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To test the model, we measured the leaching of atrazine through soil columns in the laboratory.
Using a bench model, we measured the effects of filtration and deflection achieved with surgical masks and N95 respirators.
Using an engineering model system in which design specifications were the same as those of the flight model, we measured charge transfer inefficiency (CTI) and the effects of charge trailing.
Within highly suitable areas (occurrence probability higher than 0.66 according to the landscape model), we measured average habitat features and compared them with the optimal mosaic depicted by the territory level models.
To verify the elastic modulus model, we measured the elastic modulus of the cement paste after 1, 3, and 7 days, in which 10%% expansive additive(Ettringite-gypsum type, Density 3.05 g/cm3) was mixed as a binder, where the water/binder ratio was 0.50.
Using rat cornea wounds as a model, we measured the dynamic timecourses of individual ion fluxes with ion-selective probes.
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For both models, we measured clade support by non-parametric bootstrap with 100 replicates.
In these models, we measured the spontaneous formation of lung metastatic nodules.
To quantify how they deviate from optimality and to motivate dynamic models, we measured their stimulus sensitivity and reward bias separately according to the Signal Detection Theory analysis described in the Introduction.
To compare the different models, we measured their precision (discrimination and calibration) with the Brier score.
To verify that these genes were also differently expressed in our cellular models, we measured their expression levels using real time polymerase chain reaction (RT-PCR).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com