270 likes | 280 Views
This research explores modeling the yeast cell cycle to understand controls and problems in growth, division, and checkpoint mechanisms. Investigating the molecular network dynamics sheds light on size control and cell cycle progression.
E N D
Modeling the yeast cell cycle Béla Novák Molecular Network Dynamics Research Group Budapest University of Technology and Economics and Hungarian Academy of Sciences John J. Tyson Department of Biology Virginia Polytechnic Institute and State University
S Low MPF alternation of S and M M High MPF balanced growth and division checkpoint controls problems (S, M, growth) Cell cycle engine
Wee1 P M delay M S/G2 M Cdc25 Schizosaccharomyces pombe G1 mass/nucleus Cdc13 AA Cdc20 Cdc2 Finish Wee1 Cdc20 +APC P Cdc2 Cdc2 Cdc2 Cdc13 Cdc13 Cdc25 P Cdh1 G2/M Cdc2 Cdh1 Rum1 Cdc13 SK P Rum1 Rum1 AA Start
3.0 M 0.8 Cdc2:Cdc13 0.4 S/G2 G1 0 Hopf SN2 SN3 SN1 SNIC 0 1 2 3 4 5 mass/nucleus
P Cdc2 Cdc13 Cdc2 Cdc13 0 50 100 150 200 250 300 S G2 M G1 S G2 M G1 S 5 mass/nucleus 4 3 2 1 0 Rum1 Ste9 Slp1 Wee1+Mik1 Cdc25 Time (min)
3.0 M 0.8 Cdc2:Cdc13 0.4 S/G2 G1 0 0 1 2 3 4 5 mass/nucleus
Balanced growth and division: size control WT WT wee1 wee1
Balanced growth and division: size control WT WT wee1 wee1
3.0 M 0.8 Cdc2:Cdc13 0.4 S/G2 G1 0 average 0 1 2 3 4 5 mass/nucleus
normal division length normal birth length The cycle time in oversized cells
G1 checkpoint M 0.4 Cdc2:Cdc13 S/G2 G1 0 0 2 3 5 1 4 mass/nucleus metaphase checkpoint G2 checkpoint 1.6 M M 1.2 0.4 Finish Cdc2:Cdc13 Cdc2:Cdc13 G2/M 0.8 S/G2 0.4 G1 G1 S/G2 0 0 4 4 0 2 3 5 0 2 3 5 1 1 mass/nucleus mass/nucleus Checkpoint controls
Disruption of G2/M size control reveals a G1/S size control WT WT wee1 wee1
delay Ste9 Schizosaccharomyces pombe mass/nucleus Cdc13 AA Slp1 Wee1 P Cdc2 Finish Wee1 Slp1 +APC P Cdc2 Cdc2 Cdc2 Cdc13 Cdc13 Cdc25 P Ste9 Cdc25 G2/M Cdc2 Rum1 Cdc13 SK P Rum1 Rum1 AA Start
delay Cdc25 Schizosaccharomyces pombe unreplicated DNA mass/nucleus Cdc13 AA Cdc20 Mik1 P Cdc2 Finish Mik1 Cdc20 +APC P Cdc2 Cdc2 Cdc2 Cdc13 Cdc13 Cdc25 P Cdh1 G2/M Cdc2 Cdh1 Rum1 Cdc13 SK P Rum1 Rum1 AA Start
1.2 0.8 0.4 0 0 1 2 3 4 5 wee1 M Cdc2:Cdc13 S/G2 G1 mass/nucleus
1.2 0.8 0.4 0 0 1 2 3 4 5 Mitotic catastrophe wee1 mik1- M Cdc2:Cdc13 S/G2 G1 mass/nucleus
Wee1 P delay Cdc25 Schizosaccharomyces pombe mass/nucleus Cdc13 AA Cdc20 Cdc2 Finish Wee1 Cdc20 +APC P Cdc2 Cdc2 Cdc2 Cdc13 Cdc13 Cdc25 P Cdh1 G2/M Cdc2 Cdh1 Rum1 Cdc13 SK P Rum1 Rum1 AA Start
3.0 0.8 0.4 0 0 1 2 3 4 5 The Start module is not required during mitotic cycles rum1 M Cdc2:Cdc13 S/G2 G1 mass/nucleus
delay Schizosaccharomyces pombe mass/nucleus Cdc13 AA Cdc20 Wee1 P Cdc2 Finish Wee1 Cdc20 +APC P Cdc2 Cdc2 Cdc2 Cdc13 Cdc13 Cdc25 P Cdh1 Cdc25 G2/M Cdc2 Cdh1 Rum1 Cdc13 SK P Rum1 Rum1 AA Start
1st 2nd 3rd 4th Cells become progressively smaller without size control rum1 wee1ts 2.0 0.8 M Cdc2:Cdc13 0.4 S/G2 G1 0 0 1 2 3 4 5 mass/nucleus
0.8 0.4 0 0 1 2 3 4 5 cdc25 wee1ts M Cdc2:Cdc13 S/G2 G1 mass/nucleus
3.0 0.8 0.4 0 In the absence of SK M Cdc2:Cdc13 S/G2 G1 0 1 2 3 4 5 6 mass/nucleus
X Martin-Castellanos et al. (2000): Mol. Biol. Cell11: 543-554. Cdc20 Cdh1 Cdc2 Cdc13 Rum1 SK cdc13 mass/DNA Cdc13 M G1 S/G2 M G1 S/G2 time (min)
Differential equations Analysis and computation Molecular network ??? Cell Physiology
John J. Tyson Attila Csikász-Nagy Kathy Chen Béla Győrffy Ákos Sveiczer
Hungarian Academy of Sciences Homepage: http://www.cellcycle.bme.hu/ Supporting agencies: