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Revision notes on thermochemistry-energetics - Solving enthalpy problems using Hess's Law

Parts 1.2a–b(i)–(iii) Thermochemistry – Hess's Law and how to do Enthalpy Calculations using the enthalpy cycle diagrams

[Author ©  Dr Phil Brown PhD: Doc Brown's exam revision notes suitable for students of advanced pre-university level theoretical-physical chemistry courses: Energetics-Thermochemistry- Thermodynamics: Using Hess's Law to solve thermochemistry problems [updated May 31st 2026 *]

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GCSE Level introduction to basic thermochemistry and calculations


Page introduction

This page describes Hess's Law of 'constant heat summation' and the use of thermochemical cycles to determine unknown enthalpy changes from known data e.g. involving the calculation of enthalpy of reaction, enthalpy of formation, enthalpy of combustion.

As well as Hess's Law calculations other methods of solving numerical enthalpy problems without using thermochemical cycles are also described.

1.2 Thermochemistry – Hess's Law and Enthalpy Calculations


Hess's Law diagram for several pathways from reactants A to products B1.2a Hess's Law and its importance

Hess's Law is a version of the general law of conservation of energy.

i.e. the first law of thermodynamics which can be stated as energy cannot be destroyed or created but merely changed in form or distributed in different ways.

Hess's Law states that the energy change from reactants A to products B is independent of the pathway taken no matter how varied or how many stages it involves as long as the initial and final conditions are the same i.e. same temperature.

This is shown in the diagram of enthalpy cycles on the right.

ΔH1 = ΔH(A to B) Pathway 1 the most direct route with no intermediate stages,

 or  ΔH1 = ΔH2 + ΔH3 pathway 2 involving one set of intermediates C, or

or  ΔH1 = ΔH4 + ΔH5 + ΔH6 pathway 3 involving two sets of intermediates D and E

etc. etc. – there is no limit to the complexity of the Hess's Law Cycle as long as A and B are constant.


Many problems can be set out as a 'Hess's Law' triangle e.g.

Application of Hess's Law (i)

ΔHθ1

  B

ΔHθ2

(c) doc b    

ΔHθ3

C
Clearly there are two pathways from A to B

direct and via C following the arrows direction

so,  ΔHθ1  =  ΔHθ2  +  ΔHθ3

or    ΔHθ2  =  ΔHθ1  -  ΔHθ3

or    ΔHθ3  =  ΔHθ1  -  ΔHθ2

Application of Hess's Law (ii)

ΔHθ1

  B

ΔHθ2

(c) doc b     (c) doc b

ΔHθ3

C
In this case there are two pathways from A to C

direct and via B following the arrows direction

so,  ΔHθ2  =  ΔHθ1  +  ΔHθ3

or   ΔHθ1  =  ΔHθ2  -  ΔHθ3

or    ΔHθ3  =  ΔHθ2  -  ΔHθ1

Always take care with the ΔH signs which ever way you set up the triangle to apply Hess's Law Although slightly more awkward, (ii) might be better suited to the way the experiment results are obtained or given data.

Note: Superscript θ means a standard enthalpy value (see further down the page)

and each ΔHθ could be a composite of several ΔHθ values - see enthalpy of combustion calculations below.


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1.2b Using Hess's Law to perform enthalpy calculations

1.2b(i) Using known enthalpies of reaction or combustion

Using a Hess's Law Cycle you can calculate enthalpies of formation which you could not determine by laboratory experiment. However, using these calculated enthalpies of formation and experimentally determined enthalpies of combustion a huge variety of other enthalpies for other reactions can then be calculated.

The 1st example of calculating the enthalpy of formation of methane illustrates the principles of using Hess's Law, especially as this cannot be determined by direct laboratory experiment!

Given the following data below from text/data book calculate the enthalpy of formation of methane.

