The largest database of trusted experimental protocols

174 protocols using matlab r2021a

1

Ginsenoside Identification using In-House Library

Check if the same lab product or an alternative is used in the 5 most similar protocols
The in-house library was constructed by collecting ginsenosides and other steroid compounds in the existing literature and database (i.e., FoodB). In total, 468 compounds were included in our in-house library, and the complete list of these compounds is provided in the supplementary materials (Table S2). For each record, the chemical name, formula, CAS number (if available), FoodB ID (if available), HMDB ID (if available), source of information, accurate mass, and the m/z of possible adduct ions and multiply charged ions in both positive and negative modes, are provided.
The m/z in the ion feature list from the XCMS analysis was compared with the m/z in the in-house database to screen the possible ginsenosides, and if the ∆m/z is within the ±5 mDa, the ion feature is flagged and considered as a potential ginsenoside. This process was conducted using MATLAB R2021a (MathWorks Inc., Natick, MA, USA). The extracted ginsenoside ion features were exported into an Excel spreadsheet and verified manually. The remaining ion features from the XCMS analysis were used as non-ginsenoside features. The chemometric analysis was conducted using MATLAB R2021a (MathWorks Inc., Natick, MA, USA) with the PLS toolbox (Eigenvector Research, Inc., Manson, WA, USA).
+ Open protocol
+ Expand
2

EEG Data Pre-Processing and Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols
Offline, EEG data were imported to EEGLAB toolbox 2021.0 (Delorme and Makeig 2004 (link)) running under Matlab R2021a (The MathWorks, Natick, MA), with the additional ERPLAB 8.20 plug-in (Delorme and Makeig 2004 (link)). EEG signal was digitally filtered using low-pass and high-pass filters set to 30 and 0.1 Hz, respectively. To reduce artifacts from the continuous EEG data (i.e. eye movements, eye blink, muscle contractions and movement) EEGLAB plugin clean_rawdata() including artifact subspace reconstruction (ASR) was applied to the data (Gabard-Durnam et al. 2018 (link); Blum et al. 2019 (link); Chang et al. 2019 (link)). The parameters used were flat line removal, 5 s; electrode correlation, 0.8; ASR, 20; window rejection, 0.5. As a result, the mean channel rejection rate was 6.5% (SD 2.6, range 2.5–13.7), while the mean data rejection rate was 2% (SD 2.9, range 0–14). The rejected channels were interpolated using EEGLAB's spline interpolation function and the signal was then re-referenced to the average electrode. Continuous data were segmented into 600-ms epochs from 100 ms pre-stimulus to 500 ms post stimulus onset and, successively, baseline corrected from −100 ms to 0 ms before the onset of the stimulus. Datasets with less than 11 epochs per condition were excluded from the analyses.
+ Open protocol
+ Expand
3

NIRS Signal Processing for Recovery Phase Detection

Check if the same lab product or an alternative is used in the 5 most similar protocols
Data were analyzed in a custom-made MatLab program (MatLab R2021a (9.10.0.1602886), Mathworks, Nattick, MA, USA). A Hampel filter was used to detect outliers in the NIRS signal (e.g., from unwanted body movements). These outliers were replaced with the median value if exceeding three standard deviations from the value itself and three neighboring points to each side [30 (link)]. Signals were then filtered using a 5th order Butterworth low-pass filter with a 1 Hz cut-off frequency. Zero-lag filtering was used to prevent phase shifting. The end of the cyclic pattern in the signal was considered as the start-point of the recovery phase [5 (link),18 (link),19 (link)].
+ Open protocol
+ Expand
4

Scanning Electron Microscopy Imaging Protocol

Check if the same lab product or an alternative is used in the 5 most similar protocols
The handmade SE-ADM imaging system was attached to a field-emission SEM (SU5000, Hitachi High-Tech Corp, Japan) (Fig. 1A). The liquid sample holder was mounted onto the SEM stage and the detector terminal was connected to a pre-amplifier under the holder [13] (link), [14] (link). The electrical signal from the pre-amplifier was fed into the external input of SEM. The SEM images (1280 × 1020 pixels) were captured at 1000–20,000 × magnification with a scanning time of 40 s, a working distance of 7 mm, an EB acceleration voltage of 6–8 kV and a current of 1–10 pA. High-resolution SE-ADM images were processed from the LPF signal and scanning signal using the image-processing toolbox of MATLAB R2021a (Math Works Inc. Natick, MA, USA). The original SE-ADM images were filtered using a 2D Gaussian filter (GF) with a kernel size of 11 × 11 pixels and a radius of 1.2 s. Background subtraction was achieved by subtracting SE-ADM images from the filtered images using a broad GF (400 × 400 pixels, 200σ).
+ Open protocol
+ Expand
5

Quantifying Tumor-to-Background Ratios via NIR-nCLE

Check if the same lab product or an alternative is used in the 5 most similar protocols
The mean fluorescence of each CLE imaging sequence was calculated using MATLAB R2021a (MathWorks, Natick, MA, USA) with dedicated software that finds clusters in histograms allowing the segmentation in NIR-nCLE frames. The average signals in the fluorescent and background areas and standard deviation for each acquisition were calculated. The average tumor fluorescent signal from each NIR-nCLE sequence of the tumor was normalized by the average fluorescent signal from each NIR-nCLE sequence of the normal lung from the same subject by dividing the average tumor fluorescent signal by the average normal tissue fluorescent signal (background) to estimate the tumor-to-background ratio (TBR). The interquartile ranges (IQR) were also calculated.
+ Open protocol
+ Expand
6

