Retinitis pigmentosa: rapid neurodegeneration is governed by slow cell death mechanisms

For most neurodegenerative diseases the precise duration of an individual cell''s death is unknown, which is an obstacle when counteractive measures are being considered. To address this, we used the rd1 mouse model for retinal neurodegeneration, characterized by phosphodiesterase-6 (PDE6) dysfunction and photoreceptor death triggered by high cyclic guanosine-mono-phosphate (cGMP) levels. Using cellular data on cGMP accumulation, cell death, and survival, we created mathematical models to simulate the temporal development of the degeneration. We validated model predictions using organotypic retinal explant cultures derived from wild-type animals and exposed to the selective PDE6 inhibitor zaprinast. Together, photoreceptor data and modeling for the first time delineated three major cell death phases in a complex neuronal tissue: (1) initiation, taking up to 36 h, (2) execution, lasting another 40 h, and finally (3) clearance, lasting about 7 h. Surprisingly, photoreceptor neurodegeneration was noticeably slower than necrosis or apoptosis, suggesting a different mechanism of death for these neurons.     

Budding yeast morphogenesis: signalling, cytoskeleton and cell cycle

Yeast-like fungi such as Saccharomyces cerevisiae exhibit a range of cell types differing in cell shape, gene expression and growth pattern. Signal transduction pathways mediate transitions between different cell types. Nutritional signals induce rounded yeast-form cells either to enter invasive growth as elongated filamentous cells or to arrest to prepare for stationary phase, conjugation, or meiosis. An emerging theme is that development critically depends upon differential regulation of vegetative functions, including cytoskeletal organization and cell cycle progression, as much as on the expression of cell type specific gene products.     

Water in the Avian Egg Overall Budget of Incubation

The loss of mass in eggs during incubation was examined andevidence is presented to show that this is essentially due toloss of water. The mean fraction of water lost by diffusionthroughout incubation is 0.150 ± 0.025 S D per gram ofegg and 0.162 ± 0.026 S D per gram of egg content for81 species. The water fraction of fresh eggs and of hatchingeggs was examined in 32 species divided according to maturityat hatching, and found to be very similar within each category(83% in altricial 83% in semi-altricial 78% in semi-precocial72% in precocial eggs). The 11% difference between the altricialand precocial categories is statistically significant. Duringincubation, dry matter is metabolized increasing the water fractionwhich is further increased by metabolic water production. Hence,water loss during incubation is mandatory if the relative watercontent of an egg at the end of incubation is to remain essentiallythe same as at the beginning. Equations are developed whichallow one to estimate the difference between diffusive waterloss and the total water loss in altricial and piecocial eggscaused by additional water loss during pipping and hatching.     

Gas Exchange of the Avian Egg Time, Structure, and Function

Data are presented for oxygen consumption water loss duringincubation water vapor conductance of the shell and pore numberof avian eggs and the way in which these values relate not onlyto egg mass but also to incubation time. It is proposed thatall these functions are proportional to the product of egg massand rate of development where the latter is defined as the inverseof incubation time. These interrelationships account at theend of incubation for similar O₂ and CO₂ tensions in the airspace of eggs utilization of calories (0.5 kcal g^–1) andwater loss (15 g g^–1)     

Statistical properties of the variation at linked microsatellite loci: implications for the history of human Y chromosomes [published erratum appears in Mol Biol Evol 1997 Mar;14(3):354]

It has recently been suggested that observed levels of variation at microsatellite loci can be used to infer patterns of selection in genomes and to assess demographic history. In order to evaluate the feasibility of these suggestions it is necessary to know something about how levels of variation at microsatellite loci are expected to fluctuate due simply to stochasticity in the processes of mutation and inheritance (genetic sampling). Here we use recently derived properties of the stepwise mutation model to place confidence intervals around the variance in repeat score that is expected at mutation-drift equilibrium and outline a statistical test for whether an observed value differs significantly from expectation. We also develop confidence intervals for the time course of the buildup of variation following a complete elimination of variation, such as might be caused by a selective sweep or an extreme population bottleneck. We apply these methods to the variation observed at human Y-specific microsatellites. Although a number of authors have suggested the possibility of a very recent sweep, our analyses suggest that a sweep or extreme bottleneck is unlikely to have occurred anytime during the last approximately 74,000 years. To generate this result we use a recently estimated mutation rate for microsatellite loci of 5.6 x 10(-4) along with the variation observed at autosomal microsatellite loci to estimate the human effective population size. This estimate is 18,000, implying an effective number of 4,500 Y chromosomes. One important general conclusion to emerge from this study is that in order to reject mutation-drift equilibrium at a set of linked microsatellite loci it is necessary to have an unreasonably large number of loci unless the observed variance is far below that expected at mutation-drift equilibrium.