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Equilibrium Shift Investigation Lab

A full Le Chatelier investigation with quantitative Kc tracking. Apply concentration spikes, sweep temperature, and change volume on five preset gas-phase equilibria. Predict the shift, then check Q against K to confirm.

Choose an Investigation

Investigation A. Concentration Stress

When a single species concentration is changed, in which direction does the system shift to re-establish equilibrium, and does K stay constant?

Independent Variable

Spike amount on one chosen species (positive = add, negative = remove)

Dependent Variable

Reaction quotient Q immediately after the stress, and shift direction toward new equilibrium

Controlled Variables
  • Temperature T (held constant for this investigation)
  • Total volume (no compression or expansion)
  • Identity of the reaction and its K at the chosen T
Hypothesis Prompt

Predict the shift direction (forward or reverse) for each stress before running it. Then check: does Q match K after the system re-equilibrates? Does K itself change?

Expected Result

Adding a reactant raises Q's denominator-side moles, pushing Q below K and shifting forward. Adding a product raises Q above K and shifts reverse. K is unchanged because temperature is constant.

Procedure
  1. Pick a reaction and let it equilibrate at T (K is computed from van't Hoff)
  2. Choose a species to spike and an amount (positive add, negative remove)
  3. Predict the shift direction using Le Châtelier's principle
  4. Record the trial, then compare predicted vs observed shift
  5. Summarize how many predictions matched, and what K stayed at

Setup

N₂(g) + 3 H₂(g) ⇌ 2 NH₃(g) · K(298 K) = 6.00e+2 · ΔH = -92 kJ/mol · Δn(gas) = -2

K
M

Investigation A spikes a single species while T is held; B sweeps T and derives ΔH from van't Hoff; C compresses or expands the volume.

Equilibrium Analysis

T
298 K
K(T)
600.000
Q after stress
116.778
Q at new eq.
600.000
Observed shift
Forward →
SpeciesInitial equilibrium [M]After stress [M]New equilibrium [M]
N₂ (1)0.1210.574
H₂ (3)0.3620.223
NH₃ (2)1.8581.951

Initial equilibrium is solved at T using K from van't Hoff. The stress is applied to the equilibrium snapshot, then the system re-equilibrates.

Prediction vs Observation

Predicted
none
Observed
forward

Pick a prediction before recording.

The shift direction is computed from sign of (Q after stress) − K. If Q below K, system goes forward; if above K, reverse. Δn-zero reactions show no shift to volume changes.

Q after stress vs Trial

-0.0500.2250.5000.7751.050-0.1000.2000.5000.8001.100TrialQ after stress

Record at least 2 trials (or load sample data) to see the regression line.

Le Châtelier hint: Based on the current stress, the system should shift forward. R = 8.314 J/(mol·K).

Data Table

(0 rows)
#TrialReactionStress appliedQ after stressK at TPredicted shiftObserved shiftMatch?
0 / 500
0 / 500
0 / 500

Reference Guide

Le Chatelier's Principle

When a stress is applied to a system at equilibrium, the system shifts to partially counteract the stress and restore Q to K.

  • Add reactant -> shift forward (toward products)
  • Add product -> shift reverse
  • Remove a species -> shift toward the side just depleted
  • Raise T (exothermic) -> shift reverse and K decreases
  • Lower V (compression) -> shift toward fewer mol of gas

Concentration and volume stresses do not change K, but temperature stresses do.

Reaction Quotient and K

For a A + b B ⇌ c C + d D the quotient is

Q=[C]c[D]d[A]a[B]bQ = \frac{[C]^c\,[D]^d}{[A]^a\,[B]^b}

Compare Q to K. If Q is below K the system shifts forward; if Q is above K the system shifts reverse; if Q equals K the system is already at equilibrium.

vant Hoff Equation

The temperature dependence of K follows

lnK=ΔHR1T+ΔSR\ln K = -\frac{\Delta H^{\circ}}{R}\,\frac{1}{T} + \frac{\Delta S^{\circ}}{R}

Plot ln K vs 1/T. The slope is -deltaH/R. With R = 8.314 J/(mol K) the derived enthalpy is deltaH = -slope x R, expressed in kJ/mol. Negative deltaH means exothermic; raising T lowers K.

Pressure and Volume

For an ideal gas at constant T, compressing the volume by a factor f multiplies every gas concentration by 1/f. Q scales by f to the power of deltaN where deltaN = (c + d) - (a + b) for gas species.

If deltaN is zero the compression does not shift the system. If deltaN is negative compression drives forward; if positive compression drives reverse.

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