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A Hill model was used to reconstruct a concentration mortality response profile.
According to the obtained release profiles for the samples, the release profiles followed from a Hill model.
Briefly, these models were a constant model, a Hill model and as gain loss model (the product of two Hill functions with a shared top).
The differences and unstable stratification effects between the windward and leeward sides of a hill model were investigated for different upwind velocity.
If the literature model in Eq. (9) is simulated at [ET] = 0.1 nM and sampled at 12 [ST] points between 0.1 μM to 1.2 μM, these "data" (Fig. 8B circles) are fitted well by a Hill model with kmax = 4.18/sec, S50 = 0.714 μM and h = 1.14.
Analysis of the binding data according to a Hill model yields a Kapp of (9.2 ± 0.4) × 10 M–1 and a Hill coefficient n of 3 ± 1. Virtually identical results were obtained with [ I2-R3-I1], a 75 bp duplex that contains both I2 and I1 elements located at the ends of the duplex rather than the center.
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The EMS data were analyzed according to a phenomenological Hill model (eq S1 of the Supporting Information), which yields a Kapp of (1.2 ± 0.4) × 10 M–1 and a Hill coefficient n of 2 ± 1; these values are virtually identical with those obtained previously in our lab and with those obtained for binding of IHF to duplexes containing a high-affinity H′-element of attP.
Images of three of the four aligned models (the model of a hill, the model of a valley, and the model of a steep slope and a shallow slope) are shown in Fig. 2.
This companion study presents the biomechanical analysis of the "I-Wire" platform using a modified Hill model of muscle mechanics that allows for further characterization of construct function and response to perturbation.
A modified Hill model (Equation 2) [ 27] described the activity data better than the conventional uncompetitive substrate inhibition model (Equation 1); therefore, inhibition kinetics parameters were calculated using Equation 2 (Table 4).
This paper presents a wind tunnel study on the turbulent structure of the airflow around a three-dimensional hill model placed in a boundary-layer flow.
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