Cosmology · Gravity and an expanding Universe
Uniformity as a large-scale approximation
Galaxies form a cosmic web, yet a smooth background can still be useful. Learn exactly what is averaged, how spatial symmetries differ, and what observations can test without pretending to survey the whole Universe.
Preparation: ratios, powers of ten and ordinary arithmetic. Physical quantities and notation are introduced as they are needed.
Back to the chapterAfter reading, you can
- Distinguish homogeneity, isotropy and point-by-point uniformity.
- Explain how an averaging scale and tracer selection enter a uniformity test.
- Keep finite observational support separate from extrapolation beyond the observed region.
How can a clumpy Universe have a smooth description?
A small region containing a galaxy and a small region in a void are plainly different. A model that assigned the same matter density to every real point would miss that structure. The smooth cosmological background makes a more limited choice: it averages over small-scale detail in order to describe large-scale geometry and evolution.
The choice resembles reporting a city's average population density while retaining a separate map of its crowded and empty places. An average can answer one question without reproducing every local feature. It becomes misleading when it is used at a scale where the differences being discarded determine the answer.
For the real Universe, large-scale uniformity is statistical. Comparable regions are not required to contain precisely the same number of galaxies or identical patterns. Rather, appropriately defined averages and fluctuations can be tested for consistency with a common statistical description. Which quantities, smoothing scale and acceptable differences are used must be stated.
Changing position differs from changing direction
Homogeneity concerns translations between places: in a homogeneous description, no location has special statistical properties. Isotropy concerns directions: in an isotropic description, no direction has special statistical properties. The ideal homogeneous and isotropic cosmological background imposes both spatial symmetries on each cosmic-time slice.
The two ideas cannot be exchanged without extra assumptions. Imagine a model whose density changes with distance from one central point but is the same in every direction around that point. A central observer finds directional symmetry, yet another location is different. Isotropy about that one point has not established homogeneity.
The spatial conditions also do not mean that nothing changes with time. The background density and temperature can evolve while the model remains homogeneous and isotropic at each epoch. Comparing an early region with a later one is a different test from comparing two regions at the same cosmic time.
Our approximate cosmic rest frame is also relevant. An observer moving relative to that frame can see a directional pattern caused by motion. A measured sky pattern therefore needs interpretation before it becomes a statement about preferred spatial directions in the background.
Averages need a window and a denominator
Define a toy number density n = N/V, where N is a count of selected objects and V is the sampled volume. Number density is not automatically mass density: two samples can contain the same number of objects with different masses. For this exercise each small cell has one chosen volume unit, written u³, where u is an invented length unit.
Region A has four equal cells with counts 0, 8, 2 and 6. Region B has counts 7, 1, 6 and 2. Each region contains 16 objects in 4 u³, giving the same average n = 4 objects per u³. The local counts still range from zero to eight. Larger-window agreement and small-cell contrast coexist in this deliberately constructed example.
That arithmetic does not prove that every arrangement becomes homogeneous if we average long enough. A persistent gradient or other large-scale structure can survive the averaging. Nor do two equal averages establish a complete common probability distribution. Tests need multiple windows, uncertainty estimates and statistics chosen to address the actual proposed symmetry.
Averages over overlapping windows are correlated because some of the same objects occur in more than one window. Counting them as fully independent repetitions exaggerates the information available. Survey boundaries and the finite observed region also limit the windows that can be compared.
| Region | Four cell counts | Total count | Volume in u³ | Average in objects/u³ |
|---|---|---|---|---|
| A | 0, 8, 2, 6 | 16 | 4 | 4 |
| B | 7, 1, 6, 2 | 16 | 4 | 4 |
A telescope does not deliver an unbiased volume census
A galaxy survey samples objects meeting detection and selection conditions. Fainter objects can be missed, the sky coverage can be irregular, and the conversion from observed redshift to a spatial volume uses a cosmological model. A raw decline in detected counts with distance is therefore not by itself a cosmic density gradient.
