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Enthalpy of fusion

From Wikipedia, the free encyclopedia
Enthalpy change when a substance melts
A log-log plot of the enthalpies of melting and boiling versus the melting and boiling temperatures for the pure elements. The linear relationship between the enthalpy of melting the temperature is known as Richard's rule.
Enthalpies of melting and boiling for pure elements versus temperatures of transition, demonstratingTrouton's rule

Inthermodynamics, theenthalpy of fusion of asubstance, also known as (latent)heat of fusion, is the change in itsenthalpy resulting from providingenergy, typicallyheat, to a specific quantity of the substance to change itsstate from asolid to aliquid, atconstant pressure.

The enthalpy of fusion is the amount of energy required to convert one mole of solid into liquid. For example, whenmelting 1 kg of ice (at 0 °C under awide range of pressures), 333.55 kJ of energy is absorbed with notemperature change. Theheat of solidification (when a substancechanges from liquid to solid) is equal and opposite.

This energy includes the contribution required to make room for any associated change in volume by displacing its environment against ambient pressure. The temperature at which thephase transition occurs is themelting point or the freezing point, according to context. By convention, the pressure is assumed to be 1 atm (101.325 kPa) unless otherwise specified.

Overview

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The enthalpy of fusion is alatent heat, because, while melting, the heat energy needed to change the substance from solid to liquid does not cause any increase in temperature. Temperature remains constant during the freezing or melting process, and only begins to change again (assuming the energy input or removal (cooling) continues) after the phase change is complete. The latent heat of fusion is the enthalpy change of any amount of substance when it melts. When the heat of fusion is referenced to a unit of mass, it is usually called thespecific heat of fusion, while themolar heat of fusion refers to the enthalpy change peramount of substance inmoles.

The liquid phase has a higher internal energy than the solid phase. This means energy must be supplied to a solid in order to melt it and energy is released from a liquid when it freezes, because themolecules in the liquid experience weakerintermolecular forces and so have a higher potential energy (a kind ofbond-dissociation energy for intermolecular forces).

When liquid water is cooled, its temperature falls steadily until it drops just below the line of freezing point at 0 °C. The temperature then remains constant at the freezing point while the water crystallizes. Once the water is completely frozen, its temperature resumes a colder trend.

The enthalpy of fusion is almost always a positive quantity;helium is the only known exception.[1]Helium-3 has a negative enthalpy of fusion at temperatures below 0.3 K.Helium-4 also has a very slightly negative enthalpy of fusion below 0.77 K (−272.380 °C). This means that, at appropriate constant pressures, these substances freeze with the addition of heat.[2] In the case of4He, this pressure range is between 24.992 and 25.00 atm (2,533 kPa).[3]

Standard enthalpy change of fusion of period three
Standard enthalpy change of fusion of period two of theperiodic table of elements
SubstanceHeat of fusionMelting temperature, °C
(cal/g)(J/g)
water79.72333.550.0
methane13.9658.99−182.46
propane19.1179.96−187.7
glycerol47.95200.6217.8
formic acid66.05276.358.4
acetic acid45.90192.0916 - 17
acetone23.4297.99−94.9
benzene30.45127.405.53
myristic acid47.49198.7054.4
palmitic acid39.18163.9362.9
sodium acetate/H2O63–69264–289[4]58 (trihydrate)
sodium sulfate/H2O61254[5]32.38 (decahydrate)
stearic acid47.54198.9169.3
gallium19.280.429.76
paraffin wax (C25H52)47.8–52.6200–22046 - 68

These values are mostly from theCRCHandbook of Chemistry and Physics, 62nd edition. The conversion between cal/g and J/g in the above table uses the thermochemicalcalorie (calth) = 4.184 joules rather than the International Steam Table calorie (calINT) = 4.1868 joules.

Examples

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  • To heat 1 kg of liquid water from 0 °C to 20 °C requires 83.6 kJ (see below). However, heating 0 °C ice to 20 °C requires additional energy to melt the ice. We can treat these two processes independently and using the specific heat capacity of water to be 4.18 J/(g⋅K); thus, to heat 1 kg of ice from 273.15 K to water at 293.15 K (0 °C to 20 °C) requires:
    • (1) 333.55 J/g (heat of fusion of ice) = 333.55 kJ/kg = 333.55 kJ for 1 kg of ice to melt, plus
    • (2) 4.18 J/(g⋅°C) × 20 °C = 4.18 kJ/(kg⋅°C) × 20 °C = 83.6 kJ for 1 kg of water to increase in temperature by 20 °C
    • (1 + 2) 333.55 kJ + 83.6 kJ = 417.15 kJ for 1 kg of ice to increase in temperature by 20 °C
  • Silicon has a heat of fusion of 50.21 kJ/mol. 50 kW of power can supply the energy required to melt about 100 kg of silicon in one hour:
    • 50 kW =50kJ/s =180000kJ/h
    • 180000kJ/h × (1 mol Si)/50.21kJ ×28gSi/(mol Si) ×1kgSi/1000gSi =100.4kg/h

Solubility prediction

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The heat of fusion can also be used to predictsolubility for solids in liquids. Provided anideal solution is obtained themole fraction(x2){\displaystyle (x_{2})} of solute at saturation is a function of the heat of fusion, themelting point of the solid(Tfus){\displaystyle (T_{\text{fus}})} and thetemperature(T){\displaystyle (T)} of the solution:

lnx2=ΔHfusR(1T1Tfus){\displaystyle \ln x_{2}=-{\frac {\Delta H_{\text{fus}}^{\circ }}{R}}\left({\frac {1}{T}}-{\frac {1}{T_{\text{fus}}}}\right)}

