
  • Astronomy & The Sky

More

  • Thermodynamics
  • Biophysics, Fluids & Geoscience
  • Math Visualization
  • Engineering
  • Chemistry

© 2026 PhysSandbox. Free interactive science simulators.

PrivacyTermsContact
Home/Astronomy & The Sky/Exoplanet Transit (light curve)

Exoplanet Transit (light curve)

For a star modeled as a uniformly bright disk, a planet of radius R_p transiting at separation ρ between centers blocks flux in proportion to the geometric overlap area of two circles divided by πR_*². With ρ² = b² + (vt)² for impact parameter b in units of stellar radius, ingress and egress durations grow for grazing geometries. Limb darkening, stellar spots, blended binaries, and instrumental systematics are omitted.

Who it's for: Introductory exoplanet detection; pairs with radial-velocity pages and stellar parallax.

Key terms

  • transit photometry
  • impact parameter
  • transit depth
  • orbital period

Live graphs

Transit photometry (uniform disk)

0.12
0.15
1.05
3.5 d

**Uniform disk** star: blocked flux equals the **overlap area** of two circles divided by **πR_*²**. **Central** transit (**b ≈ 0**): minimum flux **≈ 1 − (R_p/R_*)²**. **Limb darkening** and **blending** omitted — qualitative.

Shortcuts

  • •Central transits (small b) give deeper, boxier dips; grazing transits are V-shaped

Measured values

Approx. depth (1 − F_min)0.014400
Depth (ppm)14400.0 ppm
Period (display)3.50 d

How it works

When a planet passes in front of its star (transit), the observed flux drops by the fraction of the stellar disk covered, for a uniform brightness disk: **ΔF/F ≈ (R_p/R_*)² for a central transit. Grazing transits (impact parameter b approaching 1) have longer ingress/egress and smaller depth. Time between transits gives the orbital period; depth and duration constrain size and inclination together with stellar radius. Real light curves add limb darkening, star spots, and noise**.

Key equations

F/F₀ = 1 − A_overlap(ρ) / (πR_*²) · ρ = √(b² + (vt)²)
Central: ΔF/F ≈ (R_p/R_*)²

Frequently asked questions

Why ppm for Earth-sized planets?
For a Sun-like star, (R_⊕/R_☉)² is of order 10⁻⁴, so depths are roughly 100 ppm before noise and stellar variability.
Does this give the planet mass?
Not by itself — transits yield radius and period (with stellar mass). Mass typically needs radial velocities or timing variations.