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Further, by means of a novel characteristic length scale, the solutions for a number of fundamental shapes are shown to be weak functions of geometry.
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Within thin samples, absorbed power is shown to be weak function of position, while it decays exponentially within thick sample.
It was found that the quenching distance and flame speed are very weak functions of dust concentration in rich mixtures.
Where nm initial medium refractive index and B is is a weak function of particle shape and order of multipole resonances which reduces by increase in the order.
The kinetics of the first transition depend strongly on voltage, while the kinetics of the second two are only weak functions of voltage.
The optimum pressure is observed to be a weak function of design solar radiation.
However, the circumferential temperature difference is found to be a weak function of annulus diameter.
The current at any potential was observed to be a weak function of the flow rate.
The shear rate coefficient was found to be a weak function of the fluid rheology and system geometry above the flow behavior index of 0.4.
The buoyancy interaction in the reciprocating duct reduced heat transfer, which effect was enhanced by increasing the pulsating number, but appeared to be a weak function of Reynolds number.
For the NS, the Q LSPR is a weak function of wavelength and is smaller than 25 throughout the spectral range 400 1000 nm.
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