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V A F ρv = ρ Now is a good time to bring in the continuity equation Av1 = av2 so 1 v2 A a v = Plug this into the equation above, after multiplying the equation above by 2 on both sides 2 2 2 2 2 2 2 v A F v A a ρ = ρ which gives = − 2 2 2 2 1 2 A a v A F ρ Solving this for the speed at point 2 gives () 2 2 2 2 2 2 1 2 A a FA A a.
Mvft v. Tabelle 12 W˜armelehre Zustandsgleichungen Formel Einheit Druck p = F / A N/m2 = 1 Pascal = 10¡5 bar Zustandsgleichung ideales Gas p¢V = N ¢kBT VanderWaals reales Gas (pa=V2)¢(V ¡b) = NkBTa=V2 Binnendruck, b Kovolumen Innere Energie U = f=2N ¢kBT f Zahl der Freiheitsgrade (Translation, Rotation,Vibration), f = 3 f˜ur einatomiges Gas Boltzmannfaktor exp(¡E=kBT). The New York herald volume (New York NY) , June 29, 1862, Page 7, Image 7, brought to you by Library of Congress, Washington, DC,. Tb v nr I ndee 1 acaanii nf nv II lug t o al I of tut "Tlinclnnn ha romn audlrrdv npon us that we are almnt likomru lint ilreami and althnugh wo anliliie a tooling down of the prment fervor, and the npairanre of romi of Ih ol I rina, when thn prn lillng alarm h t CM.
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