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Table 1 Summary of the Monte-Carlo simulation study.

From: An evaluation of R2 as an inadequate measure for nonlinear models in pharmacological and biochemical research: a Monte Carlo approach

s.d = 0.01

Model

R 2 adj

AICc

Akaike weights

BIC

resVar

red. Chi 2

 

L5

0.99999471

-156.22

0.0818

-156.35

0.00009933

0.9924

 

L4

0.99999471

-158.36

0.2389

-158.33

0.00009935

0.9930

 

L3

0.99999470

-160.20

0.5969

-160.33

0.00009959

0.9927

 

B5

0.99999258

-147.31

0.0010

-147.44

0.00013945

1.4739

 

B4

0.99975702

-57.72

0.0000

-57.69

0.00456696

42.5939

 

B3

0.99959911

-47.29

0.0000

-47.42

0.00734455

63.5805

 

W4

0.99853046

-10.89

0.0000

-10.85

0.02762048

282.3939

 

W3

0.99829856

-7.91

0.0000

-8.04

0.03336157

334.1353

 

baro5

0.99999471

-156.21

0.0814

-156.34

0.00009936

0.9927

s.d = 0.02

L5

0.99997869

-119.98

0.0774

-120.11

0.00040059

0.9946

 

L4

0.99997868

-122.13

0.2273

-122.10

0.00040068

0.9959

 

L3

0.99997871

-124.06

0.5954

-124.19

0.00040007

0.9957

 

B5

0.99997653

-117.49

0.0224

-117.62

0.00044108

1.1135

 

B4

0.99974038

-56.14

0.0000

-56.11

0.00487955

11.4098

 

B3

0.99958227

-46.30

0.0000

-46.43

0.0076527

16.6958

 

W4

0.99851513

-10.64

0.0000

-10.61

0.02790803

71.2971

 

W3

0.99828395

-7.71

0.0000

-7.84

0.03364791

84.1649

 

baro5

0.99997869

-119.98

0.0775

-120.11

0.00040044

0.9956

s.d. = 0.05

L5

0.99986676

-72.33

0.0765

-72.46

0.00250459

0.9897

 

L4

0.99986656

-74.44

0.2194

-74.41

0.00250829

0.9904

 

L3

0.99986662

-76.34

0.5674

-76.47

0.00250720

0.9882

 

B5

0.99986439

-71.87

0.0608

-72.00

0.00254924

1.0096

 

B4

0.99962966

-47.44

0.0000

-47.40

0.00696139

2.6343

 

B3

0.99946832

-40.44

0.0000

-40.57

0.00973888

3.4859

 

W4

0.99839915

-8.85

0.0000

-8.81

0.03009194

12.3020

 

W3

0.99817327

-6.21

0.0000

-6.34

0.03582530

14.3447

 

baro5

0.99986669

-72.32

0.0759

-72.45

0.00250592

0.9902

s.d. = 0.1

L5

0.99947371

-36.57

0.0742

-36.70

0.00989448

0.9984

 

L4

0.99947362

-38.73

0.2180

-38.70

0.00989607

0.9972

 

L3

0.99947374

-40.62

0.5618

-40.75

0.00989674

0.9972

 

B5

0.99947135

-36.46

0.0701

-36.59

0.00993888

1.0037

 

B4

0.99923746

-29.03

0.0017

-28.99

0.01433573

1.4052

 

B3

0.99907025

-26.35

0.0004

-26.48

0.01703305

1.6200

 

W4

0.99800791

-3.50

0.0000

-3.47

0.03745226

3.8282

 

W3

0.99779177

-1.55

0.0000

-1.68

0.04333951

4.3370

 

baro5

0.99947355

-36.56

0.0737

-36.69

0.00989740

0.9982

s.d. = 0.2

L5

0.99786138

-0.07

0.0675

-0.20

0.04025347

0.9948

 

L4

0.99785879

-2.18

0.1942

-2.15

0.04030142

0.9940

 

L3

0.99785563

-4.04

0.4930

-4.17

0.04035658

0.9928

 

B5

0.99785959

-0.05

0.0668

-0.18

0.04028754

0.9960

 

B4

0.99762513

0.49

0.0512

0.52

0.04470201

1.1027

 

B3

0.99740761

0.20

0.0592

0.06

0.04751535

1.1543

 

W4

0.99640798

11.41

0.0002

11.44

0.06760434

1.6764

 

W3

0.99625943

11.71

0.0002

11.58

0.07350697

1.8059

 

baro5

0.99786149

-0.07

0.0676

-0.20

0.04025146

0.9941

s.d. = 0.4

L5

0.99160836

35.58

0.0490

35.45

0.15887711

0.9987

 

L4

0.99157911

33.50

0.1387

33.53

0.15941969

0.9981

 

L3

0.99158878

31.58

0.3613

31.45

0.15928956

0.9980

 

B5

0.99154493

35.68

0.0466

35.55

0.15991031

1.0001

 

B4

0.99135309

34.16

0.0996

34.19

0.16370200

1.0242

 

B3

0.99098926

32.68

0.2084

32.55

0.16621846

1.0372

 

W4

0.99017401

37.58

0.0180

37.61

0.18602148

1.1663

 

W3

0.99028174

36.53

0.0305

36.40

0.19208006

1.1995

 

baro5

0.99159379

35.62

0.0480

35.49

0.15915529

0.9989

  1. Six different magnitudes of gaussian noise (low: s.d. = 0.01, 0.02; medium: s.d. = 0.05, 0.1; high: s.d. = 0.2, 0.4) were added to the fitted data of a three-parameter log-logistic model (L3). Nine different sigmoidal models were fit by nonlinear least-squares to the perturbed data and different measures for the goodness of fit (see Materials & Methods) averaged after all 2000 iterations. From the AICc values, Akaike weights were calculated in order to obtain the weight of evidence of the models.