A quantitative comparison of higher-order chromatin arrangements was perfor
med in human cell types with three-dimensionally (3D) preserved, differentl
y shaped nuclei. These cell types included flat-ellipsoid nuclei of diploid
amniotic fluid cells and fibroblasts and spherical nuclei of B and T lymph
ocytes from peripheral human blood. Fluorescence in-situ hybridization (FIS
H) was performed with chromosome paint probes for large (#1-5) and small (#
17-20) autosomes, and for the two sex chromosomes. Other probes delineated
heterochromatin blocks of numerous larger and smaller human chromosomes. Sh
ape differences correlated with distinct differences in higher order chroma
tin arrangements: in the spherically shaped lymphocyte nuclei we noted the
preferential positioning of the small, gene dense #17, 19 and 20 chromosome
territories (CTs) in the 3D nuclear interior - typically without any appar
ent connection to the nuclear envelope. In contrast, CTs of the gene-poor s
mall chromosomes #18 and Y were apparently attached at the nuclear envelope
. CTs of large chromosomes were also preferentially located towards the nuc
lear periphery. In the ellipsoid nuclei of amniotic fluid cells and fibrobl
asts, all tested CTs showed attachments to the upper and/or lower part of t
he nuclear envelope: CTs of small chromosomes, including #18 and Y, were lo
cated towards the centre of the nuclear projection (CNP), while the large c
hromosomes were positioned towards the 2D nuclear rim. In contrast to these
highly reproducible radial arrangements, 2D distances measured between het
erochromatin blocks of homologous and heterologous CTs were strikingly vari
able. These results as well as CT painting let us conclude that nuclear fun
ctions in the studied cell types may not require reproducible side-by-side
arrangements of specific homologous or non-homologous CTs. 3D-modelling of
statistical arrangements of 46 human CTs in spherical nuclei was performed
under the assumption of a linear correlation between DNA content of each ch
romosome and its CT volume. In a set of modelled nuclei, we noted the prefe
rential localization of smaller CTs towards the 3D periphery and of larger
CTs towards the 3D centre. This distribution is in clear contrast to the ex
perimentally observed distribution in lymphocyte nuclei. We conclude that p
resently unknown factors (other than topological constraints) may play a de
cisive role to enforce the different radial arrangements of large and small
CTs observed in ellipsoid and spherical human cell nuclei.