Statistical Analysis of Empirical Scores

Check if the same lab product or an alternative is used in the 5 most similar protocols
The scores were summarized in terms of median and interquartile range (i.e., the interval between the first and third quartiles of the empirical distribution). The distribution of scores for different arms or parameters was compared using a non-parametric Kruskall-Wallis Mann–Whitney test [32 (link)], whereas for comparison of only two groups, we used Mann–Whitney U test [33 ]. The scores measured before and after the treatment were compared using paired T test [34 (link)]. A result was considered statistically significant when the p value was less than 0.05. MATLAB R2021a (MathWorks, Inc., Natick, MA, USA) software was used for the statistical analysis.
+ Open protocol
+ Expand
7

Automated Design of Prosthetic Heart Valve Leaflets

Check if the same lab product or an alternative is used in the 5 most similar protocols
The developed algorithm receives geometric parameters of the designed leaflet apparatus from the user in a simple and understandable form: height, size, degree of leaflet dome sagging, its thickness, and angle of the free edge deviation. On the basis of the point cloud generated by these parameters, building of the leaflet node links in a single closed surface is performed. Then, a 3D mesh is built and files are created, which will be used for initiating a numerical experiment (see “Simulation” block). The “Generator” is realized in the form of its own algorithm using the package of applied programs Matlab R2021a (The MathWorks, USA) for solving the tasks of technical computations.
The following set of geometric parameters is used as input data (Figure 1 (a)):
H1 (mm) — height of the proposed leaflet from its lower part up to the top point of the commissural strut;
φ (°) — angle of the free leaflet edge deviation;
R (%) — degree of leaflet dome “sagging”;
Rin (mm) — radius of the proposed prosthesis;
T (mm) — leaflet thickness;
Sec (°) — the number of degrees occupied by one leaflet.
+ Open protocol
+ Expand
8

Tapping Synchronization Dynamics Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols
The data were analyzed with MATLAB R2021a (MathWorks, USA). The force signal was low-pass filtered at 10 Hz (fourth-order Butterworth filter) to remove noises and down-sampled to 1 kHz. Asynchrony time was calculated as a difference between tap onset and metronome onset. The tap onset was defined as the first time point at which the force signal reached above mean + 5 standard deviation (SD) of the baseline (− 400 to − 200 ms before each stimulus onset). We calculated SD of asynchrony time to evaluate synchronization stability.
+ Open protocol
+ Expand
9

Evaluating Heel Pad Biomechanics in Plantar Fasciitis

Check if the same lab product or an alternative is used in the 5 most similar protocols
The shear wave speed and thickness of MIC and MAC of the symptomatic heel pad of each plantar fasciitis patient during static standing were measured with and without plastic heel cup (Innovative Healthcare Ltd., New Taipei City, Taiwan), respectively, using the measurement protocol described above performed by a single tester having more than 5 years of experience in musculoskeletal ultrasound. In the measurement with the plastic heel cup, the plastic heel cup was secured to the heel by a strap after applying an ample amount of ultrasound coupling gel to the contact surface of the plastic heel cup and heel (Figure 5). Each condition (with or without a plastic heel cup) of each heel pad was tested for three successive trials, and the mean value of these three trials was used for the statistical analysis. Paired t-test was applied to determine the difference in the shear wave speed (or thickness) of MIC (or MAC) between the conditions with and without plastic heel cup. The level of statistical significance was set at p < 0.05. Statistical analysis and data processing were performed using MATLAB R2021a (The MathWorks, Natick, MA, USA).
+ Open protocol
+ Expand
10

Biophysical Modeling of Human Cortical Cells

Check if the same lab product or an alternative is used in the 5 most similar protocols
Biophysical parameters involving Allen Brain Atlas morphologies were obtained from previous studies122 (link). The geometries were manually aligned to a three-dimensional template soma and simulated using Python LFPy119 (link) and NEURON121 . Human middle temporal gyrus layer 3, middle temporal gyrus layer 6, frontal lobe layer 3, and middle frontal gyrus layer 3 cells were simulated (n = 4 each). Action potentials were induced by raising the membrane potential, raising the sodium Nernst potential, and lowering the potassium Nernst potential. A 20 µm inclusion zone around subcellular compartments defined somatal, axonal, and dendritic voxel categories. Magnetization was quantified during the largest action potential peak within the first 20 ms, and the mean values for each cell compartment class were grouped in aggregate to define the significance between cell types. One-way ANOVA (anova1) in MATLAB R2021a (The MathWorks, Inc. Natick, MA, USA) was used to determine significance between cell type groups, with three different biophysical parameter sets yielding equivalent quantification significance outcomes.
+ Open protocol
+ Expand

About PubCompare

Our mission is to provide scientists with the largest repository of trustworthy protocols and intelligent analytical tools, thereby offering them extensive information to design robust protocols aimed at minimizing the risk of failures.

We believe that the most crucial aspect is to grant scientists access to a wide range of reliable sources and new useful tools that surpass human capabilities.

However, we trust in allowing scientists to determine how to construct their own protocols based on this information, as they are the experts in their field.

Ready to get started?

Sign up for free.
Registration takes 20 seconds.
Available from any computer
No download required

Sign up now

Revolutionizing how scientists
search and build protocols!