C(s) + O2(g) ==> CO2(g)   ΔHθc(C(s)) = ΔHθf(CO2(g)) = –393 kJmol–1

H2(g) + 1/2O2(g) ==> H2O(l)  ΔHθc(H2(g)) = ΔHθf(H2O(l)) = –286 kJmol–1

CH4(g) + 2O2(g) ==> CO2(g) + 2H2O(l)  ΔHθc(CH4(g)) = –890 kJmol–1

All of the three enthalpies above can be very accurately determined by direct experiment in a calorimeter.

BUT ΔHθf for C(s)  +  2H2(g)  ===>  CH4(g) cannot be determined directly.

 
ΔHΨf (methane) = ??? kJmol–1
C(s) + 2H2(g) (c) doc b CH4(g)

ΔHθc(C(s)) + 2 x ΔHθc(H2(g))

= (–393) + (2 x –286)

C => CO2 and 2H2 => 2H2O

(c) doc b

+2O2(g)       

     (c) doc b

+2O2(g)

ΔHθc(CH4(g)) = –890

OR change the arrow round and change the signs as below, remember, change direction, you change the sign BUT not the numerical energy value!

OR

ΔHθf(CO2(g)) + 2 x ΔHθf(H2O(l))

same numbers due to coincidence of enthalpy names

(c) doc b

+2O2(g) 

–2O2(g) 

= –ΔHθc(CH4(g))

= –(–890) = +890

CO2(g) + 2H2O(l)

Note that you double the enthalpy of combustion of hydrogen to make the cycle balance in molar terms

The cycle for the standard enthalpy of formation of methane, ΔHθf

From Hess's Law, add up the sequence of enthalpy changes via the lower 'staged route' to get the overall enthalpy change for the enthalpy of formation of methane from its elements in their normal stable states.

ΔHθf (methane) = (–393) + (2 x –286) + (+890) = –75 kJmol–1


2nd example of Hess's Law Cycle calculation

From the following thermochemical data

(1)  ½H2(g) + ½Cl2(g) ==> HCl(g)   ΔHθf(hydrogen chloride) = –92.3 kJmol–1

(2)  2C(s) + 3H2(g) + ½O2(g) ==> CH3CH2OH(l)   ΔHθf(ethanol) = –278.0 kJmol–1

(3)  2C(s) + 1½H2(g) + ½O2(g) + ½Cl2(g) ==> CH3COCl(l)   ΔHθf(ethanoyl chloride) = –275.0 kJmol–1

(4)  4C(s) + 4H2(g) + O2(g) ==> CH3COOCH2CH3(l)   ΔHθf(ethanol) = –481.0 kJmol–1

Calculate the enthalpy change for the reaction

(5)  CH3COCl(l) + CH3CH2OH(l) ==> CH3COOCH2CH3(l) +  HCl(g)  

ΔHθr@(esterification) = ??? kJmol–1

ΔHΨreaction(esterification) = ??? kJmol–1
CH3COCl(l) + CH3CH2OH(l) (c) doc b CH3COOCH2CH3(l) + HCl(g)

–ΔHθf(CH3COCl(l))

+ {–ΔHθf(CH3CH2OH(l))}

= –(–275.0) + {–(–278.0)}

(c) doc b            

ΔHθf(HCl(g))

+ ΔHθf(CH3COOCH2CH3(l))

= (–92.3) + (–481.0)

4C(s) + 41/2H2(g) + O2(g) + 1/2Cl2(g)

from {2C(s) + 11/2H2(g) + 1/2O2(g) + 1/2Cl2(g)} + {2C(s) + 3H2(g) + 1/2O2(g)}

Note that you didn't have to double or treble etc any enthalpy value because the molar ratio is 1 : 1 ==> 1 : 1

Adding up all the  ΔHθ's in the lower route of the cycle

ΔHθ298(esterification) = (+275.0) + (+278.0) + (–92.3) + (–481.0) = –20.3 kJmol–1

Note that the sign of enthalpy of formation of ethanoyl chloride and ethanol is reversed to fit in with the direction of change.


