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For large mass changes, flight performance during escape follows the inverse relation predicted by Newtonian physics but apparently not for small mass changes.
For small mass loadings, the effects of such spatially non-uniform deposition can be described by simple convolution of the added mass and the spatial sensitivity function; the response is linear with added mass.
Remark 1 Only for small mass losses and heat sources, i.e. in the case c m = O ( M ), c q = O ( M ), a = O ( M ). the Boussinesq approximation would be applicable and we obtain the well known 'incompressibility' condition u x ( 0 ) = 0 and a u ( 0 ) = u ( 0 ) ( t ).
However, 44.4% (20/45) of SMM had SWVs of less than the 2.545 m/s cutoff, indicating a low sensitivity (55.6%) of SWV for small mass groups.
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For small masses below some threshold parameter (m < m_{ MA }), we instead check (left|m^{prime }-mright| le MA cdot m_{ MA }).
In addition, one can relatively easily identify the fragment's correct molecular formula, as well as distinguish fragment peaks from noise, due to the small "combinatorial diversity": the chance that the mass of a noise peak coincidence with the theoretical mass of a molecular formula is very small for small masses.
This statement would justify a policy of greater vigilance for small masses than for calcifications.
For small masses adjacent to normal lung parenchyma, CT was used as the modality of choice.
Especially for small masses, VTI pattern significantly improved the sensitivity (93.3% versus 55.6%), compared with SWV.
For big masses, SWV and AR are both efficient measures; nevertheless, for small masses, AR seems to be the best feature.
No radiological findings were of substantial help in differentiating MA from malignant renal tumours, especially for small masses.
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