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But, in this case Q-1 is found to be very small (Sharma, 2005a) and then, from Eq. (8), β (< 0.5Q-1 will also be very small. Moreover, in viscoelastic solids, it is observed that for δ = 0, the value of β is found to be very near to zero (Sharma, 2008a).
Generally the raises will be very small.
The dicing should be very small.
The projected Tikhonov regularization method developed and used in this investigation to solve the Fredholm integral equations of the first kind is very simple and effective, owing to the fact that the dimension of the subspace of projection is very small ((n=2,3)); moreover, the regularized solution remains stable for a strong noise ((varepsilon =1/100)) and for regular data.
Moreover, this value is very small compared to superficial damage to the NCC panel.
Moreover, Δθ i is very small (|Δθ i | ≤ 0.43° for a small antenna with the azimuth length of 2 m at X-band) in practice.
Moreover, their fluctuations were very small.
Moreover the mapping file is very small and can be updated with ease.
Moreover, the maximum inhibitory effect achievable in such systems is very small compared to those in compensated systems.
Moreover, interpreting predictions is possible if the number of features is very small.
Moreover, the effect of pressure on the density of PET is very small (Eslami & Müller-Plathe 2009).
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