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In agreement with experimental results, the engineering of resonance frequency of the sample is achieved through the number of loops of the coiling.
For this purpose, an improved impact resonance method is proposed for measuring the identical resonance frequency of the sample and for evaluating the dynamic elastic modulus, and an experimental study is performed on a total of 350 concrete samples.
The experiment lasted until the resonance frequency of the sample changed significantly (by more than 10%%).
The spinning frequency of the sample was νR = 12 kHz, the applied 1H 90° pulse length was 3.8 μs and the signal was acquired under two-pulse phase-modulated (TPPM) [29]1H decoupling at 70 kHz by averaging 10.000 scans with a recycle delay of 3 s.
Also, in the plot of B allele frequency of the sample, LOH was found in the same region which decreased all signal intensity (Figure 1C). Figure 1D shows large-scale duplication in chr8 3674807 5938053 (Size: 2.3 mb) of KOBB060879 sample, with split of heterozygosity clearly displayed in plot of B allele frequency and increase of signal intensity.
An obvious problem of this normalized metatranscriptomic method is that we cannot evaluate the gene expression frequency of the sample.
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We also show that the degree to which these oscillations are unobservable depends on the sampling frequency of the sampler.
To this end, the non-contact experimental modal analysis is conducted to identify the natural frequency of the samples.
Meanwhile, with the increase of sintering temperature, continuous modification in the resonance frequency of the samples in the range of 1.45 to 2.54 GHz has been achieved, which is much higher than previously reported [31].
where p = P q) is the prior probability of state q and is given by the frequency of the samples assigned to the root node out of all the training set samples.
This frequency of the sampling points is known by the name Nyquist-frequency.
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