SECTION 1
Historical Context & Motivation
The concept of chemical equilibrium was not immediately obvious to early chemists, who often assumed reactions proceeded to completion. The realization that many reactions reach a dynamic balance — where forward and reverse rates equalize — emerged gradually throughout the nineteenth century. As chemists began to quantify equilibrium positions, they naturally confronted a practical question: should the equilibrium constant be expressed in terms of molar concentrations or partial pressures? This question is particularly acute for gas-phase reactions, where both representations are physically meaningful and experimentally accessible.
1864 • Law of Mass Action
1884 • Le Chatelier's Principle
1901 • van 't Hoff's Thermodynamic Treatment
1920s • Standardization of Kp and Kc Notation
The central question that this lesson addresses is both conceptual and practical: given that gas-phase equilibria can be described equally well in terms of concentrations or partial pressures, how do we convert between Kc and Kp? The answer lies in the ideal gas law, which provides a direct algebraic link between concentration (n/V) and pressure (P) for each gaseous species in the equilibrium mixture.
SECTION 2
Core Principles & Definitions
Before deriving the conversion formula, it is essential to establish clear definitions for the two forms of the equilibrium constant and the assumptions that underpin them. Both Kp and Kc describe the same equilibrium position for a gas-phase reaction, but they differ in the units used to express the activities of gaseous species. Understanding these foundational concepts ensures that the mathematical conversion is not merely a formula to memorize but a logical consequence of the ideal gas law.
Kc — Concentration-Based Constant
Kp — Pressure-Based Constant
Δn — Change in Moles of Gas
Ideal Gas Assumption
KEY TAKEAWAY
SECTION 3
Visual Explanation
The following diagram illustrates the conceptual relationship between Kp and Kc. At the center sits the ideal gas law, which provides the mathematical bridge between concentration (n/V) and partial pressure (P) for each species. The conversion factor (RT)Δn emerges naturally when the substitution P = (n/V)RT is applied to every gaseous species in the equilibrium expression.
As the diagram makes clear, the conversion between Kp and Kc is not arbitrary — it is a direct consequence of the ideal gas law. The three bottom boxes emphasize a critical insight: when Δn = 0, the conversion factor (RT)0 equals 1, so the two constants are numerically identical regardless of temperature. This occurs whenever the total moles of gaseous products equal the total moles of gaseous reactants.
SECTION 4
Mathematical Framework
We now derive the conversion formula rigorously. Consider a generic gas-phase equilibrium: aA(g) + bB(g) ⇌ cC(g) + dD(g). The equilibrium constant Kc is written in terms of molar concentrations, while Kp uses partial pressures. The ideal gas law for each species i states that Pi = [i]RT, where [i] is the molar concentration of species i. Substituting this into the Kp expression yields the conversion formula.
CONCENTRATION EQUILIBRIUM CONSTANT
Square brackets denote molar concentrations (mol·L⁻¹) at equilibrium. The exponents a, b, c, d are stoichiometric coefficients.
PRESSURE EQUILIBRIUM CONSTANT
Pi denotes the partial pressure of species i at equilibrium, typically in atmospheres (atm) or bar.
Derivation via the Ideal Gas Law
From PV = nRT, we can write Pi = (ni/V)RT = [i]RT. Substituting into Kp: Kp = ([C]RT)ᶜ([D]RT)ᵈ / (([A]RT)ᵃ([B]RT)ᵇ). Factoring out (RT) from each term, Kp = ([C]ᶜ[D]ᵈ / [A]ᵃ[B]ᵇ) × (RT)⁽ᶜ⁺ᵈ⁻ᵃ⁻ᵇ⁾. Recognizing that the concentration quotient is Kc and defining Δn = (c + d) − (a + b), we arrive at the master conversion equation.
MASTER CONVERSION EQUATION
R = 0.08206 L·atm·mol⁻¹·K⁻¹ (when pressures are in atm). T is the absolute temperature in Kelvin. Δn = (total moles of gaseous products) − (total moles of gaseous reactants). Only gaseous species are counted when computing Δn.