Here,R{\displaystyle R} is thegas constant. For example, the solubility ofparacetamol in water at 298K is predicted to be:

x2=exp[28100 J mol18.314 J K1 mol1(1298 K1442 K)]=0.0248{\displaystyle x_{2}=\exp {\left[-{\frac {28100~{\text{J mol}}^{-1}}{8.314~{\text{J K}}^{-1}~{\text{mol}}^{-1}}}\left({\frac {1}{298~{\text{K}}}}-{\frac {1}{442~{\text{K}}}}\right)\right]}=0.0248}

Since the molar mass of water and paracetamol are18.0153gmol−1 and151.17gmol−1 and the density of the solution is1000gL−1, an estimate of the solubility in grams per liter is:

which is a deviation from the real solubility (240 g/L) of 11%. This error can be reduced when an additionalheat capacity parameter is taken into account.[6]

Proof

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Atequilibrium thechemical potentials for the solute in the solution and pure solid are identical:

μsolid=μsolute{\displaystyle \mu _{\text{solid}}^{\circ }=\mu _{\text{solute}}^{\circ }\,}

or

μsolid=μliquid+RTlnX2{\displaystyle \mu _{\text{solid}}^{\circ }=\mu _{\text{liquid}}^{\circ }+RT\ln X_{2}\,}

withR{\displaystyle R\,} thegas constant andT{\displaystyle T\,} thetemperature.

Rearranging gives:

RTlnX2=(μliquidμsolid){\displaystyle RT\ln X_{2}=-\left(\mu _{\text{liquid}}^{\circ }-\mu _{\text{solid}}^{\circ }\right)\,}

and since

ΔGfus=μliquidμsolid{\displaystyle \Delta G_{\text{fus}}^{\circ }=\mu _{\text{liquid}}^{\circ }-\mu _{\text{solid}}^{\circ }\,}

the heat of fusion being the difference in chemical potential between the pure liquid and the pure solid, it follows that

RTlnX2=(ΔGfus){\displaystyle RT\ln X_{2}=-\left(\Delta G_{\text{fus}}^{\circ }\right)\,}

Application of theGibbs–Helmholtz equation:

((ΔGfusT)T)p=ΔHfusT2{\displaystyle \left({\frac {\partial \left({\frac {\Delta G_{\text{fus}}^{\circ }}{T}}\right)}{\partial T}}\right)_{p\,}=-{\frac {\Delta H_{\text{fus}}^{\circ }}{T^{2}}}}

ultimately gives:

((lnX2)T)=ΔHfusRT2{\displaystyle \left({\frac {\partial \left(\ln X_{2}\right)}{\partial T}}\right)={\frac {\Delta H_{\text{fus}}^{\circ }}{RT^{2}}}}

or:

lnX2=ΔHfusRT2×δT{\displaystyle \partial \ln X_{2}={\frac {\Delta H_{\text{fus}}^{\circ }}{RT^{2}}}\times \delta T}

and withintegration:

X2=1X2=x2δlnX2=lnx2=TfusTΔHfusRT2×ΔT{\displaystyle \int _{X_{2}=1}^{X_{2}=x_{2}}\delta \ln X_{2}=\ln x_{2}=\int _{T_{\text{fus}}}^{T}{\frac {\Delta H_{\text{fus}}^{\circ }}{RT^{2}}}\times \Delta T}

the result is obtained:

lnx2=ΔHfusR(1T1Tfus){\displaystyle \ln x_{2}=-{\frac {\Delta H_{\text{fus}}^{\circ }}{R}}\left({\frac {1}{T}}-{\frac {1}{T_{\text{fus}}}}\right)}

See also

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Notes

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  1. ^Atkins & Jones 2008, p. 236.
  2. ^Ott & Boerio-Goates 2000, pp. 92–93.
  3. ^Hoffer, J. K.; Gardner, W. R.; Waterfield, C. G.; Phillips, N. E. (April 1976). "Thermodynamic properties of4He. II. The bcc phase and the P-T and VT phase diagrams below 2 K".Journal of Low Temperature Physics.23 (1):63–102.Bibcode:1976JLTP...23...63H.doi:10.1007/BF00117245.S2CID 120473493.
  4. ^Page 155 in:"Thermal Energy Storage Methods".Thermal Energy Storage. 2021. pp. 125–260.doi:10.1002/9781119713173.ch3.ISBN 978-1-119-71315-9.
  5. ^Tao, Wen; Kong, Xiangfa; Bao, Anyang; Fan, Chuangang; Zhang, Yi (17 November 2020)."Preparation and Phase Change Performance of Graphene Oxide and Silica CompositeNa
    2
    SO
    4
    ·10H
    2
    O
    Phase Change Materials (PCMs) as Thermal Energy Storage Materials"
    .Materials.13 (22): 5186.doi:10.3390/ma13225186.PMC 7698442.PMID 33212870.
  6. ^Hojjati, H.; Rohani, S. (November 2006). "Measurement and Prediction of Solubility of Paracetamol in Water−Isopropanol Solution. Part 2. Prediction".Organic Process Research & Development.10 (6):1110–1118.doi:10.1021/op060074g.

References

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  • Atkins, Peter; Jones, Loretta (2008),Chemical Principles: The Quest for Insight (4th ed.), W. H. Freeman and Company, p. 236,ISBN 978-0-7167-7355-9
  • Ott, BJ. Bevan; Boerio-Goates, Juliana (2000),Chemical Thermodynamics: Advanced Applications, Academic Press,ISBN 0-12-530985-6
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