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In the spectral moment method, we determine the shift velocity and the broadening velocity from the measurements, and compare with the Doppler shift and broadening.
In some retinal images, blue channel is noisy; therefore, to decrease the effect of blue channel on our localizing method, we determine the lowest weight for blue channel.
Using this method, we determine an average H2O abundance of 18.7 and 18.3 wt.% for the Ivuna and Orgueil samples, respectively.
In the proposed method, we determine the patch priority using the scheme in[24] and, thus, the difference between our method and[24] is the algorithm for estimating missing intensities.
Using the least squares method, we determine that the correlation between the ΔSST and the Δ T 1km is given by: Delta T_{24text{km}}(Delta text{SST})! =! (0.2768 pm 0.0131) Delta text{SST} + (1.678 pm 0.394) (4) Fig. 11 Scatter plot of ΔSST and Δ T 1km.
Using the least square method, we determine that the correlation between the Δ T 1km and the Δ T 24km is given by begin{aligned} Delta T_{24text{km}}(Delta text{SST}) &= (0.00168 pm 0.000495) Delta text{SST} &quad + (3.82 pm 0.015) end{aligned} (5) Fig. 12 Scatter plot of ΔSST and Δ T 24km.
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In our method, we determined the precision by utilizing a large representative sample (determined statistically) of extracted entities which were drawn from a large size of documents.
In this method, we determined the free-flight time after calculating the various scattering rates.
To validate our established method, we determined the percentage of chimerism in three transplanted female dogs.
Here, using single-particle electron cryo-microscopy (cryo-EM) method, we determined the structure of mTRPML1 in lipid nanodiscs at a resolution of 5.4 Å.
Using single particle cryo-EM method, we determined the structure of mTRPML1 at a resolution of 5.4 Å (Figs. 1B, 1D, S2, and STAR METHODS).
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