Choice of R Matters
REARRANGED FOR Kc
This rearrangement is useful when Kp is given and you need to find Kc.
SECTION 5
Detailed Breakdown by Δn
The value of Δn is the single parameter that determines how Kp and Kc relate to one another numerically. A careful tabulation of common reaction types alongside their Δn values illuminates this relationship and helps build intuition about when the two constants diverge significantly and when they coincide.
| Reaction Example | Δn | Relationship |
|---|---|---|
| H₂(g) + I₂(g) ⇌ 2 HI(g) | 2 − 2 = 0 | Kp = Kc |
| PCl₅(g) ⇌ PCl₃(g) + Cl₂(g) | 2 − 1 = +1 | Kp = Kc × (RT) |
| N₂(g) + 3 H₂(g) ⇌ 2 NH₃(g) | 2 − 4 = −2 | Kp = Kc × (RT)⁻² |
| 2 SO₂(g) + O₂(g) ⇌ 2 SO₃(g) | 2 − 3 = −1 | Kp = Kc × (RT)⁻¹ |
| 2 NO₂(g) ⇌ N₂O₄(g) | 1 − 2 = −1 | Kp = Kc × (RT)⁻¹ |
Common reactions and their Δn values showing the Kp–Kc relationship
The graph above provides a powerful visual tool. Because log₁₀(Kp/Kc) = Δn × log₁₀(RT), the relationship is perfectly linear. At T = 500 K, RT ≈ 41.03 L·atm·mol⁻¹, so each unit increase in Δn shifts the logarithmic ratio by about 1.613. For a reaction with Δn = +2, Kp is roughly 1684 times larger than Kc. Conversely, for Δn = −2, Kp is about 1684 times smaller. This reinforces why getting the sign of Δn correct is absolutely essential.
SECTION 6
Worked Example
Consider the synthesis of ammonia via the Haber process at 500 K. Given that Kc = 0.500 for N₂(g) + 3 H₂(g) ⇌ 2 NH₃(g), find Kp at 500 K.
Converting Kc to Kp for the Haber Process
- 1
Step 1 — Write the Balanced Equation and Identify Δn
The balanced equation is N₂(g) + 3 H₂(g) ⇌ 2 NH₃(g). Count the total moles of gaseous products and reactants: products = 2 mol (NH₃), reactants = 1 + 3 = 4 mol (N₂ + H₂). Therefore, Δn = 2 − 4 = −2.Δn = −2 - 2
Step 2 — Identify Known Values
Kc = 0.500, T = 500 K, R = 0.08206 L·atm·mol⁻¹·K⁻¹ (since we want Kp in atm units). - 3
Step 3 — Calculate RT
RT = (0.08206 L·atm·mol⁻¹·K⁻¹)(500 K) = 41.03 L·atm·mol⁻¹.RT = 41.03 - 4
Step 4 — Calculate (RT)^Δn
(RT)Δn = (41.03)−2 = 1 / (41.03)² = 1 / 1683.5 = 5.940 × 10⁻⁴.(RT)^Δn = 5.940 × 10⁻⁴ - 5
Step 5 — Apply the Conversion Formula
Kp = Kc × (RT)Δn = (0.500)(5.940 × 10⁻⁴) = 2.97 × 10⁻⁴.Kp = 2.97 × 10⁻⁴ - 6
Step 6 — Verify Reasonableness
Because Δn is negative (more moles of gas on the reactant side), we expect Kp < Kc. Indeed, 2.97 × 10⁻⁴ ≪ 0.500. The result is consistent with our earlier analysis: a negative Δn compresses the equilibrium constant when switching from concentration to pressure units.
