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{{for|the plastic welding technique|Heat fusion}}
 
The '''enthalpy of fusion''' or '''heat of fusion''' is the change in [[enthalpy]] resulting from [[heat]]ing a given quantity of a substance to change its state from a solid to a liquid. The [[temperature]] at which this occurs is the [[melting point]].
 
The 'enthalpy' of fusion is a [[latent heat]], because during melting the introduction of heat cannot be observed as a temperature change, as the temperature remains constant during the process. 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 the '''specific heat of fusion''', while the '''molar heat of fusion''' refers to the enthalpy change per [[amount of substance]] in [[Mole (unit)|mole]]s.
 
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 the [[molecule]]s in the liquid experience weaker intermolecular forces and so have a higher potential energy (a kind of bond-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 continues to fall.
 
The enthalpy of fusion is almost always a positive quantity; helium is the only known exception.{{sfn|Atkins|Jones|2008|p=236}} [[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 0.8 K. This means that, at appropriate constant pressures, these substances freeze with the addition of heat.{{sfn|Ott|Boerio-Goates|2000|pp=92–93}}
 
==Reference values of common substances==
[[File:Enthalpy of Fusion period three.PNG|thumb|right|150px|Standard enthalpy change of fusion of period three.]][[File:Molar heat of fusion period two.png|thumb|right|150px|Standard enthalpy change of fusion of period two of the [[periodic table of elements]].]]
{| class="wikitable sortable"
|-
! Substance
! Heat of fusion<br> (cal/g)
! Heat of fusion<br> (kJ/kg)
|-
| [[water]]
| 79.8
| 334
|-
| [[methane]]
| 13.96
| 58.99
|-
| [[propane]]
| 19.11
| 79.96
|-
| [[glycerol]]
| 47.95
| 200.62
|-
| [[formic acid]]
| 66.05
| 276.35
|-
| [[acetic acid]]
| 45.91
| 192.09
|-
| [[acetone]]
| 23.42
| 97.99
|-
| [[benzene]]
| 30.45
| 127.40
|-
| [[myristic acid]]
| 47.49
| 198.70
|-
| [[palmitic acid]]
| 39.18
| 163.93
|-
| [[stearic acid]]
| 47.54
| 198.91
|-
| [[Paraffin wax]] (C<sub>25</sub>H<sub>52</sub>)
| 47.8-52.6
| 200–220
|-
|}
These values are from the [[CRC Press|CRC]] ''Handbook of Chemistry and Physics'', 62nd edition. The conversion between cal/g and kJ/kg in the above table uses the thermochemical [[calorie]] (cal<sub>th</sub>) = 4.184 joules rather than the International Steam Table calorie (cal<sub>INT</sub>) = 4.1868 joules.
 
==Applications==
1) To heat one kilogram (about 1 litre) of water from 283.15 K to 303.15 K (10 °C to 30 °C) requires 83.6 kJ. <br>
However, to melt ice and raise the resulting water temperature by 20 K requires extra energy. To heat 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·K)· 20K = 4.18 kJ/(kg·K)· 20K  = 83.6 kJ for 1kg of water to go up 20 K
:= 417.15 kJ
Or to restate it in everyday terms, one part ice at 0 °C will cool almost exactly 4 parts water at 20 °C to 0 °C.
 
2) Silicon has a heat of fusion of 50.21 kJ/mol.  50&nbsp;kW of power can supply the energy required to melt about 100&nbsp;kg of silicon in one hour, after it is brought to the melting point temperature:
 
50&nbsp;kW = {{gaps|50|kJ/s}} = {{gaps|180|000|kJ/h}}
 
{{gaps|180|000|kJ}}/h * (1&nbsp;mol Si)/{{gaps|50.21|kJ}} * {{gaps|28|g|Si}}/(mol Si)  * {{gaps|1|kg|Si}}/{{gaps|1|000|g|Si}} = {{gaps|100.4|kg/h}}
 
==Solubility prediction==
The heat of fusion can also be used to predict [[solubility]] for solids in liquids. Provided an [[ideal solution]] is obtained the [[mole fraction]] <math>(x_2)</math> of solute at saturation is a function of the heat of fusion, the [[melting point]] of the solid <math>(T_{fus})</math> and the [[temperature]] (T) of the solution:
 
:<math> \ln x_2  = - \frac {\Delta H^\circ_{fus}}{R} \left(\frac{1}{T}- \frac{1}{T_{fus}}\right)</math>
 
Here, R is the [[gas constant]]. For example the solubility of [[paracetamol]] in water at 298 [[Kelvin (unit)|K]] is predicted to be:
 
