biomodel-123465498
Name: “Jung_PNAS_2017_wildtypeM1R_figure5”
Saved: Mon, 08 Jan 2018 21:58:24 GMT
vcell identifier: biomodel-123465498
Owned by: “jsr007”
biomodel-123465505
Name: “Jung_PNAS_2017_BiasedM1R_Figure4”
Saved: Mon, 08 Jan 2018 21:58:52 GMT
vcell identifier: biomodel-123465505
Owned by: “jsr007”
biomodel-101963252
Name: “Falkenberg_PodocyteStability”
Saved: Tue, 16 Aug 2016 16:43:51 GMT
vcell identifier: biomodel-101963252
Owned by: “falkenbe”
biomodel-124562627
Name: “Yeast 3D_FRAP”
Saved: Wed, 31 Jan 2018 9:51:29 GMT
vcell identifier: biomodel-124562627
Owned by: “Wasim”
biomodel-113655498
Name: “Mohan chemotaxis 2017”
Saved: Mon, 12 Jun 2017 19:05:00 GMT
vcell identifier: biomodel-113655498
Owned by: “jnosbis”
VCell simulation service online 2/8/2018 9pm EST
02/08/2018 9pm EST: Sorry for the interruption, but now our VCell “release” site is back online. 11:00pm EST, Beta site back up also.
VCell simulation services down
02-08-2018 11:51 am EST: VCell services are running in a degraded mode while some hardware failures are being addressed. Long-running simulations may need to be restarted later today or this evening after services are completely restored.
Sorry for any inconvenience,
Jim Schaff.
VCell server maintenance: 2/8/2018 4-5pm EST
02-07-2018 11:19pm EST: Our computational facility which hosts VCell requests an hour to perform some necessary maintenance.
VCell will be unavailable from 4:00pm to 5:00pm EST on Thursday, Feb 8, 2018.
Sorry for any inconvenience,
Jim Schaff
Wittek et al., 2017
The fungal UmSrt1 and maize ZmSUT1 sucrose transporters battle for plant sugar resources
Wittek,A, Dreyer,I, Al-Rasheid,KAS, Sauer,N, Hedrich,R, Geiger,D
J Integr Plant Biol. 2017 Jun;59(6):422-435.
PUBMED:28296205 doi:10.1111/jipb.12535
VCell BioModels referenced in publication:
user: idreyer, model name: Wittek_et_al_JIntegrPlantBiol_2017_Phloem Fungus
Dreyer,I, 2017
Plant potassium channels are in general dual affinity uptake systems
Dreyer,I
AIMS Biophysics, 2017, 4(1): 90-106.
doi:10.3934/biophy.2017.1.90