SECTION 7
Common Pitfalls & Best Practices
The conversion between Kp and Kc is conceptually straightforward, but several common errors can undermine accurate calculations. The following table catalogues the most frequent mistakes and their remedies, so you can approach these problems with confidence.
| Common Pitfall | Why It's Wrong | Correct Approach |
|---|---|---|
| Including solids or liquids in Δn | Only gaseous species contribute to partial pressure expressions; pure solids and liquids have activity = 1 and do not appear in Kp or Kc. | Count only species with (g) designation when computing Δn. |
| Using temperature in °C instead of K | The ideal gas law requires absolute temperature. Using Celsius gives wildly incorrect RT values. | Always convert to Kelvin: T(K) = T(°C) + 273.15. |
| Using the wrong value of R | R = 8.314 J·mol⁻¹·K⁻¹ gives RT in units incompatible with atm-based Kp. | Use R = 0.08206 L·atm·mol⁻¹·K⁻¹ for atm, or R = 0.08314 L·bar·mol⁻¹·K⁻¹ for bar. |
| Getting the sign of Δn wrong | Reversing (reactants − products instead of products − reactants) inverts the exponent, yielding the reciprocal of the correct answer. | Δn = Σ(moles gaseous products) − Σ(moles gaseous reactants). Always subtract reactants from products. |
| Forgetting to recalculate Δn when the equation is scaled | Multiplying an equation by a factor k changes Δn by the same factor, altering the conversion. | Recompute Δn each time the balanced equation is modified. |
Summary of common errors in Kp–Kc conversions
KEY TAKEAWAY
SECTION 8
Connection to the Thermodynamic Equilibrium Constant
In more advanced treatments, you will encounter the thermodynamic equilibrium constant K (sometimes denoted K° or Kthermo), which is defined in terms of activities rather than concentrations or pressures. Activities are dimensionless quantities that reduce to partial pressure divided by the standard pressure (P° = 1 bar) for ideal gases, or concentration divided by the standard concentration (c° = 1 mol/L) for ideal solutions. The thermodynamic K is therefore itself dimensionless, and it is this quantity that appears in the fundamental relation ΔG° = −RT ln K.
| Feature | Kc and Kp | Thermodynamic K |
|---|---|---|
| Defined in terms of | Molar concentrations (Kc) or partial pressures (Kp) | Activities (dimensionless ratios to standard states) |
| Units | Generally have units (unless Δn = 0), though often treated as dimensionless by convention | Always dimensionless |
| Relation to ΔG° | Kp can be used in ΔG° = −RT ln Kp when pressures are referenced to 1 bar | Direct: ΔG° = −RT ln K |
| Ideal gas assumption | Required for the Kp = Kc(RT)^Δn conversion | Not required — fugacity coefficients can replace partial pressures |
| When they coincide | At low pressures and moderate temperatures (ideal gas regime) | K reduces to Kp (numerically) when P° = 1 bar and gases behave ideally |
Comparison of Kc/Kp with the thermodynamic equilibrium constant
Understanding the distinction between Kp, Kc, and the thermodynamic K is crucial as you advance into physical chemistry and chemical thermodynamics. In most general chemistry courses, the distinction is minimal because problems typically assume ideal gas behavior, but the awareness of these deeper foundations will serve you well in kinetics, electrochemistry, and advanced equilibrium calculations involving non-ideal mixtures.
SECTION 9
Practice Problems
Question 1: CONCEPTUAL
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Question 2: BASIC CALCULATION
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Question 3: INTERMEDIATE
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Question 4: APPLIED
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Question 5: CRITICAL THINKING
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SUMMARY
Lesson Summary
Summary
Gas-phase equilibria can be described using either Kc (molar concentrations) or Kp (partial pressures). The two are linked by the ideal gas law through the master equation Kp = Kc × (RT)^Δn, where Δn is the change in total moles of gas (products minus reactants), R = 0.08206 L·atm·mol⁻¹·K⁻¹ (for atm-based Kp), and T is in Kelvin.
When Δn = 0, Kp = Kc exactly. When Δn > 0, Kp > Kc; when Δn < 0, Kp < Kc. Common pitfalls include using Celsius instead of Kelvin, choosing the wrong R value, or counting solid or liquid species in Δn. Always verify that your result is reasonable: negative Δn should yield Kp < Kc, and positive Δn should yield Kp > Kc (at temperatures where RT > 1, which is essentially always in chemistry).