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Thermodynamics Chander Gupta and Matt Hagopian. Introduction into Thermo Thermodynamics is the study of energy and its transformations Thermochemistry.

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Presentation on theme: "Thermodynamics Chander Gupta and Matt Hagopian. Introduction into Thermo Thermodynamics is the study of energy and its transformations Thermochemistry."— Presentation transcript:

1 Thermodynamics Chander Gupta and Matt Hagopian

2 Introduction into Thermo Thermodynamics is the study of energy and its transformations Thermochemistry deals with the transformations of energy (usually heat) during chemical reactions

3 Types of Energy Kinetic Energy- energy associated with the motion of an object KE=1/2mv 2 Potential Energy- energy an object possesses relative to others Energy is measured in Joules (J) or calories (cal) 1 cal = the energy required to increase the temperature of 1 gram of water by 1°C = 4.184 J 1 J = 1 (kg x m 2 )/s 2 Potential Energy is converted into Kinetic Energy

4 System and Surroundings Everything that is singled out in a reaction is called the system (reactants and products) Everything outside of this system is the surroundings Closed systems are the ones that are most readily studied - they can exchange energy but not matter with surroundings

5 Transferring Energy: Work and Heat Work is the energy used to move an object against force (w= F x d) Energy can be transferred back and forth between a system and its surroundings in the form of work and heat The measurement of work is usually Joules (J)

6 The First Law of Thermodynamics Energy is conserved - it cannot be created or destroyed Any energy lost by the system must be gained by the surroundings Internal energy- the sum of all kinetic and potential energy of a system ∆E = E final - E initial ∆E+ = energy gained from surroundings ∆E- = energy lost to surroundings ∆E = q + w (q = sum of heat transferred in/out of system, and w = work done on or by the system) Endothermic processes absorbs heat from the surroundings Exothermic processes release heat to the surroundings

7 Enthalpy (∆H) ∆H = the heat flow = enthalpy ∆H rxn = H products - H reactants ∆H- = exothermic reaction ∆H+ = endothermic reaction Ex. 2 H 2 (g) + O 2 --> 2H 2 O (g) ∆H = -483.6 kJ The enthalpy of the products is lower than the enthalpy of the reactants, therefore ∆H is negative

8 Properties of Enthalpy Enthalpy is an extensive property: the magnitude of ∆H is proportional to the amount of reactant used in the reaction Enthalpy change for a rxn is equal in magnitude, but opposite sign, for the reverse rxn Enthalpy change depends on the state of the reactants and products - 2H 2 O (l) --> 2H 2 O (g) ∆H=+88 kJ

9 Calorimetry The measurement of heat flow Calorimeter is a device used to measure heat flow The amount of heat a substance gains differs from substance to substance Heat capacity (C) = the amount of heat required to raise the temperature of a substance 1 K (or 1°C) The greater the heat capacity, the greater the amount of heat required to increase the temp.

10 Calorimetry Molar Heat Capacity = C molar = heat capacity of one mole of substance Specific heat= heat capacity of one gram of substance q= m x C x ∆T q= the change in heat of the substance m=the mass C=specific heat (J/g-K or J/g-°C) ∆T = change in temperature (T final - T initial )

11 Calorimetry ∆H = q p, if carried out under constant pressure We assume the calorimeter does not lose heat and doesn’t absorb it - the heat is fully confined in the system In an exothermic/endothermic reaction, the heat lost/gained by the system is gained/lost by the surroundings, so q soln =-q rxn Combustions take place in bomb calorimeters- heat from the combustion is measured by the ∆T if the surrounding water We must know the heat capacity of the calorimeter q rxn = -C cal x ∆T