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3rd example of Hess's Law Cycle calculations

Problem solving from the following thermochemical data:


1.2b(ii) Solving enthalpy problems using an 'algebraic–equation style' method

BUT, remember, the question might specify solving the problem via a Hess's Law cycle!

Given the following data

(1)  C(s) + O2(g) ==> CO2(g)   ΔHθ = –393 kJmol–1

(2)  H2(g) + ½O2(g) ==> H2O(l)  ΔHθ = –286 kJmol–1

(3)  3C(s) + 4H2(g) ==> C3H8(g)  ΔHθ = –104 kJmol–1

Calculate the standard enthalpy of combustion of propane

(4)  C3H8(g) + 5O2(g) ==> 3CO2(g) + 4H2O(l)  ΔHθc,298(propane) = ??? kJ mol–1

What you do is rearrange, if necessary, the data equations and add up the results – both equation components and delta H values, cancelling out the equation components should leave you with the correct equation whose enthalpy value you require.

3C(s) + 3O2(g) ==> 3CO2(g) (1) add ΔHθ = 3 x –393 kJmol–1
4H2(g) + 2O2(g) ==> 4H2O(l) (2) plus ΔHθ = 4 x –286 kJmol–1
C3H8(g) ==> 3C(s) + 4H2(g) (3) plus ΔHθ = +104 kJmol–1  (equation and sign reversed)

C3H8(g) + 5O2(g) ==> 3CO2(g) + 4H2O(l)

(4) = ΔHθc,298(propane) = –2219 kJ mol–1

adding up (1) + (2) + (3) gives (4), cancelling out unwanted equation components,

the ==> treated as an = sign

Note that here you are using factors of 3 and 4 to make the cycle balance in molar terms


2nd example of 'algebraic' calculation style

Given the following thermochemical data:

(1)  1/2H2(g) + 1/2Cl2(g) ==> HCl(g) ΔHθ = –92.3 kJmol–1

(2)  2C(s) + 3H2(g) ==> CH3CH3(g) ΔHθ = –84.7 kJmol–1

(3)  2C(s) + 2H2(g) + Cl2(g) ==> ClCH2CH2Cl(l) ΔHθ = –166.0 kJmol–1

Calculate the enthalpy change for the reaction

(4)  2Cl2(g) + CH3CH3(g) ==> ClCH2CH2Cl(l) +  2HCl(g) ΔHθ = ??? kJmol–1

H2(g) + Cl2(g) ==> 2HCl(g) (1) add ΔHθ = 2 x –92.3 kJmol–1
CH3CH3(g) ==> 2C(s) + 3H2(g) (2) plus ΔHθ = +84.7 kJmol–1  (equation and sign reversed)
2C(s) + 2H2(g) + Cl2(g) ==> ClCH2CH2Cl(l) (3) plus ΔHθ = –166 kJmol–1

2Cl2(g) + CH3CH3(g) ==> ClCH2CH2Cl(l) +  2HCl(g)

(4) = ΔHθ298(chlorination reaction) = –265.9 kJ mol–1

adding up (1) + (2) + (3) gives (4), cancelling out unwanted equation components, ==> treated as an = sign

Note that you double the enthalpy of formation hydrogen chloride to make the cycle balance in molar terms


1.2b(iii) A 3rd method using the summation of enthalpies of reactants and products

A very simple example of an enthalpy summation method

molecule ethanoic acid +   ethanol ==> ethyl ethanoate +    water
equation CH3COOH(l) +   CH3CH2OH(l)

==>

CH3COOCH2CH3(l) +   H2O(l)
ΔHθf,298/kJmol–1 –487 –278   –481 –286

ΔHreaction = ∑Hproducts – ∑Hreactants

(this is still a form of using Hess's Law, but it just doesn't look like it!)

