Compute packing fraction for mixtures using several particle shapes quickly and accurately. Choose container geometry, convert units, then download reports for your experiments easily.
Set container geometry, units, and up to three particle components.
| Case | Container | Particles | Packing fraction φ |
|---|---|---|---|
| 1 | Box 10×10×10 cm | Sphere d=1 cm, N=1222 | 0.6398 |
| 2 | Cylinder r=5 cm, h=20 cm | Cube a=1 cm, N=911 | 0.5800 |
| 3 | Direct volume 2000 cm³ | Ellipsoid a=0.5 cm, b=0.4 cm, c=0.3 cm, N=5000 | 0.6283 |
The packing fraction is the ratio of solid volume to container volume: φ = Vparticles / Vcontainer. Porosity is ε = 1 − φ.
v = π d³ / 6v = π r² hv = a³v = (4/3) π a b cVparticles = Σ Nᵢ vᵢThe packing fraction φ is the volume share occupied by solids inside a container. For granular materials, foams, and particulate suspensions, φ connects directly to density, permeability, and mechanical response. This calculator evaluates φ from geometry, then reports porosity ε = 1 − φ for transport and flow work.
For equal, frictional spheres poured without strong vibration, random loose packing is often around 0.55–0.60. With moderate agitation, random close packing commonly clusters near 0.64. The crystalline benchmark (face-centered cubic or hexagonal close packed) reaches about 0.7405, showing the gap between disordered and ordered structure.
Near walls, particles arrange differently than in the bulk, lowering or raising local φ depending on size and friction. Tall cylinders can show vertical gradients after tapping, while shallow boxes exaggerate wall layers. Using the same container in repeated tests reduces systematic bias and makes φ comparisons more meaningful.
Polydispersity can increase φ because smaller particles fill voids between larger ones. Well-chosen bimodal blends may exceed monodisperse random close packing and approach 0.68–0.72 in some laboratory protocols. The calculator supports multiple components so you can estimate the solid-volume sum from counts and per-particle volumes.
Non-spherical grains change how voids interlock. Cylinders, cubes, and ellipsoids can pack more densely or more loosely depending on aspect ratio and alignment. Mildly elongated or flattened ellipsoids may reach higher random packing than spheres, while strongly angular shapes often lock earlier, producing higher friction and different porosity trends.
Porosity ε determines how much void space is available for fluid flow, diffusion, and acoustic attenuation. For example, if φ = 0.62 then ε = 0.38, meaning 38% of the container volume is void. When comparing samples, keep the same compaction method because ε is highly process dependent.
If φ exceeds 1, either particle volumes or container dimensions are inconsistent, or a unit conversion is wrong. In real experiments, uncertainty is dominated by count errors, diameter tolerances, and container measurement. Reporting φ with 3–4 significant figures is often appropriate unless metrology is exceptionally tight.
The CSV export is convenient for lab notebooks and parameter sweeps, while the PDF summary is useful for attaching to experimental runs. In modeling, φ and ε can be fed into continuum closures, effective medium estimates, or initial conditions for discrete element simulations. Consistent assumptions make comparisons reliable and repeatable.
No. It depends on friction, preparation method, size spread, and boundaries. Values near 0.64 are common for equal spheres, but different protocols can shift the measured fraction noticeably.
Your inputs may describe non-spherical particles, mixtures, or a different compaction state. Also check units and whether counts and dimensions reflect the same measurement basis.
It is φ divided by your chosen benchmark value. A value of 1.00 matches the benchmark; 0.90 is 10% lower; 1.05 is 5% higher.
Yes, as an estimate. Enter a representative particle volume for a “custom” component or approximate with a simple shape. Irregularity mainly affects the true volume and the achievable packing state.
Use an average diameter from calipers, microscopy, or sieve data, and include uncertainty. Small diameter errors amplify because sphere volume scales with d³.
For hard particles, φ cannot exceed 1. Ordered sphere packing tops out near 0.7405. Results above these bounds almost always indicate inconsistent geometry or units.
Not fully. Permeability also depends on pore connectivity, tortuosity, particle size, and shape. Porosity is a key input, but flow models typically require additional microstructural information.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.