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Pimple3soy

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10.69 4.76 12.73 29.21 31.75 38.77 16.63 -12.1 2 3 4 5 6 714-3-3-Zeta Adipsin (Complement factor D) Albumin Aldehyde dehydrogenase AHD-M1 Aldehyde dehydrogenase II Aldehyde dehydrogenase, Dimeric NADP-preferring (EC 1.2.1.5) (ALDH class 3) Alpha-1-antitrypsin 1-1 precursor (Serine protease inhibitor 1-1) Alpha-1-antitrypsin 1-6 precursor (Serine protease inhibitor 1-6) (Alpha-1 protease inhibitor)
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10.69 4.76 12.73 29.21 31.75 38.77 16.63 -12.1 2 3 4 5 6 714-3-3-Zeta Adipsin (Complement factor D) Albumin Aldehyde dehydrogenase AHD-M1 Aldehyde dehydrogenase II Aldehyde dehydrogenase, Dimeric NADP-preferring (EC 1.2.1.5) (ALDH class 3) Alpha-1-antitrypsin 1-1 precursor (Serine protease inhibitor 1-1) Alpha-1-antitrypsin 1-6 precursor (Serine protease inhibitor 1-6) (Alpha-1 protease inhibitor)
1
10.69 4.76 12.73 29.21 31.75 38.77 16.63 -12.1 2 3 4 5 6 714-3-3-Zeta Adipsin (Complement factor D) Albumin Aldehyde dehydrogenase AHD-M1 Aldehyde dehydrogenase II Aldehyde dehydrogenase, Dimeric NADP-preferring (EC 1.2.1.5) (ALDH class 3) Alpha-1-antitrypsin 1-1 precursor (Serine protease inhibitor 1-1) Alpha-1-antitrypsin 1-6 precursor (Serine protease inhibitor 1-6) (Alpha-1 protease inhibitor)
1
Not yet known what causes these rapid changes. They may result from the presence of bacteria, the influx of immune cells to combat the bacteria, or the release of mediator(s) from immune cells or epithelium to deal with the insult. We speculate that the rapidity of the response (within 4 hr) is due to the release of stored mediators, such as chemokines, rather than due to the synthesis and secreti
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N of a -sheet using strands from the two monomers. As expected, CS-Rosetta calculations of the individual monomers failed to converge (Figure 5A); the native state cannot be energetically distinguished by considering only interactions within the monomer. If nevertheless the low energy, partially unfolded monomers are used as starting points in the symmetric docking protocol we obtain a converged s
1
N of a -sheet using strands from the two monomers. As expected, CS-Rosetta calculations of the individual monomers failed to converge (Figure 5A); the native state cannot be energetically distinguished by considering only interactions within the monomer. If nevertheless the low energy, partially unfolded monomers are used as starting points in the symmetric docking protocol we obtain a converged s
1
N of a -sheet using strands from the two monomers. As expected, CS-Rosetta calculations of the individual monomers failed to converge (Figure 5A); the native state cannot be energetically distinguished by considering only interactions within the monomer. If nevertheless the low energy, partially unfolded monomers are used as starting points in the symmetric docking protocol we obtain a converged s
1
N of a -sheet using strands from the two monomers. As expected, CS-Rosetta calculations of the individual monomers failed to converge (Figure 5A); the native state cannot be energetically distinguished by considering only interactions within the monomer. If nevertheless the low energy, partially unfolded monomers are used as starting points in the symmetric docking protocol we obtain a converged s