$\frac{3}{4}$

$\frac{1}{4}$

$\frac{2}{3}$

$\frac{1}{8}$

Isobaric process

Isochoric process

Isothermal process

Adiabatic process

${\left( {\partial V/\partial T} \right)_P} = K\;$

${\left( {\partial V/\partial T} \right)_P} = - K\;$

${\left( {\partial V/\partial T} \right)_P} = - K/T\;$

None of these

$273\,{\rm{K}}$ and ${\rm{760}}$ mm Hg

273\,\,^\circ C\,\,and\,\,760\,\,mm\,Hg

$273\,{\rm{K}}$ and ${\rm{76}}$ mm Hg

273\,\,^\circ C\,\,and\,\,76\,\,\,mm\,\,Hg

Boyle’s law

Charles’ law

Avogadro’s law

Dalton’s law

${V_t} = K{V_0}t$

${V_t} = \frac{{K{V_0}}}{t}$

${V_t} = {V_0}\left( {1 + \frac{{273}}{t}} \right)$

${V_t} = {V_0}\left( {1 + \frac{t}{{273}}} \right)$

$1{\rm{ }}\,mL{\rm{ }}\,\,of{\rm{ }}\,\,gas$

$1{\rm{ }}\,litre{\rm{ }}\,\,of{\rm{ }}\,gas$

$22.4{\rm{ }}\,litre{\rm{ }}\,\,of{\rm{ }}\,\,gas$

$22.4{\rm{ }}\,mL{\rm{ }}\,\,of{\rm{ }}\,\,gas$

$250\,\,{\rm{K}}$

$250^\circ C$

$2500\,\,{\rm{K}}$

$25^\circ C$

The specific heat is in the order ${\rm{C}}{{\rm{l}}_2} > {\rm{B}}{{\rm{r}}_2} > {{\rm{I}}_2}$

Intermolecular forces among molecules of chlorine are the weakest and those in iodine are the strongest

The order of density is ${{\rm{I}}_2} > {\rm{B}}{{\rm{r}}_2} > C{{\rm{l}}_2}$

The order of stability is ${\rm{C}}{{\rm{l}}_2} > {\rm{B}}{{\rm{r}}_2} > {{\rm{I}}_2}$

Increases

Decreases

Remains constant

Fluctuates

$100^\circ$

$130^\circ$

$60^\circ$

$- 40^\circ$