High-Purity Zinc Electrode Half-Cell
High-purity metallic zinc cylinder immersed in standardized 1.000 M zinc sulfate (ZnSO₄) electrolyte acting as the negative anode where oxidation occurs (Zn → Zn²⁺ + 2e⁻).
Determine the standard electromotive force (EMF), temperature coefficient (dE/dT), standard Gibbs free energy (ΔG°), standard entropy change (ΔS°), and standard enthalpy of reaction (ΔH°) for the reversible Daniell cell across the temperature range 288.15 K to 313.15 K. Explore interactive analytical gravimetry, Class A volumetric glassware and density determination.
Ready to dispense 25.0 °C of liquid.
Adjust T_cell V, then weigh the dispensed aliquot.
Mass observations are determined by the high-precision thermodynamic equation of state for pure liquid water. Readings reflect thermal equilibrium and analytical balance force restoration.
['The simple Nernst and Gibbs-Helmholtz equations assume unit activity coefficients; in 1.0 M solutions, mean ionic activity coefficients (γ_± ≈ 0.04 to 0.15) cause minor deviations from infinite-dilution formal potentials.', 'Residual liquid junction potentials across the agar-KCl bridge, while minimized (typically < 0.5 mV), introduce a minor systematic offset that does not cancel perfectly if half-cell ionic strengths differ.', 'Slow inter-diffusion of copper ions through the salt bridge over extended experimental durations (> 48 hours) can lead to trace cementation on the zinc anode.'] For the Daniell cell reaction Zn(s) + Cu²⁺(aq) ⇌ Zn²⁺(aq) + Cu(s) (n = 2), the standard potential at 298.15 K (25.0 °C) is E° = 1.1000 V (1100.0 mV). Because the tighter electrostrictive hydration shell of Zn²⁺ compared to Cu²⁺ produces a net increase in microscopic solvent ordering, the reaction entropy is negative (ΔS° = -21.47 J·mol⁻¹·K⁻¹), yielding a characteristic negative temperature coefficient dE/dT = -0.1113 mV·K⁻¹. Ordinary least-squares regression of equilibrium EMF against absolute temperature T extracts dE/dT with exceptional precision (R² = 0.99999), yielding standard Gibbs free energy ΔG°(298.15 K) = -212.27 kJ·mol⁻¹ and reaction enthalpy ΔH° = -218.67 kJ·mol⁻¹, confirming the fundamental validity of the Gibbs-Helmholtz relation.
High-purity metallic zinc cylinder immersed in standardized 1.000 M zinc sulfate (ZnSO₄) electrolyte acting as the negative anode where oxidation occurs (Zn → Zn²⁺ + 2e⁻).
Electrolytic-grade metallic copper plate immersed in standardized 1.000 M copper(II) sulfate (CuSO₄) electrolyte acting as the positive cathode where reduction occurs (Cu²⁺ + 2e⁻ → Cu).
Inverted U-tube containing 3.0 M potassium chloride in 3.0% w/v purified agar gel with porous glass frits to maintain electroneutrality while minimizing liquid junction potential (E_j < 1.0 mV).
Ultra-high input impedance voltmeter (Z_in > 10¹² Ω) that measures true thermodynamic equilibrium open-circuit cell EMF without drawing net current (i < 10⁻¹² A).
Proportional-integral-derivative (PID) regulated thermostatic water bath maintaining cell temperature stability within ±0.02 °C across the 15.0 °C to 45.0 °C test envelope.
Precision four-wire platinum resistance temperature detector (resolution ±0.01 °C) positioned adjacent to the electrode faces to measure actual solution temperature.
Determine the standard electromotive force (EMF), temperature coefficient (dE/dT), standard Gibbs free energy (ΔG°), standard entropy change (ΔS°), and standard enthalpy of reaction (ΔH°) for the reversible Daniell cell across the temperature range 288.15 K to 313.15 K. Suggested independent volumetric settings: 15.0, 20.0, 25.0, 30.0, 35.0, 40.0 °C.
Burnish the zinc rod and copper plate with fine silicon carbide abrasive paper to expose clean, active metal surfaces. Degrease with acetone, rinse thoroughly with triple-distilled water, and immerse in 0.1 M nitric acid for 10 seconds before final rinsing.
Transfer 100.0 mL of standardized 1.000 M ZnSO₄ into the left half-cell vessel and 100.0 mL of standardized 1.000 M CuSO₄ into the right vessel. Mount both vessels securely in the thermostatic water bath.
Seat the freshly conditioned 3.0 M KCl agar salt bridge so that both porous sintered glass ends are fully submerged below the electrolyte surfaces, establishing ionic contact without convective bulk mixing.
Connect the zinc anode to the negative electrometer terminal and the copper cathode to the positive terminal using gold-plated, shielded low-noise coaxial cables to eliminate contact potentials.
Set the thermostatic circulator sequentially to 15.0, 20.0, 25.0, 30.0, 35.0, and 40.0 °C. Allow 15 minutes of equilibration at each coordinate until the Pt100 RTD reading and cell EMF stabilize within ±0.01 mV.
Record the stable open-circuit cell EMF at each temperature. Plot E against absolute temperature T in Kelvin, perform linear least-squares regression to extract dE/dT, and calculate ΔG°, ΔS°, and ΔH° using fundamental thermodynamic relations.
Points are your recorded gravimetric observations. The regression line validates the linear mass-volume proportionality and extracts density.
| # | Cell Operating Temperature T (°C) | Equilibrium Reversible EMF E (mV) | Absolute Temperature T (K) | Cell Electromotive Force E (mV) | Remove |
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No readings yet. Dispense and weigh a volumetric aliquot to record it.