:<math> x_2  = \exp {\left(- \frac {28100 \mbox{ J mol}^{-1}} {8.314 \mbox{ J K}^{-1} \mbox{ mol}^{-1}}\left(\frac{1}{298}- \frac{1}{442}\right)\right)}= 0.0248 </math>
 
This equals to a solubility in grams per liter of:
 
<math> \frac{0.0248*\frac{1000 \mbox{ g}}{18.053 \mbox{ mol}^{-1}}}{1-0.0248}*151.17 \mbox{ mol}^{-1} = 213.4</math>
 
which is a deviation from the real solubility (240 g/L) of 11%. This error can be reduced when an additional [[heat capacity]] parameter is taken into account<ref>''Measurement and Prediction of Solubility of Paracetamol in Water-Isopropanol Solution. Part 2. Prediction'' H. Hojjati and S. Rohani Org. Process Res. Dev.; '''2006'''; 10(6) pp 1110 - 1118; (Article) {{DOI|10.1021/op060074g}}</ref>
 
===Proof===
At [[Chemical equilibrium|equilibrium]] the [[chemical potential]]s for the pure solvent and pure solid are identical:
 
:<math>\mu^\circ_{solid} = \mu^\circ_{solution}\,</math>
 
or
 
:<math>\mu^\circ_{solid} = \mu^\circ_{liquid} + RT\ln X_2\,</math>
 
with <math>R\,</math> the [[gas constant]] and <math>T\,</math> the [[temperature]].
 
Rearranging gives:
 
:<math>RT\ln X_2  = - (\mu^\circ_{liquid} -  \mu^\circ_{solid})\,</math>
 
and since
 
:<math> \Delta G^\circ_{fus}  = - (\mu^\circ_{liquid} -  \mu^\circ_{solid})\,</math>
 
the heat of fusion being the difference in chemical potential between the pure liquid and the pure solid, it follows that
 
:<math>RT\ln X_2  = - ( \Delta G^\circ_{fus})\,</math>
 
Application of the [[Gibbs-Helmholtz equation]]:
 
:<math>\left( \frac{\partial ( \frac{\Delta G^\circ_{fus} } {T} ) } {\partial T} \right)_{p\,} = - \frac {\Delta H^\circ_{fus}} {T^2} </math>
 
ultimately gives:
 
:<math>\left( \frac{\partial ( \ln X_2 ) } {\partial T} \right)  =  \frac {\Delta H^\circ_{fus}} {RT^2}</math>
 
or:
 
:<math> \partial \ln X_2  =  \frac {\Delta H^\circ_{fus}} {RT^2}*\delta T</math>
 
and with [[Integral|integration]]:
 
:<math> \int^{x_2=x_2}_{x_2 = 1} \delta \ln X_2 = \ln x_2  = \int_{T_fus}^T \frac {\Delta H^\circ_{fus}} {RT^2}*\Delta T</math>
 
the end result is obtained:
 
:<math> \ln x_2  = - \frac {\Delta H^\circ_{fus}} {R}\left(\frac{1}{T}- \frac{1}{T_{fus}}\right)</math>
 
==See also==
*[[Heat of vaporization]]
*[[Heat capacity]]
*[[Thermodynamic databases for pure substances]]
*[[Joback method]] (Estimation of the heat of fusion from molecular structure)
*[[Latent heat]]
 
==Notes==
{{Reflist}}
 
==References==
*{{Citation |last=Atkins |first=Peter |last2=Jones |first2=Loretta |year=2008 |title=Chemical Principles: The Quest for Insight |edition=4th |publisher=W. H. Freeman and Company |isbn=0-7167-7355-4 |page=236}}
*{{Citation |last=Ott |first=J. Bevan |last2=Boerio-Goates |first2=Juliana |year=2000 |title=Chemical Thermodynamics: Advanced Applications |publisher=Academic Press |isbn=0-12-530985-6}}
 
{{States of matter}}
 
{{DEFAULTSORT:Enthalpy Of Fusion}}
[[Category:Thermodynamic properties]]

Revision as of 16:42, 24 March 2013

28 year-old Painting Investments Worker Truman from Regina, usually spends time with pastimes for instance interior design, property developers in new launch ec Singapore and writing. Last month just traveled to City of the Renaissance.

The enthalpy of fusion or heat of fusion is the change in enthalpy resulting from heating a given quantity of a substance to change its state from a solid to a liquid. The temperature at which this occurs is the melting point.

The 'enthalpy' of fusion is a latent heat, because during melting the introduction of heat cannot be observed as a temperature change, as the temperature remains constant during the process. 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 the specific heat of fusion, while the molar heat of fusion refers to the enthalpy change per amount of substance in moles.

