88 research outputs found
Survival function for the grades (1: Well-differentiated; 2: Moderately differentiated; 3: Poorly differentiated or undifferentiated) using all complete data (n = 233,125).
Survival function for the grades (1: Well-differentiated; 2: Moderately differentiated; 3: Poorly differentiated or undifferentiated) using all complete data (n = 233,125).</p
Variables in the Equation using all the data (n = 233,125).
Variables in the Equation using all the data (n = 233,125).</p
Evaluating (<i>α</i> = 0.05) and the power of testing <i>H</i><sub><i>o</i></sub>: <i>β</i><sub>2</sub> = 0 vs <i>H</i><sub><i>a</i></sub>: <i>β</i><sub>2</sub> ≠0 adjusting for the auxiliary variable (Z) in the model.
(Continuous risk factor) {Censoring variable = ci = U(0,1)*1.5}.</p
Evaluating the (<i>α</i> = 0.05) and the power of testing <i>H</i><sub><i>o</i></sub>: <i>β</i><sub>2</sub> = 0 vs <i>H</i><sub><i>a</i></sub>: <i>β</i><sub>2</sub> ≠0 adjusting for (Z) in the model.
(Binary risk factor) {Censoring variable = ci = U(0,1)*1.5}.</p
Estimating 95% confidence Interval length and coverage probability (CP) of the Hazard Ratio (HR) (Binary risk factor) {Censoring variable = ci = U(0,1)*1.5}.
Estimating 95% confidence Interval length and coverage probability (CP) of the Hazard Ratio (HR) (Binary risk factor) {Censoring variable = ci = U(0,1)*1.5}.</p
Estimating 95% confidence interval length and coverage probability (CP) of the Hazard Ratio (HR) (Continuous risk factor) {Censoring variable = ci = U(0,1)*1.5}.
Estimating 95% confidence interval length and coverage probability (CP) of the Hazard Ratio (HR) (Continuous risk factor) {Censoring variable = ci = U(0,1)*1.5}.</p
sj-docx-1-smm-10.1177_09622802231168248 - Supplemental material for Misclassification simulation extrapolation method for a Weibull accelerated failure time model
Supplemental material, sj-docx-1-smm-10.1177_09622802231168248 for Misclassification simulation extrapolation method for a Weibull accelerated failure time model by Varadan Sevilimedu, Lili Yu and Hani Samawi in Statistical Methods in Medical Research</p
Estimating Hazard ratio (HR) estimation and their MSE (Continuous risk factor) {Censoring variable = ci = U(0,1)*1.5}.
Estimating Hazard ratio (HR) estimation and their MSE (Continuous risk factor) {Censoring variable = ci = U(0,1)*1.5}.</p
Estimation of Hazard ratio (HR) estimation and their MSE (Binary risk factor) {Censoring variable = ci = U(0,1)*1.5}.
Estimation of Hazard ratio (HR) estimation and their MSE (Binary risk factor) {Censoring variable = ci = U(0,1)*1.5}.</p
Computing Protein–Protein Association Affinity with Hybrid Steered Molecular Dynamics
Computing
protein–protein association affinities is one
of the fundamental challenges in computational biophysics/biochemistry.
The overwhelming amount of statistics in the phase space of very high
dimensions cannot be sufficiently sampled even with today’s
high-performance computing power. In this article, we extend a potential
of mean force (PMF)-based approach, the hybrid steered molecular dynamics
(hSMD) approach we developed for ligand–protein binding, to
protein–protein association problems. For a protein complex
consisting of two protomers, P1 and P2, we choose <i>m</i> (≥3) segments of P1 whose <i>m</i> centers of mass
are to be steered in a chosen direction and <i>n</i> (≥3)
segments of P2 whose <i>n</i> centers of mass are to be
steered in the opposite direction. The coordinates of these <i>m</i> + <i>n</i> centers constitute a phase space
of 3Â(<i>m</i> + <i>n</i>) dimensions (3Â(<i>m</i> + <i>n</i>)ÂD). All other degrees of freedom
of the proteins, ligands, solvents, and solutes are freely subject
to the stochastic dynamics of the all-atom model system. Conducting
SMD along a line in this phase space, we obtain the 3Â(<i>m</i> + <i>n</i>)ÂD PMF difference between two chosen states:
one single state in the associated state ensemble and one single state
in the dissociated state ensemble. This PMF difference is the first
of four contributors to the protein–protein association energy.
The second contributor is the 3Â(<i>m</i> + <i>n</i> – 1)ÂD partial partition in the associated state accounting
for the rotations and fluctuations of the (<i>m</i> + <i>n</i> – 1) centers while fixing one of the <i>m</i> + <i>n</i> centers of the P1–P2 complex. The two
other contributors are the 3Â(<i>m</i> – 1)ÂD partial
partition of P1 and the 3Â(<i>n</i> – 1)ÂD partial
partition of P2 accounting for the rotations and fluctuations of their <i>m</i> – 1 or <i>n</i> – 1 centers while
fixing one of the <i>m</i>/<i>n</i> centers of
P1/P2 in the dissociated state. Each of these three partial partitions
can be factored exactly into a 6D partial partition in multiplication
with a remaining factor accounting for the small fluctuations while
fixing three of the centers of P1, P2, or the P1–P2 complex,
respectively. These small fluctuations can be well-approximated as
Gaussian, and every 6D partition can be reduced in an exact manner
to three problems of 1D sampling, counting the rotations and fluctuations
around one of the centers as being fixed. We implement this hSMD approach
to the Ras–RalGDS complex, choosing three centers on RalGDS
and three on Ras (<i>m</i> = <i>n</i> = 3). At
a computing cost of about 71.6 wall-clock hours using 400 computing
cores in parallel, we obtained the association energy, −9.2
± 1.9 kcal/mol on the basis of CHARMM 36 parameters, which well
agrees with the experimental data, −8.4 ± 0.2 kcal/mol
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