ΔHθreaction,298 = ∑ΔHθf,298(products) – ∑ΔHθf,298(reactants)

ΔHθesterification = {ΔHθf(ethyl ethanoate) + ΔHθf(water)} – {ΔHθf(ethanoic acid) + ΔHθf(ethanol)}

ΔHθesterification = {–481 + –286} – {–487 + –278}

ΔHθ(esterification reaction) = (–767) – (–765) = –2 kJmol–1

What would be ΔHθ(hydrolysis)? Answer! just reverse the sign! i.e. +2 kJmol–1


2nd example of enthalpy summation method

A more complicated example where you need to think more about mole ratios in the equation.

Given the following data from laboratory measurements

(1)  C(s) + O2(g) ==> CO2(g)   ΔHθf,298(carbon dioxide) = –393 kJmol–1

(2)  H2(g) + 1/2O2(g) ==> H2O(l)  ΔHθf,298(water) = –286 kJmol–1

(3)  C4H10(g) + 61/2O2(g) ==> 4CO2(g) + 5H2O(l)  ΔHθc,298(butane) = –2877 kJ mol–1

Calculate the standard enthalpy of formation of butane gas, which cannot be determined by experiment.

(4)  4C(s) + 5H2(g) ==> C4H10(g)  ΔHθ = ??? kJmol–1

To solve this you can use equation (3) and the data from equations (1) and (2) to obtain a value for equation (4)

ΔHreaction = ∑Hproducts – ∑Hreactants

for equation (3) ΔHcombustion(butane) = ∑ΔHθf(products) – ∑ΔHθf(reactants)

ΔHθc,298(butane) = {4 x ΔHθf(carbon dioxide) + 5 x ΔHθf,298(water)} – {ΔHθf(butane) + ΔHθf(oxygen)}

Since oxygen is an element, ΔHθf(oxygen) = 0, therefore after rearranging we get

ΔHθc,298(butane) = {4 x ΔHθf(carbon dioxide) + 5 x ΔHθf,298(water)} – {ΔHθf(butane)}

–2877 = {(4 x –393) + (5 x –286)} – ΔHθf(butane)

ΔHθf(butane) = 2877 – 1572 – 1430 = –125 kJmol–1


Key revision points about using Hess's Law

Hess’s Law states that the enthalpy change of a reaction is independent of the route taken, provided the initial and final conditions are the same.

It is crucial because many enthalpy changes cannot be measured directly, so Hess cycles and enthalpy data (formation, combustion, bond enthalpies) are used to calculate them.


  • Definition:

    • Hess’s Law: The total enthalpy change for a reaction is the same, no matter which route is taken, provided the starting and finishing conditions are the same.

    • Hess's Law is based on the law of conservation of energy.

  • Mathematical Forms e.g.

    • ΔHreaction = ∑Hproducts – ∑Hreactants

    • ΔHθreaction,298 = ∑ΔHθf,298(products) – ∑ΔHθf,298(reactants)

    • ΔHθreaction,298 = ∑ΔHθ298(bonds formed) – ∑ΔHθ298(bonds broken)

  • Energy Cycles:

    • Draw cycles with arrows showing alternative routes.

    • Label each arrow with the correct enthalpy change.

    • Use algebra to solve for the unknown enthalpy.

  • Applications:

    • Calculating enthalpy of reaction from enthalpies of formation.

    • Calculating enthalpy of reaction from enthalpies of combustion.

    • Using bond enthalpies to estimate enthalpy changes.

    • Explaining why experimental values differ from theoretical (bond enthalpy averages, incomplete combustion, non-standard conditions).


Common Misconceptions about Hess's Law

  • Sign Errors:

    • Students often forget that combustion enthalpies are negative (exothermic).

    • Wrongly add instead of subtracting enthalpy values.

  • Cycle Construction Mistakes:

    • Arrows pointing the wrong way in Hess cycles.

    • Forgetting to balance chemical equations before applying enthalpy data.

  • Confusing Routes:

    • Mixing up formation versus combustion cycles.

    • Forgetting that bond enthalpy calculations are approximate (average values).

  • Units:

    • Omitting “per mole” in kJ mol⁻Ή.

