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V.2. Separarea sistemelor eterogene Sistemele eterogene sunt ...

V.2. Separarea sistemelor eterogene Sistemele eterogene sunt ...

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2<br />

dv m v<br />

m⋅ = m⋅a− ⋅ρ ⋅a−ξ⋅A⋅ ⋅ρ<br />

dt ρ<br />

2<br />

D<br />

C C<br />

(V.67)<br />

Dupa punerea in miscare a particulei, singura forta<br />

variabila este forta de rezistenta, a carei valoare creste cu<br />

patratul vitezei. La o anumita valoare a vitezei particulei, forta<br />

de rezistenta egaleaza rezultanta fortelor ( F a – F p ), astfel<br />

incat:<br />

F e –F p –F r = 0 (V.68)<br />

dv<br />

Ceea ce inseamna ca: m⋅ = 0<br />

dv<br />

, deci, 0 . Prin urmare<br />

dt<br />

dt<br />

din acest moment particula se deplaseaza, in continuare, cu<br />

viteza constanta, v = v0 , denumita viteza de sedimentare<br />

libera, iar relatia (V.67), devine:<br />

=<br />

9

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