1. Pituitary somatotrophs secrete growth hormone spontaneously. This is controlled by burstinG oscillations in membrane potential (that is, action potentials occur in bursts separated by silent periods). This grouping together of action potentials produces an oscillatory but generally elevated calcium level, which is more efficient for secretion than isolated action potentials. Modulation up or down from this basic level is mediated by hypothalamic input of growth hormone releasing hormone (GHRH) and somatostatin (SRIF), respectively. We carried out mathematical modeling in parallel with experiments in the laboratory of S. Stojilkovic (NICHD) using channel blockers and ion substitution experiments to elucidate both the oscillation mechanism and its modulation. The key element of the model is negative feedback on large conductance (BK) calcium-activated potassium channels. We found that up-regulation could be explained by activation of an inward, non-selective cation current and/or deactivation of an inward rectifier potassium (KIR) channel. The reverse is true for down regulation. Finally, we found that the natural variability of oscillation period (a few seconds to tens of seconds) could be accounted for by different levels of BK conductance. The identity of the inward cation current is still unknown, but some of its properties have been clarified, such as that it is blocked by magnesium and carries sodium, which may help in ultimately identifying it. See Ref. # 1.? ? 2. Like the pituitary somatotrophs described above, other pituitary cells (lactotrophs, which secrete prolactin; and corticotrophs, which secrete adrenocorticotropic hormone) show bursting oscillations that are similar in appearance. For example, the spikes on the plateau are small and noisy. We were interested to contrast models for such oscillations with models for more classically studied bursting in insulin-secreting pancreatic beta-cells. The latter look somewhat different, with much larger spikes and often, but not always, longer lasting plateaus. However, such quantitative differences are subtle and not reliable for distinguishing fundamental mechanisms. Instead, we found that models for the two types of oscillations can be distinguished by the stability of the depolarized (active) state. In the classic models for square-wave bursting in beta-cells, the spiking state consists of a family of stable periodic orbits. It is thus possible to reset cells in the silent phase of the burst to the active phase with brief depolarizations. This has been confirmed by experiments on beta-cells. The pituitary-type models, on the other hand, have small spikes corresponding to transients that decay slowly toward a weakly attracting upper steady state rather than stable oscillations. As a consequence, it is very difficult to reset the state from silent to active. This was a prominent topic of discussion at a recent workshop involving both theoreticians and experimentalists organized by the PI and colleagues, so there may be attempts to verify this prediction experimentally.

Project Start
Project End
Budget Start
Budget End
Support Year
2
Fiscal Year
2008
Total Cost
$66,049
Indirect Cost
City
State
Country
United States
Zip Code
Fletcher, Patrick A; Sherman, Arthur; Stojilkovic, Stanko S (2018) Common and diverse elements of ion channels and receptors underlying electrical activity in endocrine pituitary cells. Mol Cell Endocrinol 463:23-36
Stern, Julie V; Osinga, Hinke M; LeBeau, Andrew et al. (2008) Resetting behavior in a model of bursting in secretory pituitary cells: distinguishing plateaus from pseudo-plateaus. Bull Math Biol 70:68-88
Tsaneva-Atanasova, Krasimira; Sherman, Arthur; van Goor, Frederick et al. (2007) Mechanism of spontaneous and receptor-controlled electrical activity in pituitary somatotrophs: experiments and theory. J Neurophysiol 98:131-44
Ong, Hwei Ling; Liu, Xibao; Tsaneva-Atanasova, Krasimira et al. (2007) Relocalization of STIM1 for activation of store-operated Ca(2+) entry is determined by the depletion of subplasma membrane endoplasmic reticulum Ca(2+) store. J Biol Chem 282:12176-85