Intracellular phosphate pools show compartmentalization of intracellular pH in turtle urinary bladder

The urinary bladder of the fresh water turtle is capable of acidification and Na transport, in vitro, and it has been extensively used as a model of distal nephron of the kidney. In the course of measuring intracellular pH of stripped turtle bladder mucosa with phosphorus nuclear magnetic resonance, we observed the consistent presence of two inorganic phosphorus resonances under aerobic conditions, indicating the existence of a pH gradient possibly between cytosol and mitochondrion. This pH gradient was collapsed by addition of N₂ and could be restored by reintroduction of oxygen. These observations demonstrate the existence of a spontaneous pH gradient between cytosol and mitochondria of turtle bladder epithelial cells.     

Initiation of DNA synthesis in mammary epithelium and mammary tumors by lithium ions

The growth promoting effects of lithium and insulin on cultures of mammary gland epithelium and CZF mouse mammary tumor cells were investigated. Lithium chloride exerts a 450-fold increase in the rate of DNA synthesis in mammary epithelium from mid-pregnant mice in organ culture or monolayer culture. There is an increase in both the percentage of cells initiating DNA synthesis and the net accumulation of DNA. The most effective lithium concentration is 10 mM, and the maximally effective rate of stimulation is reached 48 hours after addition. The magnitude of response to lithium varies with the physiological state of the mammary epithelial cell donor: epithelium from non-pregnant or lactating mice is less responsive than that from mid-pregnant mice. In combination, insulin and lithium produce either a synergistic or an additive effect on the growth of epithelium dependent upon the physiological state of the donor animal. Lithium also promotes the growth of mammary tumor cells in the absence of serum or other mitogens. The action of lithium on DNA synthesis appears to be a direct effect on the epithelial cells.     

THE ROLE OF LIPIDS IN THE OBSERVED LACK OF PHOSPHATIDYLCHOLINE EXCHANGE IN MYELIN

Abstract— When exchange between liposomal phosphatidylcholine and that in a whole myelin fraction from guinea-pig brain was studied, very little exchange was observed. In order to investigate the reason for this phenomenon, myelin lipids in the Ca²⁺ form were prepared and subjected to sonication under the same conditions usually used to study phosphatidylcholine exchange. Despite the high cholesterol content in these extracts, this treatment produced liposomes of a size (12 nm Stoke's radius) similar to that of pure phosphatidylcholine liposomes. In this form, myelin total lipids were capable of undergoing exchange, and this was only demonstrable in the fraction containing phosphatidylcholine and that containing phosphatidylinositol. Since the level of acidic phospholipids in these total lipid extracts is potentially capable of producing 40% inhibition of phosphatidylcholine exchange (H ellings et al , 1974; B rammer & S heltawy , 1975), control experiments were carried out to ensure that the observed phosphatidylcholine exchange in the myelin lipid extract was not due to the loss of phosphoinositides. This was found to be the case, and it was concluded therefore that total myelin lipids, in the Ca²⁺ form, are capable of phosphatidylcholine exchange and that the observed lack of it in the whole myelin is due either to the effect of myelin proteins or the compact structure of the myelin membrane.
Calculations based on the difference between the rate of phosphatidylcholine exchange in the myelin liposomes and in the sonicated phosphatidylcholine liposomes indicated that the phosphatidylcholine is asymmetrically distributed in the myelin liposomes. Almost all the phosphatidylcholine seems to be present in the outer half of the bilayer.     

Correction to: Integrative transcriptomics reveals genotypic impact on sugar beet storability

Plant Molecular Biology - In the above mentioned publication, part of Fig. 6B was distorted (extra diagonal lines appeared). The original article has been corrected and the proper version...     

An Automated System for Monitoring and Regulating the pH of Bicarbonate Buffers

The bicarbonate buffer is considered as the most biorelevant buffer system for the simulation of intestinal conditions. However, its use in dissolution testing of solid oral dosage forms is very limited. The reason for this is the thermodynamic instability of the solution containing hydrogen carbonate ions and carbonic acid. The spontaneous loss of carbon dioxide (CO₂) from the solution results in an uncontrolled increase of the pH. In order to maintain the pH on the desired level, either a CO₂ loss must be completely avoided or the escaped CO₂ has to be replaced by quantitative substitution, i.e. feeding the solution with the respective amount of gas, which re-acidifies the buffer after dissociation. The present work aimed at the development of a device enabling an automatic pH monitoring and regulation of hydrogen carbonate buffers during dissolution tests.     

Validation of density–elasticity relationships for finite element modeling of human pelvic bone by modal analysis

In total hip arthroplasty and particularly in revision surgery, computer assisted pre-operative prediction of the best possible anchorage strategy for implant fixation would be a great help to the surgeon. Computer simulation relies on validated numerical models. In the current study, three density–elasticity relationships (No. 1–3) from the literature for inhomogeneous material parameter assignment from CT data in automated finite element (FE) modeling of long bones were evaluated for their suitability for FE modeling of human pelvic bone. Numerical modal analysis was conducted on 10 FE models of hemipelvic bone specimens and compared to the gold standard provided by experimental modal analysis results from a previous in-vitro study on the same specimens. Overall, calculated resonance frequencies came out lower than measured values. Magnitude of mean relative deviation of numerical resonance frequencies with regard to measured values is lowest for the density–elasticity relationship No. 3 (−15.9%) and considerably higher for both density–elasticity relationships No. 1 (−41.1%) and No. 2 (−45.0%). Mean MAC values over all specimens amount to 77.8% (No. 1), 78.5% (No. 2), and 83.0% (No. 3). MAC results show, that mode shapes are only slightly influenced by material distribution. Calculated resonance frequencies are generally lower than measured values, which indicates, that numerical models lack stiffness. Even when using the best suited (No. 3) out of three investigated density–elasticity relationships, in FE modeling of pelvic bone a considerable underestimation of model stiffness has to be taken into account.