Calorimetry – Specific Heat Capacity of an Unknown Solid

Learning Objectives
  • Utilize calorimetry to determine the specific heat capacity (Cp) of an unknown solid metal.

  • Apply the Law of Conservation of Energy to heat-exchange problems.

  • Use the Law of Dulong & Petit to estimate the unknown metal’s approximate atomic weight after Cp has been found.

Introduction & Core Theory
  • Calorimeter- A thermally insulated container that minimizes heat exchange with the surroundings.

  • In this experiment, the calorimeter’s wall insulation is assumed ideal.

  • Law of Conservation of Energy

  • For an isolated system: qtotal=0q_{total}=0

  • Here: q{metal}+q{water}+q_{calorimeter}=0

  • Heat (q) dependence- q=mCpΔTq = m\,C_p\,\Delta T

  • mm = mass (g)

  • CpC_p = specific heat capacity of a substance

  • (calgC)\left(\frac{\text{cal}}{\text{g}\,^{\circ}C}\right)

  • ΔT=T<em>finalT</em>initial\Delta T = T<em>{final}-T</em>{initial}

  • Calorimeter heat capacity- Given constant: Kc=20cal/CK_c = 20\,\text{cal}/^{\circ}\text{C} (acts like an “effective mass·Cp”).

  • Dulong–Petit Law (1819)- Empirical relationship for many (but not all) crystalline solids:
    Cp×(Approx. Atomic Weight)6.0  calmolC\text{C}_p\times (\text{Approx. Atomic Weight}) \approx 6.0\; \frac{\text{cal}}{\text{mol}\,^{\circ}C}

  • Enables rough atomic-weight estimation once CpC_p is known.

Key Equations & Constants
  • Metal: q<em>metal=m</em>metalC<em>p,metal(TfT</em>i,metal)q<em>{metal}=m</em>{metal}\,C<em>{p,metal}\,(Tf-T</em>{i,metal})

  • Water: q<em>water=m</em>water(1cal/gC)(TfTi,water)q<em>{water}=m</em>{water}\,(1\,\text{cal}/\text{g}\,^{\circ}C)\,(Tf-T_{i,water})

  • Calorimeter: q<em>calorimeter=K</em>c(TfTi,water)q<em>{calorimeter}=K</em>c\,(Tf-T_{i,water})

  • Energy balance: q<em>metal+q</em>water+qcalorimeter=0q<em>{metal}+q</em>{water}+q_{calorimeter}=0

  • Solving for unknown C<em>p,metalC<em>{p,metal}: C</em>p,metal=[q<em>water+q</em>calorimeter]m<em>metal(TfT</em>i,metal)C</em>{p,metal}=\frac{-\bigl[q<em>{water}+q</em>{calorimeter}\bigr]}{m<em>{metal}\,(Tf-T</em>{i,metal})}

  • Approx. atomic weight:
    A.W.6.0  cal/molCCp,metal\text{A.W.}\approx\frac{6.0\;\text{cal}/\text{mol}\,^{\circ}C}{C_{p,metal}}

Reagents
  • Unknown metal sample (identify by letter).

  • Tap water (for boiling bath).

  • Deionized (DI) water (25 mL for calorimeter content).

Apparatus
  • Calorimeter (inner tube, outer insulating container, fitted thermometer & stirrer).

  • 250-mL beaker (boiling water bath).

  • Large test tube (holds metal while heating).

  • Hot plate.

  • Test-tube tongs.

  • 25-mL graduated cylinder.

  • Analytical balance (±0.0001 g readability).

Hazardous-Waste Disposal
  • After experiment, rinse and return the unknown metal to its labeled original container (no landfill or drain disposal).

Experimental Procedure (Step-wise)
  • Preparation of hot bath-

  • Fill 250-mL beaker ≈⅔ with tap water; place on hot plate to boil.

  • Calorimeter‐mass determinations-

  • Remove inner calorimeter tube; record its mass (±0.0001 g).

  • Add ≈25 mL DI water via 25-mL graduated cylinder.

  • Re-weigh the water-filled inner tube; difference gives mwaterm_{water}.

  • Insert inner tube back into calorimeter body.

  • Metal setup-

  • Obtain unknown metal sample; note letter code.

  • Weigh the dry metal (±0.0001 g); transfer to clean large test tube.

  • Heating the metal-

  • Immerse the test tube (with metal) into the boiling-water bath; ensure metal fully submerged but remains dry (no water enters tube).

  • Allow to equilibrate (≥85 °C).

  • Measure Ti,metalT_{i,metal}-

  • Insert calorimeter thermometer (still in rubber stopper) into hot metal within test tube; record max temperature to 0.1 °C.

  • Measure Ti,waterT_{i,water}-

  • Rapidly cool thermometer under tap water to ambient.

  • Insert thermometer into calorimeter through lid; record water temperature (initial for both water and calorimeter).

  • Mixing step-

  • Remove calorimeter lid; quickly but carefully pour hot metal from test tube into calorimeter’s inner tube (minimize splashes).

  • Replace lid immediately; stir gently with built-in stirrer (up-down motion).

  • Record maximum mixture temperature to 0.1 °C (this TfT_f applies to water, calorimeter, and metal).

  • Cleanup-

  • Return wet metal to original test tube; place on lab cart for drying/return.

Calculations & Data Analysis
  • Heat gained by water
    q<em>water=m</em>water(1cal/gC)(TfTi,water)q<em>{water}=m</em>{water}\,(1\,\text{cal}/\text{g}\,^{\circ}C)\,(Tf-T_{i,water})

  • Heat gained by calorimeter
    q<em>calorimeter=20cal/C(TfT</em>i,water)q<em>{calorimeter}=20\,\text{cal}/^{\circ}C\,(Tf-T</em>{i,water})

  • Heat lost by metal (by energy balance)
    q<em>metal=(q</em>water+qcalorimeter)q<em>{metal}=-(q</em>{water}+q_{calorimeter})

  • Specific heat of metal
    C<em>p,metal=q</em>metalm<em>metal(TfT</em>i,metal)C<em>{p,metal}=\frac{q</em>{metal}}{m<em>{metal}\,(Tf-T</em>{i,metal})}
    (Note sign convention: (q$_{metal}$) is negative, but denominator & final Cp are positive.)

  • Approximate atomic weight A.W.=6.0Cp,metal  g mol1\text{A.W.}=\frac{6.0}{C_{p,metal}}\;\text{g mol}^{-1}

  • Compare to periodic table values to speculate metal identity.

Conceptual Connections & Significance
  • Energy bookkeeping in calorimetry is an applied demonstration of the First Law of Thermodynamics.

  • Specific heat capacity is a molecular fingerprint; lower Cp often implies heavier atoms or stronger bonding restrictions on vibrational modes.

  • Dulong–Petit Law historically linked macroscopic heat capacity to atomic theory before the advent of quantum mechanics. (It fails at very low temperatures or for lighter atoms like Be or C