| Literature DB >> 24069559 |
Anna Gambin1, Agata Charzyńska, Aleksandra Ellert-Miklaszewska, Mikołaj Rybiński.
Abstract
Despite a conceptually simple mechanism of signaling, the JAK-STAT pathway exhibits considerable behavioral complexity. Computational pathway models are tools to investigate in detail signaling process. They integrate well with experimental studies, helping to explain molecular dynamics and to state new hypotheses, most often about the structure of interactions. A relatively small amount of experimental data is available for a JAK1/2-STAT1 variant of the pathway, hence, only several computational models were developed. Here we review a dominant approach of kinetic modeling of the JAK1/2-STAT1 pathway, based on ordinary differential equations. We also give a brief overview of attempts to computationally infer topology of this pathway.Entities:
Keywords: IFN signaling; JAK1/2-STAT1 pathway; computational model; kinetics; mathematical modeling; network inference
Year: 2013 PMID: 24069559 PMCID: PMC3772111 DOI: 10.4161/jkst.24672
Source DB: PubMed Journal: JAKSTAT ISSN: 2162-3988

Figure 1. Illustration of the paradigm of an interaction between modeling and experiments. Note that conclusions obtained from a model affect an experimental setup. Similarly, measurements that provide data to bioinformatics analysis allow for model enhancements. In the desired scenario several iterations of such cycle are performed.

Figure 2. Key steps of JAK-STAT signaling in response to IFNs. IFNs induce activation of JAKs, receptors and subsequently, of cytoplasmic STATs; all by phosphorylation. Active STATs essentially form dimers, which then are translocated to nucleus where they act as transcription factors in the specific gene promoter or enhancer regions. IFN signaling negative regulators include multiple cytoplasmic PTPs, nuclear PTP and PIAS proteins, as well as specific to IFN signaling SOCS1 which in principle inhibits STAT1 phosphorylation process. See text for more details.

Figure 3. JAK1/2-STAT1 pathway modules denoted by colors on the scheme of a model by Yamada et al. (A), and numerical simulations of modules output species representing concentration of, respectively, phosphorylated receptor dimer (B), phosphorylated nuclear STAT1 dimer (C), and SOCS1 (D) with respect to time. Additional decorations of the simulations graphs represent signaling properties, such as: peak activity time τ, duration ϑ, and amplitude α at the basal, steady-state level π, corresponding to a constant IFN input of 10 nM. In such in silico experimental setup, unbound active receptor reaches peak in ca. 25 min (B) and from that moment on it is gradually used up in activation of STAT1 proteins. In turn, phosphorylated STAT1 dimers accumulate in nuclei, with maximum concentration reached in ca. 1 h (C). Their slow concentration descent is followed up by delayed expression of SOCS1 proteins (D), which gradually overtake active receptors (B). The remaining small excess of the latter induces a second, much weaker phase of signaling, starting in ca. 5th hour (B–D). After that the signal is completely attenuated. Duration of activity of signaling molecules ν elongates downstream of the pathway, and extent of this effect depends on the strength of signaling α (compare the first and the second phase of signaling; [B–D]).

Figure 4. Scheme of the JAK1/2-STAT1 pathway model from the work of Rateitschak et al. Waved (transcription and mRNA relocation) and dashed arrows represent delayed processes. Names of variables have been adjusted for a consistency of this review. See text for details.