In planetary sciences, the moment of inertia factor or normalized polar moment of inertia is a dimensionless quantity that characterizes the radial distribution of mass inside a planet or satellite. Since a moment of inertia has dimensions of mass times length squared, the moment of inertia factor is the coefficient that multiplies these.
Definition
For a planetary body with principal moments of inertia 
,
where C is the first principal moment of inertia of the body, M is the mass of the body, and R is the mean radius of the body.[1][2] For a sphere with uniform density, 
Solar System values
The Sun has by far the lowest moment of inertia factor value among Solar System bodies; it has by far the highest central density (162 g/cm3,[3][note 3] compared to ~13 for Earth[4][5]) and a relatively low average density (1.41 g/cm3 versus 5.5 for Earth). Saturn has the lowest value among the gas giants in part because it has the lowest bulk density (0.687 g/cm3).[6] Ganymede has the lowest moment of inertia factor among solid bodies in the Solar System because of its fully differentiated interior,[7][8] a result in part of tidal heating due to the Laplace resonance,[9] as well as its substantial component of low density water ice. Callisto is similar in size and bulk composition to Ganymede, but is not part of the orbital resonance and is less differentiated.[7][8] The Moon is thought to have a small core, but its interior is otherwise relatively homogenous.[10][11]
| Body | Value | Source | Notes |
|---|---|---|---|
| Sun | 0.070 | [3] | Not measured |
| Mercury | 0.346 ± 0.014 | [12] | |
| Venus | 0.337 ± 0.024 | [13] | |
| Earth | 0.3307 | [14] | |
| Moon | 0.3929 ± 0.0009 | [15] | |
| Mars | 0.3644 ± 0.0005 | [16] | |
| Ceres | 0.36 ± 0.15[note 4] | [18] | Not measured (range reflects different assumptions for original spin rate[18]) |
| Jupiter | 0.2756 ± 0.0006 | [19] | Not measured (two-layer model calculations constrained by Juno gravity data[19]) |
| Io | 0.37824 ± 0.00022 | [20] | Not measured (Darwin-Radau relation) |
| Europa | 0.346 ± 0.005 | [20] | Not measured (Darwin-Radau relation) |
| Ganymede | 0.3115 ± 0.0028 | [20] | Not measured (Darwin-Radau relation) |
| Callisto | 0.3549 ± 0.0042 | [20] | Not measured (Darwin-Radau relation) |
| Saturn | 0.22 | [21] | Not measured (Darwin-Radau relation) |
| Enceladus | 0.3305 ± 0.0025 | [22] | Not measured (Darwin-Radau relation) |
| Rhea | 0.3911 ± 0.0045 | [23] | Not measured (Darwin-Radau relation) |
| Titan | 0.341 | [24] | Not measured (Darwin-Radau relation) |
| Uranus | 0.23 | [25] | Not measured (approximate solution to Clairaut's equation) |
| Neptune | 0.23 | [25] | Not measured (approximate solution to Clairaut's equation) |
Measurement
The polar moment of inertia is traditionally determined by combining measurements of spin quantities (spin precession rate and/or obliquity) with gravity quantities (coefficients of a spherical harmonic representation of the gravity field). These geodetic data usually require an orbiting spacecraft to collect.
Approximation
For bodies in hydrostatic equilibrium, the Darwin–Radau relation can provide estimates of the moment of inertia factor on the basis of shape, spin, and gravity quantities.[26]
Role in interior models
The moment of inertia factor provides an important constraint for models representing the interior structure of a planet or satellite. At a minimum, acceptable models of the density profile must match the volumetric mass density and moment of inertia factor of the body.
