3.1.10 - Equilibrium Constant Kp for Homogeneous Systems

3.1.10 - Equilibrium Constant Kp for Homogeneous Systems

KpK_p is the gas-phase version of an equilibrium constant. Instead of using concentrations, it uses the equilibrium partial pressures of the gases in the mixture. In this lesson, you will learn how to find partial pressures, build a correct KpK_p expression, carry out short calculations, and predict how temperature, pressure, and catalysts affect equilibrium.

From Total Pressure to Partial Pressure

In a mixture of gases, each gas contributes part of the total pressure. That matters because a gaseous equilibrium is described by the pressure exerted by each gas at equilibrium, not just by the overall pressure in the container.

Partial pressure

The partial pressure of a gas is the pressure that gas exerts as part of a mixture. It is found from the gas's mole fraction multiplied by the total pressure.

If a gas A has mole fraction xAx_A, then:

Mole fraction and partial pressure

xA=moles of Atotal moles of gasp(A)=xA×ptotal x_A = \frac{\text{moles of A}}{\text{total moles of gas}} \qquad p(\mathrm{A}) = x_A \times p_{\text{total}}
  • the mole fractions of all the gases add up to 1, so the partial pressures add up to the total pressure

So the route is always the same: work out total moles, find the mole fraction of the gas you want, then multiply by the total pressure. This is why balanced, careful arithmetic matters before you even think about KpK_p.

Suppose an equilibrium mixture contains 0.60 molHX20.60\,\mathrm{mol} \ce{H_2}, 0.20 molNX20.20\,\mathrm{mol} \ce{N_2}, and 0.20 molNHX30.20\,\mathrm{mol} \ce{NH_3} at a total pressure of 250 kPa250\,\mathrm{kPa}. The total moles of gas are 1.00 mol1.00\,\mathrm{mol}, so the mole fraction of hydrogen is 0.600.60. Therefore:

p(H2)=0.60×250=150 kPap(\mathrm{H_2}) = 0.60 \times 250 = 150\,\mathrm{kPa}

You would repeat the same process for the other gases until you had the full set of equilibrium partial pressures.

Once you can turn total pressure into separate partial pressures, you have the quantities needed to build the equilibrium constant for the gaseous system.

Building the Kp Expression

KpK_p applies to a homogeneous equilibrium in the gas phase. Here, homogeneous means every species in the equilibrium mixture is in the same phase, so for this topic all the species involved are gases.

Kp

KpK_p is the equilibrium constant for a gaseous system, expressed using the equilibrium partial pressures of the gases at a fixed temperature.

The structure of a KpK_p expression follows the balanced equation exactly. Products go on the top line, reactants go on the bottom line, and each partial pressure is raised to the power of its stoichiometric coefficient.

General Kp expression

aA(g)+bB(g)⇌cC(g)+dD(g)a\mathrm{A(g)} + b\mathrm{B(g)} \rightleftharpoons c\mathrm{C(g)} + d\mathrm{D(g)} Kp=(p(C))c(p(D))d(p(A))a(p(B))bK_p=\frac{(p(\mathrm{C}))^c (p(\mathrm{D}))^d}{(p(\mathrm{A}))^a (p(\mathrm{B}))^b}

For the Haber equilibrium,

NX2(g)+3 HX2(g)⇌2 NHX3(g)\ce{N2(g) + 3H2(g) <=> 2NH3(g)}

the expression is:

Kp=(p(NH3))2p(N2)(p(H2))3K_p=\frac{(p(\mathrm{NH_3}))^2}{p(\mathrm{N_2})(p(\mathrm{H_2}))^3}

The powers matter. They come from the balanced equation, not from the numerical values you substitute. A very common mistake is to forget the square on NHX3\ce{NH_3} or the cube on HX2\ce{H_2}.

Units depend on the overall powers of pressure. If partial pressures are in kPa\mathrm{kPa}, then the Haber KpK_p above has units:

kPa2kPa4=kPa−2\frac{\mathrm{kPa^2}}{\mathrm{kPa^4}}=\mathrm{kPa^{-2}}

For some equilibria, the total power of pressure is the same on both sides, so the units cancel. That happens for:

HX2(g)+IX2(g)⇌2 HI(g)\ce{H2(g) + I2(g) <=> 2HI(g)}

because there are two moles of gas on each side overall.

Using Kp in Calculations

There are two common calculation routes. In one, the equilibrium partial pressures are given directly and you substitute them into the expression. In the other, you are given equilibrium amounts and a total pressure, so you must find the partial pressures first and then substitute.

Always check one word carefully: equilibrium. KpK_p is built from equilibrium values only. Initial amounts are not used unless you are first taken to the equilibrium amounts.

For the equilibrium

HX2(g)+IX2(g)⇌2 HI(g)\ce{H2(g) + I2(g) <=> 2HI(g)}

suppose the equilibrium partial pressures are p(HX2)=40 kPap(\ce{H_2})=40\,\mathrm{kPa}, p(IX2)=40 kPap(\ce{I_2})=40\,\mathrm{kPa}, and p(HI)=240 kPap(\ce{HI})=240\,\mathrm{kPa}.

Kp=(p(HI))2p(H2) p(I2)=240240×40=36K_p=\frac{(p(\mathrm{HI}))^2}{p(\mathrm{H_2})\,p(\mathrm{I_2})}=\frac{240^2}{40 \times 40}=36

Here the units cancel, so the final answer is simply 3636. Because KpK_p is greater than 11, the equilibrium mixture contains relatively more products than reactants, although reactants are still present because the reaction is reversible.

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