Values of the amplitude of this waterborne shock wave correspond to predicted values, assuming it arose in the interior of the gas, so there is additional evidence of the effect.
34 and the present paper has but a minor influence on
the values of the amplitudes A˜m of the resonance waves.
43), requires substantially lower
values of the amplitudes of the considered m waves.
Not exact matches
This image shows QBO
amplitude near the equator at a height
of 11 miles: Observed
values from balloon wind measurements from 1950s to present; simulations from a climate model driven with observed concentrations
of greenhouse gases from 1900 to 2005 and then with projected increase through 2100.
A range
of 0.5 — 2.0 suggests that there is a risk that one
of the
amplitudes in two noisy series is twice the
value of the other.
Furthermore, it's easy to show that band - pass filtering
of two unrelated series
of random
values can produce a range
of different
values for the ratio
of their
amplitudes just by chance (Fig. 2).
RMS - EMG is calculated by summing all the squared
values of each instantaneous EMG
amplitude (in mV or μV) over a set time period, dividing this by the number
of seconds in the same time period, and then finally taking the square root
of this number (Burden, 2007).
P - EMG is simply the highest recorded EMG
amplitude value in any given time period, which can be measured either based on the raw signal or after applying one
of the other data processing options (A-EMG, I - EMG, RMS - EMG, etc.) across the various time windows that are measured within the overall muscle action being investigated.
Figures 1a, 1b and 1c which correspond to fragments analyzed for harpsichord, piano and violin respectively amostram the complexity
of the sound emitted by these instruments, which in confrontation between themselves and with the figure 2 let you see the difference between each taking into account the fundamental frequencies the
values of their respective
amplitude (intensity).
This fragmentation process enabled the implementation
of the music harmonic analysis from the Fast Fourier Transform (FFT — Fast Fourier Transform) in order to identify the harmonics associated to specific points (discrete) for each test and study in correspondence
of each them (points) with
values of frequency and
amplitude.
He manually inputs the frequencies,
amplitudes, and color
values that make up each work — determining each composition solely by entering this series
of numbers into a custom - designed program.
The former — an abstract collection
of images created by inputting a series
of numbers corresponding to frequencies,
amplitudes, and color
values into a custom - designed program — plays with the role technology plays in photographic representation; the latter, staged scenes from a imaginary emergency situation
of power loss in New York City, explores what happens to human emotions in such scenarios.
By using Rasmus» numbers the correspondence would be visibly lost because he gets a double
value for the sensitivity that would imply double
amplitudes of the reconstructed solar - induced temperature signal that would not fit the data for any
of the 4 centuries any more
John S: Any competent signal analyst, not just Parzen, is keenly aware that an exact Fourier decomposition
of ANY bounded series
of N real -
valued data points consists
of N complex -
valued coefficients specifying the
amplitude and phase
of a HARMONIC series
of sinusoids.
Any competent signal analyst, not just Parzen, is keenly aware that an exact Fourier decomposition
of ANY bounded series
of N real -
valued data points consists
of N complex -
valued coefficients specifying the
amplitude and phase
of a HARMONIC series
of sinusoids.
On a (2011) Climate Etc. post Pondering the Arctic Ocean, I interpreted the record in the context
of a (qualitative) change point analysis, defined by changes in trend, mean
value,
amplitude of the annual cycle, and interannual variability.It looks like 2013 was another change point year, characterized by low
amplitude seasonal cycle.
A set
of Monte Carlo simulations nevertheless indicated that the weak
amplitude of the global mean temperature response associated with GCR could easily be due to chance (p -
value = 0.6), and there has been no trend in the GCR.
The equations for Rossby waves (Calculation
of the Meridional Wave Number, Physics
of the Parameter, and Calculation
of the
Amplitudes) show that this can occur if a set
of necessary conditions are met: u ¯ > 0 in the midlatitude region; the highest
value of l within the waveguide is in the range
of the meridional wave numbers lm dominantly contributing to the external forcing with a given m, which provides closeness
of the k waves to respective m waves not only in terms
of the zonal but also the meridional wave numbers, favoring the QRA
of the m waves; the total latitudinal width
of the waveguide is no less than the characteristic spatial scale
of the relevant Airy function (25), which is used as the boundary condition at its southern and northern boundaries; and latitudinal distribution
of l is sufficiently smooth in the waveguide, and both TPs lie within a midlatitude region
of ∼ 25 ° N — 30 ° N and ∼ 65 ° N − 70 ° N, as the necessary condition for the application
of quasilinear Wentzel − Kramers − Brillouin (WKB) method (25) when solving the equations for Rossby waves.
1a) are calculated here with the use
of the
amplitudes A˜mOrt
of the external thermal and orographic forcing whose
values are derived from the daily data on temperature at 300 hPa from ref.
[S17] Then, on the strength
of A˜m, b2 (y0) = 2v ′ m, b2 ¯ (y0), the latitudinal averaging
of [S17] over the ΔQRA range results in the following estimate
of the maximum allowable
value, A˜m, b2 (ΔQRA), for the
amplitude of the 15 - d - mean m component
of the meridional velocity at the EBL over ΔQRA, A˜m, b2 (ΔQRA) = 2K4 -LSB-(K2 + l02 + l04) / (m / a) 2] 2K2l02u ¯ 02 〈 cos2l0 (y − y0) 〉 QRA, [S18] where 〈 X 〉 QRA stands for the latitudinal averaging
of X over ΔQRA.
The model's ensemble - mean P anomalies exhibit a realistic dipole pattern, with the largest positive
values (in excess
of 0.75 mm day − 1) over northern Europe, especially the west coast
of Great Britain and Scandinavia, and largest negative
values of comparable
amplitude over southern Europe, particularly Portugal, Spain, and other countries bordering the Mediterranean Sea (compare Fig. 3e, g).
1a then gives the
value of the QRA
amplitude A˜m
of the forced m wave with m close to k.
The
amplitude of this decrease ranges from 2 - 3 W / m2 to 6 - 7 W / m2 but any
value inside these ranges is highly climatologically significant and implies major changes in the Earth's radiation budget.
This second point was also made by James Annan in response to Hansen's 2008 Target CO2 paper, where he essentially used the same method as Snyder is using (but came to a smaller ESS
value of 6 degrees, because Snyder uses a greater temperature -
amplitude between glacial - interglacial).
Might the «weather»
of orbital cycles be impacted by K / T but not the «climate» — perhaps the trajectories
of obliquity, precession and eccentricity would become completely different given sufficient time, but maybe with the same general character — periods and
amplitudes and average
values being similar enough that a casual glance at any given time segment (on the necessary scale to characterize the orbital cycle «climate») wouldn't look like anything different.
While these data are most often interpreted in the context
of a linear trend, it is instructive to interpret the record in the context
of a (qualitative) change point analysis, defined by changes in trend, mean
value,
amplitude of the annual cycle, and interannual variability.