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 the molecules in the liquid experience weaker intermolecular forces and so have a higher potential energy (a kind of bond-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 continues to fall.

The enthalpy of fusion is almost always a positive quantity; helium is the only known exception.Template:Sfn 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 0.8 K. This means that, at appropriate constant pressures, these substances freeze with the addition of heat.Template:Sfn

Reference values of common substances

Standard enthalpy change of fusion of period three.
Standard enthalpy change of fusion of period two of the periodic table of elements.
Substance Heat of fusion
(cal/g)
Heat of fusion
(kJ/kg)
water 79.8 334
methane 13.96 58.99
propane 19.11 79.96
glycerol 47.95 200.62
formic acid 66.05 276.35
acetic acid 45.91 192.09
acetone 23.42 97.99
benzene 30.45 127.40
myristic acid 47.49 198.70
palmitic acid 39.18 163.93
stearic acid 47.54 198.91
Paraffin wax (C25H52) 47.8-52.6 200–220

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

Applications

1) To heat one kilogram (about 1 litre) of water from 283.15 K to 303.15 K (10 °C to 30 °C) requires 83.6 kJ.
However, to melt ice and raise the resulting water temperature by 20 K requires extra energy. To heat 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·K)· 20K = 4.18 kJ/(kg·K)· 20K = 83.6 kJ for 1kg of water to go up 20 K
= 417.15 kJ

Or to restate it in everyday terms, one part ice at 0 °C will cool almost exactly 4 parts water at 20 °C to 0 °C.

2) 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, after it is brought to the melting point temperature:

50 kW = Template:Gaps = Template:Gaps

Template:Gaps/h * (1 mol Si)/Template:Gaps * Template:Gaps/(mol Si) * Template:Gaps/Template:Gaps = Template:Gaps

Solubility prediction

The heat of fusion can also be used to predict solubility for solids in liquids. Provided an ideal solution is obtained the mole fraction (x2) of solute at saturation is a function of the heat of fusion, the melting point of the solid (Tfus) and the temperature (T) of the solution:

lnx2=ΔHfusR(1T1Tfus)

Here, R is the gas constant. For example the solubility of paracetamol in water at 298 K is predicted to be:

x2=exp(28100 J mol18.314 J K1 mol1(12981442))=0.0248

This equals to a solubility in grams per liter of:

0.02481000 g18.053 mol110.0248151.17 mol1=213.4

which is a deviation from the real solubility (240 g/L) of 11%. This error can be reduced when an additional heat capacity parameter is taken into account[1]

Proof

At equilibrium the chemical potentials for the pure solvent and pure solid are identical:

μsolid=μsolution

or

μsolid=μliquid+RTlnX2

with R the gas constant and T the temperature.

Rearranging gives:

RTlnX2=(μliquidμsolid)

and since

ΔGfus=(μliquidμsolid)

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

RTlnX2=(ΔGfus)

Application of the Gibbs-Helmholtz equation:

((ΔGfusT)T)p=ΔHfusT2

ultimately gives:

((lnX2)T)=ΔHfusRT2

or:

lnX2=ΔHfusRT2δT

and with integration:

x2=1x2=x2δlnX2=lnx2=TfusTΔHfusRT2ΔT

the end result is obtained:

lnx2=ΔHfusR(1T1Tfus)

See also

Notes

43 year old Petroleum Engineer Harry from Deep River, usually spends time with hobbies and interests like renting movies, property developers in singapore new condominium and vehicle racing. Constantly enjoys going to destinations like Camino Real de Tierra Adentro.

References

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    Naturally, you will have to pay a safety deposit and that is usually one month rent for annually of the settlement. That is the place your good religion deposit will likely be taken into account and will kind part or all of your security deposit. Anticipate to have a proportionate amount deducted out of your deposit if something is discovered to be damaged if you move out. It's best to you'll want to test the inventory drawn up by the owner, which can detail all objects in the property and their condition. If you happen to fail to notice any harm not already mentioned within the inventory before transferring in, you danger having to pay for it yourself.

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Template:States of matter

  1. Measurement and Prediction of Solubility of Paracetamol in Water-Isopropanol Solution. Part 2. Prediction H. Hojjati and S. Rohani Org. Process Res. Dev.; 2006; 10(6) pp 1110 - 1118; (Article) Electronic Instrument Positions Staff (Standard ) Cameron from Clarence Creek, usually spends time with hobbies and interests which include knotting, property developers in singapore apartment For sale and boomerangs. Has enrolled in a world contiki journey. Is extremely thrilled specifically about visiting .