12 Hess’s Law If a reaction is carried out in a series of steps, ∆H for the overall reaction will equal the sum of the enthalpy changes for the individual steps Example: CH 4(g) + 2O 2(g) --> CO 2(g) + 2 H 2 O (g) ∆H =-802kJ 2H 2 O (g) --> 2H 2 O (l) ∆H = -88kJ CH 4(g) + 2O 2(g) + 2H 2 O (g) --> CO 2(g) + 2 H 2 O (g) + 2H 2 O (l) ∆H = -890kJ Net equation : CH 4(g) + 2O 2(g) --> CO 2(g) + 2 H 2 O (l) ∆H=-890kJ

13 Enthalpy of Formation ∆H f = the enthalpy change for the reaction in which a substance is formed from its elements ∆H° = standard enthalpy change that takes place when all reactants and products are at 1 atm pressure and usually 298 K These combined to form standard enthalpy of formation ∆H° f, which forms one mole of substance from its elements in their most stable form under the standard conditions For any element in its most stable state, ∆H° f = 0. C, H 2, O 2, etc. ∆H° rxn = ∑n ∆H° f (products) - ∑m ∆H° f (reactants)

14 Covalent Bond Energies Strength of a covalent bond is measured by its bond enthalpy- molar enthalpy change upon breaking a bond Strength of covalent bonds increase with number of shared electron pairs (C=C > C-C). Bond length decreases with increasing number of bonds Breaking bonds is an endothermic process Forming bonds in an exothermic process Example: CH 4 + 2 O 2 --> CO 2 + H 2 O [4(C-H) + 2 (O=O)] - [2(C=O) + 2(O-H)] Bond energies are in Appendix 18

15 Changes of State As a substance changes phases, the molecules increase in vibrational frequency Fusion- melting -∆H fus - kJ/mol Vapor pressure increases with increasing temp. Boiling- ∆H vap ∆H vap > ∆H fus

16 Heating Curves Phase changes are endothermic processes The rise in the graph represents the rise in temperature The plateaus represent the phase changes First plateau- melting Second plateau- boiling Energy required for total curve is the sum of the individual parts (q 1 + q 2 + q 3 + q 4 + q 5 ) Plateau points- q=m∆H fus or q=m∆H vap Source: www.bbc.co.uk

17 Entropy (S) Molecules undergo 3 types of motion: Translational - entire molecule moves Vibrational - atoms of molecule move back and forth Rotational- entire molecule spins Entropy increases as these motions increase, and also with increases in volume and temperature Gases are the most random, and therefore have ∆S +

18 Entropy 2nd law of thermodynamics- ∆ S univ = ∆S sys + ∆S surr 3rd law of thermodynamics- entropy of a pure crystalline solid at 0 K = 0. There is no movement at absolute zero Standard molar entropy = S° ∆S+ means increasing randomness ∆S° = ∑n ∆S° f (products) - ∑m ∆S° f (reactants) ∆S is measured in J/K

19 Sample Problem Calculate ∆S° for: N 2 (g) + 3 H 2 (g) --> 2 NH 3 (g) ∆S° N 2 = 191.5 J/mol-K ∆S° H 2 = 130.6 J/mol-K ∆S° NH 3 = 192.5 J/mol-K

20 Answer N 2 (g) + 3 H 2 (g) --> 2 NH 3 (g) [2 mol (192.5 J/mol-K)] - [1 mol (191.5 J/mol-K) + (3 mol) (130.6 J/mol-K) ∆S° = -198.3 J/K

21 Gibbs Free Energy ∆G = ∆H - T ∆S ∆G- means spontaneous reaction At equilibrium the process is reversible and ∆G = 0 ∆G° f is analogous to ∆H° f. Equals 0 for substances in elemental state

22 Gibbs Free Energy Under nonstandard conditions, ∆G is related to ∆G° and the value of the reaction quotient, Q. ∆G = ∆G° + RT ln Q At equilibrium, (∆G=0 Q=K), ∆G° = -RT ln K Q = [products] x / [reactants] y ∆G = kJ/mol ∆G° = ∑n ∆G° f (products) - ∑m ∆G° f (reactants) K 1, products favored (highly spontaneous). K=1, rxn is in equilibrium


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