By L. D. Landau, E. M. Lifshitz

**Publish 12 months note:** First released 1980 via Butterworth-Heinemann

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A lucid presentation of statistical physics and thermodynamics which develops from the final ideas to offer a lot of purposes of the idea.

**Read or Download Statistical Physics: Part 1 (3rd Edition) (Course of Theoretical Physics, Volume 5) PDF**

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**Extra resources for Statistical Physics: Part 1 (3rd Edition) (Course of Theoretical Physics, Volume 5)**

Almost like challenge 12, yet for gases with a similar strain P0 and diverse temperatures 7\ and T2 prior to the relationship of the vessels. resolution. now we have equally { Γ TT Ί (y—1V21 challenge 14. locate the minimal paintings that has to be performed on an amazing fuel as a way to compress it from strain Ρλ to P2 at a relentless temperature equivalent to that of the encircling medium (T = T0). resolution. in keeping with (20. 2) the minimal paintings is Rmin = (E2—E{)— — T0(S2—S1)+P0(V2— Ki), the place the suffixes 1 and a couple of confer with the fuel earlier than and after compression. within the current case the power E is unchanged (since the mood ature is constant), i. e. E2—Ex = zero. utilizing (43. 6), we discover the switch of entropy comparable to the switch of strain from Px to P2: S2—S1 = Nlog (P1/P2), and the swap of quantity is V2— Vx = NTQ{\IP2—\IPl). for that reason ^n=^0[log^0(-i-±)]. challenge 15. be certain the utmost paintings that are received from an amazing fuel cooled from temperature T to the temperature of the medium ΤΌ at consistent quantity. answer. From the overall formulation (20. 3), *max = Ncv(T-T0)+NcvT0 log (Γο/Γ). challenge sixteen. almost like challenge 15, yet for a gasoline cooled from temperature T to the temperature of the medium T0 and while increasing from pres convinced P to the strain of the medium P0. answer. RmMx = Ncjr-Td+NT0 log {PIPQ)+NcpT0 log {TQIT)+N