In a synthetic comparison, suppose two equal volumes each contain 100 objects of the chosen population. A survey detects 80 percent in the first and 40 percent in the second, so its recorded counts are 80 and 40. Correcting by independently justified completeness fractions gives 80/0.80 = 100 and 40/0.40 = 100. Without that information, the data alone leave population and detection effects mixed.
A completeness correction is itself an inference to test. Assuming exactly the trend one hopes to establish could conceal a real difference. Useful analyses check selection with instrument information, simulations or other observations and propagate the resulting uncertainty. They also compare the same defined population, rather than silently swapping galaxy types between regions.
The 2012 WiggleZ homogeneity analysis illustrates a quantitative survey test using counts in spheres and their scale dependence, with selection, survey geometry and a fiducial distance model. Its result concerns that sample and operational criterion. It does not define one universal exact length beyond which every structure must disappear.
What the microwave sky adds—and what it cannot show alone
The cosmic microwave background provides a different kind of evidence: nearly uniform radiation across the sky, with small temperature variations. Our detector also receives foreground emission. Separating these components and accounting for motion and instrumental response are part of using the sky to test cosmological assumptions.
The Planck 2018 isotropy and statistics analysis, published in 2020, reported broad statistical consistency with its standard cosmological framework while retaining large-angle temperature anomalies and limitations associated with polarization systematics. This is a dated example of a qualified test, not a claim that exact isotropy was proved or that all open tests were settled in 2026.
We observe distant regions through arriving signals emitted at earlier times. We cannot simply inspect a simultaneous three-dimensional census from every possible location, and we have no direct observations of the entire unobservable Universe. Inferring spatial uniformity combines finite data, physical modelling and an assumption that our location is not specially privileged.
A smooth background is valuable because it makes clear predictions that can be refined with perturbations and confronted with observations. Preserve both sides of the statement: there is substantial observational motivation for the approximation, and its domain and extrapolations remain explicit. A striking filament is not automatically a refutation of statistical uniformity; a suspected inconsistency is not automatically something averaging can dismiss.
Worked reasoning
Compare equal quantities
A complete synthetic sample has 20 objects in 2 u³ and 30 objects in 5 u³. Which region has the larger number density?
- Compute the first density: 20/2 = 10 objects/u³.
- Compute the second: 30/5 = 6 objects/u³.
- Compare the densities, rather than counts drawn from unequal volumes.
The first region is denser in this sample, even though the second contains more objects. A significance claim would additionally need a statistical model and uncertainty.
Try the reasoning
A model is directionally identical about one chosen point, but its density increases with distance from that point. Is it homogeneous?
Show the answer and reasoning
No.
The selected centre is a special location. Directional symmetry about it does not establish equivalence between different places.
Do the equal four-cell means in the supplied toy prove that the whole point distribution is homogeneous?
Show the answer and reasoning
No.
They establish only those two averages. Other scales, windows and statistical properties can differ, and unobserved regions were not tested.
Two equal volumes yield 60 and 30 detected objects. Can those raw counts alone distinguish a density difference from a completeness difference?
Show the answer and reasoning
No.
The detected sample combines the underlying population and the probability of detecting and selecting its members. Additional information is needed to separate them.
What to carry forward
- A statistical large-scale approximation can coexist with galaxies, voids and filaments.
- Homogeneity compares locations; isotropy compares directions; neither forbids temporal evolution.
- A meaningful uniformity test states its tracer, volume, averaging scale, selection and uncertainty.
- Galaxy surveys and the microwave sky supply finite model-informed evidence, not direct access to every place in the total Universe.
References
Sources supporting the explanations, physical distinctions and examples in this lesson.
- Cosmology,1: The Expanding UniverseDavid TongCourse notes
- The WiggleZ Dark Energy Survey: the transition to large-scale cosmic homogeneityMorag I. Scrimgeour and collaboratorsResearch paper
- Planck2018 results.VII: Isotropy and Statistics of the CMBPlanck CollaborationResearch paper
- Planck and the cosmic microwave backgroundEuropean Space AgencyTeaching resource
- CMB ObservationsU.S. Planck Data Center / IPAC, CaltechTeaching resource