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Question: In Haber’s process of ammonia manufacture: \({{{N}}_{{2}}}{{(g) + 3}}{{{H}}_{{2}}}{{(g) }} \to {{2...

In Haber’s process of ammonia manufacture:
N2(g)+3H2(g)2NH3(g){{{N}}_{{2}}}{{(g) + 3}}{{{H}}_{{2}}}{{(g) }} \to {{2N}}{{{H}}_{{3}}}{{(g)}} ; ΔH0250C=92.2kJ{{\Delta }}{{{H}}^{{0}}}_{{{2}}{{{5}}^{{0}}}{{C}}}{{ = - 92}}{{.2 kJ}}

If CpC_p is independent of temperature, then reaction at 1000C{100^0}{{C}} as compared to that of 250C{{2}}{{{5}}^{{0}}}{{C}} will be.
A.More endothermic
B.Less endothermic
C.More exothermic
D.Less exothermic

Explanation

Solution

The Nitrogen from the air is combined with hydrogen from methane to form ammonia. This is a reversible reaction. It is the industrial method of preparing ammonia. High temperature and pressure should be maintained in this process. This reaction is an exothermic process that involves the release of energy. The nitrogen is obtained by liquefaction of air and hydrogen is obtained by steam reforming of natural gas. Cp{{{C}}_{{p}}} is the specific heat capacity at constant pressure.

Complete step by step answer:
Standard enthalpy of formation of ammonia at 250C{{2}}{{{5}}^{{0}}}{{C}} its given as 92.2kJ{{ - 92}}{{.2 kJ}} which shows this is an exothermic reaction
Here, Cp{{{C}}_{{p}}} each molecule is given and we can calculate the change in heat capacity.
ΔCp=2Cp(NH3)Cp(N2)3CP(H2){{\Delta }}{{{C}}_{{p}}}{{ = 2}}{{{C}}_{{{p(N}}{{{H}}_{{3}}}{{)}}}}{{ - }}{{{C}}_{{{p(}}{{{N}}_{{2}}}{{)}}}}{{ - 3}}{{{C}}_{{{P(}}{{{H}}_{{2}}}{{)}}}}
ΔCP=2(35.1)(29.1)3(28.8)JK1mol1\Rightarrow {{\Delta }}{{{C}}_{{P}}}{{ = 2(35}}{{.1) - (29}}{{.1) - 3(28}}{{.8) J}}{{{K}}^{{{ - 1}}}}{{mo}}{{{l}}^{{{ - 1}}}}
ΔCP=45.3JK1mol1\Rightarrow {{\Delta }}{{{C}}_{{P}}}{{ = - 45}}{{.3 J}}{{{K}}^{{{ - 1}}}}{{mo}}{{{l}}^{{{ - 1}}}}
We know that at constant pressure,
The change in enthalpy is the difference between the enthalpy of the product and the enthalpy of the reactant.
ΔH=HpHReq1{{\Delta H = }}{{{H}}_{{p}}}{{ - }}{{{H}}_{{R}}} \to eq1
We know that H=CpΔT{{H = }}{{{C}}_{{p}}}{{\Delta T}} at constant pressure,
So we can write ΔH=ΔCpdTeq2\Delta {{H = \Delta }}{{{C}}_{{p}}}{{dT}} \to {{eq2}}
From equation 1 and 2 we can write as ΔH2ΔH1=ΔCpdT{{\Delta }}{{{H}}_2}{{ - \Delta }}{{{H}}_1}{{ = \Delta }}{{{C}}_{{p}}}{{dT}}
Here, ΔH2{{\Delta }}{{{H}}_{{2}}} is the enthalpy at 1000C{100^0}{{C}} and ΔH1{{\Delta }}{{{H}}_{{1}}}is the enthalpy change at 250C{{2}}{{{5}}^{{0}}}{{C}}
So it can be written as ΔH2(92.2×103)=45.3(T2T1){{\Delta }}{{{H}}_{{2}}}{{ - ( - 92}}{{.2 \times 1}}{{{0}}^{{3}}}{{) = - 45}}{{.3(}}{{{T}}_{{2}}}{{ - }}{{{T}}_{{1}}}{{)}}
ΔH2(92.2×103)=45.3(10025)\Rightarrow {{\Delta }}{{{H}}_{{2}}}{{ - ( - 92}}{{.2 \times 1}}{{{0}}^{{3}}}{{) = - 45}}{{.3(100 - 25)}}
\Rightarrow ΔH2=95600J/mol{{\Delta }}{{{H}}_{{2}}}{{ = - 95600 J/mol}}
\Rightarrow ΔH2=95.6kJ/mol{{\Delta }}{{{H}}_{{2}}}{{ = - 95}}{{.6 kJ/mol}}
It is less than the enthalpy change at 250C{{2}}{{{5}}^{{0}}}{{C}} it is more negative, so we can say that it is more exothermic.
The correct answer is option C.

Note:
Kirchhoff’s law gives a relation between the temperature dependence of thermal quantities in a reaction by the difference in heat capacities of the products and reactants. At constant pressure, the heat capacity is the enthalpy divided by change in temperature. Exothermic reactions have enthalpy value always negative whereas for endothermic, the value is positive.