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Delta G Formula Equilibrium

Gibbs Free Energy Equation:

\[ \Delta G = -RT \ln(K) \]

J/mol·K
K
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1. What is the Delta G Formula Equilibrium?

The Delta G Formula Equilibrium (ΔG = -RT ln(K)) calculates the Gibbs free energy change at equilibrium from the equilibrium constant. This fundamental thermodynamic equation relates the spontaneity of a chemical reaction to its equilibrium position.

2. How Does the Calculator Work?

The calculator uses the Gibbs free energy equation:

\[ \Delta G = -RT \ln(K) \]

Where:

Explanation: The equation shows the relationship between the thermodynamic driving force (ΔG) and the position of equilibrium (K) at a given temperature.

3. Importance of Gibbs Free Energy Calculation

Details: Calculating ΔG is essential for predicting reaction spontaneity, understanding equilibrium positions, and designing chemical processes. A negative ΔG indicates a spontaneous reaction, while a positive ΔG indicates non-spontaneous.

4. Using the Calculator

Tips: Enter the gas constant (typically 8.314 J/mol·K), temperature in Kelvin, and equilibrium constant. All values must be positive numbers.

5. Frequently Asked Questions (FAQ)

Q1: What does a negative ΔG value mean?
A: A negative ΔG indicates the reaction is spontaneous in the forward direction under the given conditions.

Q2: What does a positive ΔG value mean?
A: A positive ΔG indicates the reaction is non-spontaneous in the forward direction, but spontaneous in the reverse direction.

Q3: What is the significance of ΔG = 0?
A: When ΔG = 0, the system is at equilibrium, with no net change in the concentrations of reactants and products.

Q4: How does temperature affect ΔG?
A: Temperature directly influences ΔG through the RT term. Higher temperatures can make some reactions more spontaneous while making others less spontaneous.

Q5: Can this equation be used for biological systems?
A: Yes, the equation applies to biochemical reactions, though additional factors like pH and ionic strength may need consideration in complex biological systems.

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