    • Using kJ instead of kJ mol⁻Ή in exam answers.


Exam Revision Tips when using Hess's Law

  • Learn Definitions Word-for-Word: Examiners expect precise definitions of Hess’s Law.

  • Practice Cycles: Draw neat, labelled Hess cycles for both formation and combustion routes.

  • Check Signs: Always double-check whether enthalpy values are positive or negative.

  • Balance Equations: Before using enthalpy data, ensure the chemical equation is balanced.

  • Use Algebra Carefully: which ever method you use and watch the enthalpy signs related to direction of enthalpy change.

  • Bond Enthalpy Calculations: Remember: breaking bonds = positive, making bonds = negative.

  • Cross-board Alignment: All exam boards (AQA, Edexcel, OCR, Salters, WJEC, CCEA, CIE, IB, AP) require:

    • Definition of Hess’s Law.

    • Construction of Hess cycles.

    • Calculations using formation, combustion, or bond enthalpies.

    • Awareness of experimental vs theoretical discrepancies.


Summary Table of typical errors when Hess's Law for calculations

Concept

Key Point

Common Error

Exam Tip

Hess’s Law

Enthalpy change independent of route

Forgetting conditions

Memorise definition

Formation Cycle

Use ΔHf values

Wrong states/elements

Balance equation first

Combustion Cycle

Use ΔHc values

Sign errors

Always negative values

Bond Enthalpy

Approximate via averages

Forget averages

State “approximate” in answers

Energy Cycles

Alternative routes

Wrong arrow direction

Draw arrows carefully


Final thought: Hess’s Law is the bridge between theory and experiment.

It allows indirect calculation of enthalpy changes that are impossible to measure directly, making it one of the most powerful tools in energetics.


 

for the next  problem!
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(c) doc b     (c) doc b

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Enthalpy calculation problems with worked out answers – based on enthalpies of reaction, formation, combustion

Energetics-Thermochemistry-Thermodynamics Notes INDEX

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QUICK INDEX for Energetics: GCSE Notes on the basics of chemical energy changes – important to study and know before tackling any of the three Advanced Level Chemistry pages

INDEX of ALL advanced level pages on thermochemistry and thermodynamics

Parts 1–3 here * Part 1a–b ΔH Enthalpy Changes 1.1 Advanced Introduction to enthalpy changes of reaction, formation, combustion etc. : 1.2a & 1.2b(i)–(iii) Thermochemistry – Hess's Law and Enthalpy Calculations – reaction, combustion, formation etc. : 1.2b(iv) Enthalpy of reaction from bond enthalpy calculations  : 1.3a–b Experimental methods for determining enthalpy changes and treatment of results and calculations : 1.4 Some enthalpy data patterns : 1.4a The combustion of linear alkanes and linear aliphatic alcohols : 1.4b Some patterns in Bond Enthalpies and Bond Length : 1.4c Enthalpies of Neutralisation : 1.4d Enthalpies of Hydrogenation of unsaturated hydrocarbons and evidence of aromatic ring structure in benzene : Extra Q page A set of practice enthalpy calculations with worked out answers ** Part 2 ΔH Enthalpies of ion hydration, solution, atomisation, lattice energy, electron affinity and the Born–Haber cycle : 2.1a–c What happens when a salt dissolves in water and why? : 2.1d–e Enthalpy cycles involving a salt dissolving : 2.2a–c The Born–Haber Cycle *** Part 3 ΔS Entropy and ΔG Free Energy Changes : 3.1a–g Introduction to Entropy : 3.2 Examples of entropy values and comments * 3.3a ΔS, Entropy and change of state : 3.3b ΔS, Entropy changes and the feasibility of a chemical change : 3.4a–d More on ΔG, free energy changes, feasibility and applications : 3.5 Calculating Equilibrium Constants from ΔG the free energy change : 3.6 Kinetic stability versus thermodynamic feasibility - can a chemical reaction happen? and will it happen?

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INDEX of all my notes on thermochemistry and thermodynamics

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