Gay-Lussacov zakonFrom Wikipedia, the free encyclopedia Gay-Lussacov zakon kaže da uz konstantni tlak (p) i (n) vrijedi: V T = k o n s t . {\displaystyle {\frac {V}{T}}=konst.} V ∼ T V T = const V 1 V 2 = T 1 T 2 {\displaystyle V\sim T\qquad \qquad {\frac {V}{T}}={\text{const}}\qquad \qquad {\frac {V_{1}}{V_{2}}}={\frac {T_{1}}{T_{2}}}} V ( T ) = V 0 ( 1 + γ 0 [ T − T 0 ] ) uz γ 0 = 1 T 0 = 1 273 , 15 K {\displaystyle V(T)=V_{0}\left(1+\gamma _{0}[T-T_{0}]\right)\qquad {\text{uz}}\qquad \gamma _{0}={\frac {1}{T_{0}}}={\frac {1}{273{,}15\ \mathrm {K} }}} Gay-Lussacov zakon.
Gay-Lussacov zakon kaže da uz konstantni tlak (p) i (n) vrijedi: V T = k o n s t . {\displaystyle {\frac {V}{T}}=konst.} V ∼ T V T = const V 1 V 2 = T 1 T 2 {\displaystyle V\sim T\qquad \qquad {\frac {V}{T}}={\text{const}}\qquad \qquad {\frac {V_{1}}{V_{2}}}={\frac {T_{1}}{T_{2}}}} V ( T ) = V 0 ( 1 + γ 0 [ T − T 0 ] ) uz γ 0 = 1 T 0 = 1 273 , 15 K {\displaystyle V(T)=V_{0}\left(1+\gamma _{0}[T-T_{0}]\right)\qquad {\text{uz}}\qquad \gamma _{0}={\frac {1}{T_{0}}}={\frac {1}{273{,}15\ \mathrm {K} }}} Gay-Lussacov zakon.