| Literature DB >> 35060531 |
Hans Pottel1, Karolien Goffin2, Liesbeth De Waele3, Elena Levtchenko3, Pierre Delanaye4,5.
Abstract
ABSTRACT: Plasma disappearance curves using multiple blood samples are a recognized reference method for measuring glomerular filtration rate (GFR). However, there is no consensus on the protocol for this type of measurement. A two-compartment model is generally considered acceptable for the mathematical description of the concentration-time decay curve. The impact of the fitting procedure on the reported GFR has not been questioned.We defined 8 different fitting procedures to calculate the area under the curve, and from this area under the curve, the GFR. We applied the 8 fitting methods (all considering a full concentration-time curve) on the multiple sample data (8 samples) of 20 children diagnosed with Duchenne muscular dystrophy. We evaluated the effect (variability) on the reported GFR from the different fitting methods and compared these results with GFR-values calculated from late samples only (samples after 120 minutes) and from one-sample methods.In 6 out of 20 cases, the fitting methods on the full concentration-time curve resulted in very different reported GFR-values, mainly because some methods were not able to fit the data, or methods resulted in GFR-values ranging from 0 to 120 mL/min. The reported GFR-result therefore strongly depends on the fitting method, making the full concentration-time method less robust than expected. Compared with a consensus reference GFR, the late sample models did not show fitting issues and may therefore be considered as more robust. Also the one-sample methods showed acceptable accuracy.The late sample methods (using 3 time-points) provide robust and reliable methods to determine GFR.Entities:
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Year: 2022 PMID: 35060531 PMCID: PMC8772627 DOI: 10.1097/MD.0000000000028608
Source DB: PubMed Journal: Medicine (Baltimore) ISSN: 0025-7974 Impact factor: 1.889
GFR-results (in mL/min/1.73 m2) of the 8 fitting procedures.
| ID | SI | mSI | NLLS | NLLS-w | S-NLLS | S-NLLS-w | mS-NLLS | mS-NLLS-w | Consensus |
| 1 | NA/109.6 | 108.8 | 112.2 | 111.0 | 110.0 | 109.9 | 110.3 | 110.9 | 110.6 |
| 2 | 160.1 | 159.3 | 160.6 | 160.1 | 159.3 | 160.3 | 159.4 | 160.3 | 160.0 |
| 3 | 115.3 | 133.1 | 122.6 | 125.0 | 86.6 | 124.4 | 86.6 | 124.4 | 121.7 |
| 4 | 156.8 | 146.2 | 158.8 | 156.4 | 158.5 | 157.1 | 158.6 | 157.6 | 157.5 |
| 5 | 126.5 | 113.6 | 121.8 | 122.9 | 126.2 | 126.8 | 126.2 | 126.5 | 125.5 |
| 6 | 159.6 | 156.7 | 160.9 | 161.5 | 160.4 | 160.1 | 160.5 | 160.1 | 160.3 |
| 7 | 148.6 | 144.1 | 147.1 | 148.7 | 148.1 | 148.2 | 148.1 | 148.2 | 148.2 |
| 8 | NA/146.9 | 151.8 | 146.6 | 146.8 | 142.1 | 146.1 | 142.1 | 146.1 | 146.4 |
| 9 | 142.3 | 138.9 | 140.6 | 142.4 | 141.4 | 141.9 | 141.4 | 141.8 | 141.6 |
| 10 | 126.1 | 124.5 | 124.3 | 124.8 | 124.6 | 125.0 | 124.6 | 125.0 | 124.8 |
| 11 | 128.4 | 122.3 | 128.9 | 128.8 | 128.5 | 128.3 | 128.5 | 128.3 | 128.4 |
| 12 | 128.1 | 128.1 |
| 113.4 | 129.3 | 127.8 | 130.0 | 129.1 | 128.3 |
| 13 | 132.8 | 137.3 | 117.7 | 122.7 | 81.5 | 127.2 | 81.5 | 127.2 | 123.7 |
| 14 | 225.5 | 222.3 | 225.8 | 227.0 | 225.4 | 225.3 | 225.4 | 225.3 | 225.4 |
| 15 | 137.2 | 136.3 | 136.6 | 137.3 | 136.9 | 137.2 | 136.9 | 137.2 | 137.0 |
| 16 | NA | NA | 85.6 | 88.7 |
| 83.3 |
| 83.3 | 85.2 |
| 17 | NA/117.1 | 116.5 | 116.6 | 117.4 | 116.8 | 116.8 | 116.8 | 116.8 | 116.8 |
| 18 | 163.5 | 160.4 | 165.3 | 165.2 | 164.0 | 163.6 | 164.3 | 164.7 | 164.1 |
| 19 | NA/126.7 | 131.6 | 127.8 | 127.2 | 126.9 | 126.2 | 126.9 | 126.2 | 127.2 |
| 20 | NA | 108.3 | 110.5 | 110.1 | 110.4 | 100.7 | 110.4 | 100.7 | 109.8 |
Statistics for GFR (in mL/min) from n simulations, based on a ±2.5% error in time-points, counts, and dosage.
