Causal set theory is an approach to quantum gravity in which spacetime is fundamentally discrete: instead of a smooth manifold with a metric at every point, the basic structure is a set of elementary “events” equipped with a causal (before/after) relation. In many presentations, one imagines obtaining a causal set by sprinkling elements into a continuum spacetime via a Poisson process with a fixed density—typically taken to be roughly one element per Planck 4‑volume. In that idealized picture, the expected number of elements in a spacetime region is approximately its 4‑volume divided by the Planck 4‑volume.
This page implements that simple estimate for a spherical spatial region of radius R observed for a time interval T. You provide R (in light‑years) and T (in years). The calculator converts them into SI units, computes an approximate 4‑volume, and returns the corresponding expected element count.
We approximate the region as a spatial ball (a 3D sphere including its interior) of radius R, with spatial 3‑volume:
Spatial volume:
To form a 4‑volume, we multiply by a time extent expressed as a length using the speed of light c. If T is a duration (seconds), then cT has units of meters, so:
4‑volume (flat‑spacetime, no expansion):
The Planck length is
Planck length: lP = 1.616255 × 10−35 m
so the Planck 4‑volume scale is:
Planck 4‑volume: lP4 (units of m4)
Finally, the expected number of sprinkled elements is:
Expected element count:
The output is an expected value (mean) under the “one element per Planck 4‑volume” density assumption. Because the Planck scale is extraordinarily small, even everyday spacetime regions correspond to enormous counts. That does not mean we can directly observe these elements—only that, in the causal set hypothesis, the discrete structure would have to be extremely dense to recover a smooth-looking continuum at macroscopic scales.
Also note that if sprinkling is modeled as a Poisson process with mean N, then typical fluctuations are of order sqrt(N). For such huge N, the relative fluctuation sqrt(N)/N is tiny, so the mean is a good summary; for small regions (still far larger than Planck scale in most user inputs), discreteness noise could matter conceptually.
Example: radius R = 1 light‑year, duration T = 1 year.
R = 9.4607×10^15 m, T = 3.15576×10^7 s.V3 = (4/3)πR^3 (in m3).V4 = V3·c·T (in m4).lP^4 to get N.The resulting N will be astronomically large, reflecting the tiny Planck 4‑volume. Use this as an order‑of‑magnitude intuition-builder rather than a precision prediction about our universe.
The estimate scales as N ∝ R^3 T. Doubling the radius multiplies N by 8; doubling the duration multiplies N by 2.
| Scenario | Radius R | Duration T | Relative scaling vs (1 ly, 1 yr) |
|---|---|---|---|
| Baseline | 1 ly | 1 yr | 1× |
| Half the radius | 0.5 ly | 1 yr | (0.5)3 = 1/8 |
| Double the radius | 2 ly | 1 yr | 23 = 8× |
| Ten times the duration | 1 ly | 10 yr | 10× |
| Double radius and duration | 2 ly | 2 yr | 8× · 2× = 16× |
(4/3)πR^3. It does not incorporate general relativistic curvature.It’s the fourth power of the Planck length, lP^4, which sets a characteristic spacetime volume scale in approaches that treat discreteness as Planckian.
No. This calculator assumes a causal set–style density and reports what that assumption would imply for a region’s 4‑volume. It’s a way to build intuition, not evidence.
To express the time interval as a length so that multiplying a 3‑volume (m3) by a length (m) gives a 4‑volume (m4) in a simple flat-spacetime model.