| ID | %CV | Mean GFR | Stdev | Min | Max | P2.5 | Median | P97.5 | n | GFR Ind |
| 1 | 1.8% | 102.5 | 1.8 | 96.9 | 108.0 | 99.0 | 102.5 | 105.9 | 3000 | 109.4 |
| 2 | 1.9% | 110.8 | 2.1 | 97.0 | 116.5 | 106.9 | 110.9 | 114.5 | 3000 | 159.7 |
| 3 | 6.3% | 85.6 | 5.4 | 28.6 | 93.8 | 70.4 | 86.7 | 91.1 | 3000 | 119.9 |
| 4 | 1.7% | 108.8 | 1.8 | 104.2 | 113.5 | 105.5 | 108.8 | 112.0 | 3000 | 157.2 |
| 5 | 1.7% | 116.2 | 2.0 | 111.1 | 122.5 | 112.6 | 116.2 | 119.8 | 3000 | 126.4 |
| 6 | 1.8% | 100.5 | 1.8 | 75.5 | 104.9 | 97.3 | 100.5 | 103.6 | 3000 | 159.2 |
| 7 | 1.7% | 113.3 | 1.9 | 108.4 | 119.0 | 109.8 | 113.3 | 116.8 | 3000 | 148.1 |
| 8 | 6.4% | 105.6 | 6.8 | 5.4 | 114.5 | 89.1 | 106.9 | 112.1 | 3000 | 144.9 |
| 9 | 1.8% | 105.9 | 1.9 | 99.3 | 111.7 | 102.4 | 105.9 | 109.3 | 3000 | 142.3 |
| 10 | 2.3% | 109.9 | 2.6 | 64.1 | 116.4 | 105.7 | 110.0 | 114.1 | 3000 | 125.8 |
| 11 | 1.7% | 129.9 | 2.2 | 123.5 | 136.0 | 125.9 | 129.9 | 133.9 | 3000 | 128.2 |
| 12 | 24.1% | 113.6 | 27.3 | −671.9∗ | 1004.4 | 106.0 | 114.1 | 119.4 | 3000 | 126.4 |
| 13 | 6.9% | 87.2 | 6.0 | 21.5 | 94.5 | 71.7 | 88.6 | 92.5 | 3000 | 129.8 |
| 14 | 1.7% | 96.4 | 1.6 | 91.7 | 100.6 | 93.5 | 96.4 | 99.3 | 3000 | 225.9 |
| 15 | 1.7% | 118.9 | 2.1 | 113.6 | 124.4 | 115.2 | 118.9 | 122.7 | 3000 | 136.9 |
| 16 | 7.1% | 84.2 | 6.0 | 70.2 | 88.9 | 72.4 | 85.4 | 88.8 | 8 | 84.4 |
| 17 | 2.6% | 102.4 | 2.6 | 65.1 | 108.5 | 97.2 | 102.6 | 106.1 | 2998 | 116.1 |
| 18 | 1.7% | 75.6 | 1.3 | 71.8 | 79.6 | 73.2 | 75.6 | 78.0 | 3000 | 163.1 |
| 19 | 8.3% | 90.9 | 7.6 | 6.8 | 100.7 | 71.0 | 92.8 | 97.8 | 3000 | 121.6 |
| 20 | 9.4% | 75.5 | 7.1 | 6.2 | 83.0 | 55.5 | 77.1 | 81.1 | 1469 | 106.4 |
Figure 1GFR distributions for the 3000 simulations of cases ID = 2 (left) and ID = 12 (right). GFR = glomerular filtration rate.
Figure 2Relationship between slow and total AUC. AUC = area under the curve.
Figure 3GFR (indexed for BSA) obtained from S-NLLS-w against slow GFR (indexed for BSA) obtained from the slow component of the S-NLLS-w method. Diagonal is the identity line. The solid curve is the Ng-correction formula (f = 0.0012); the dashed curve is the Fleming correction (f = 0.0017) and the dotted curve is the BM-correction. BSA = body surface area, GFR = glomerular filtration rate, S-NLLS-w = split scenario for weighted non-linear least-squares.
Performance statistics of the different multiple late-samples and one-sample methods.
| Method | RMSE | Lin CCC | Bias | SD | |
| Multiple late samples methods | BM | 13.3 | 0.875 | 8.5 | 10.5 |
| Ng | 7.9 | 0.960 | 0.1 | 8.2 | |
| Fleming | 12.7 | 0.891 | 9.2 | 9.0 | |
| Jodal-BM | 14.8 | 0.844 | 9.9 | 11.3 | |
| Chantler | 12.6 | 0.925 | −6.8 | 10.9 | |
| BM_BSA | 8.4 | 0.964 | −1.7 | 8.4 |
Lin concordance correlation coefficient (upper triangle) and Pearson correlation coefficients (lower triangle) calculated from the mean GFR-values obtained from the 3000 simulations and calculated with the SI-method from the full compartment model (GFR), from the late sample methods (Bröchner-Mortensen [BM], Ng, Fleming [Flem], Bröchner-Mortensen-Jodal [BMJ], Chantler [C]), and from the one-sample methods (Piepsz and Jacobsson at 120 minutes [Jac120]).
| GFR | BM | Ng | Flem | BMJ | C | Piepsz | Jac120 | |
| GFR | 0.869 | 0.958 | 0.886 | 0.838 | 0.922 | 0.923 | 0.958 | |
| BM | 0.941 | 0.928 | 0.996 | 0.996 | 0.796 | 0.765 | 0.908 | |
| Ng | 0.958 | 0.997 | 0.935 | 0.902 | 0.947 | 0.910 | 0.968 | |
| Flem | 0.954 | 0.998 | 1.000 | 0.992 | 0.817 | 0.791 | 0.920 | |
| BMJ | 0.931 | 0.998 | 0.994 | 0.996 | 0.767 | 0.736 | 0.878 | |
| C | 0.967 | 0.989 | 0.998 | 0.996 | 0.986 | 0.970 | 0.924 | |
| Piepsz | 0.974 | 0.950 | 0.965 | 0.962 | 0.944 | 0.972 | 0.931 | |
| Jac120 | 0.962 | 0.968 | 0.973 | 0.972 | 0.957 | 0.971 | 0.980 |