Chemical Thermodynamics Notes PDF

Summary

These notes cover fundamental concepts in chemical thermodynamics, including system types, properties (extensive and intensive), state and path functions, thermodynamic equilibrium, various processes (isothermal, isobaric, isochoric, adiabatic), and calculations related to work, internal energy, enthalpy, and entropy. These notes are suited for undergraduate studies in chemistry.

Full Transcript

# ABHISHEK SIR CHEMISTRY ## CHEMICAL THERMODYNAMICS **System:** A part of the universe under thermodynamic investigation. ### TYPES OF SYSTEM * **Open system:** exchanges both energy & matter * **CLOSED SYSTEM:** exchanges only energy & not matter. * **ISOLATED SYSTEM:** exchanges not allow exch...

# ABHISHEK SIR CHEMISTRY ## CHEMICAL THERMODYNAMICS **System:** A part of the universe under thermodynamic investigation. ### TYPES OF SYSTEM * **Open system:** exchanges both energy & matter * **CLOSED SYSTEM:** exchanges only energy & not matter. * **ISOLATED SYSTEM:** exchanges not allow exchange of either energy or matter ### EXTENSIVE Property: A property which depends on amount of matter * eg: Mass, Volume, internal energy, heat capacity, no. of moles. ### INTENSIVE Property: A property which is independent of amt of matter * eg: Pressure, Temp. ### State Function: Property which depends on state of the system & independent of path. * eg: density, enthalpy. ### Path function: Property which depends on path. * eg: klork, heat. ## Thermodynamic Equilibrium: A system is said to be in the thermodynamic equilibrium when it's state functions do not vary with time. Thermodynamics considered here is limited to equilibrium states. ### PROCESS & Its TYPES 1. **ISOTHERMAL PROCESS** It is the process in which temperature of the system remains constant. ΔT = 0 2. **ISOBARIC PROCESS.** It is the process in which pressure remains constant during the transformation. ΔP = 0 3. **ISOCHORIC PROCESS:** It is the process during which the volume of the system remains constant during the transformation. ΔV = 0 4. **ADIABATIC PROCESS** The process in which there is no exchange of heat between the system and surrounding is Adiabatic process. Q = 0 ## # Nature of klork: P = f /A : PV = f x V/A = f x d3/d2 : W = fd ## # SIGN CONVENTIONS * **Work done on the system:** +W * **Work done by the system:** -W * **Heat absorbed:** +Q * **Heat released:** -Q ## # Expression for PV Work f = -Pext x A - (1) W=Fxd .: W = -Pext x Axd... from (1) AV = Axod - (2) .: W = -Pext x ΔV .... from(2) ∴ W = -Pext (V2-V1) If V=0 W = -Pext x ΔV W = 0 ## # Concept of Maximum Work ΔP = P-Pext Pext = P-ΔP W = - Pext ΔV W = -(P-ΔP) ΔV ## # Expression for Maximum klork: | Step 1 | Step 2 | Step 3 | continued | | :------------ | :------------- | :------------- | :---------- | | Gas | Gas | gas | gas | | dv | dv↑ | dv↑ | | | | | | | dw = -Pext dv P-Pext = dp .: P-dp = Pext - (1) dw = -(P-dp). dv .... from (1) dw = - P. dv + dp. dv dw = - P. dv By integrating We get, final ∫dw = -∫ P.dv initiat PV=nRT Wmax = -∫ P.dv = -∫ dRT/V. dv V1 Wmax = -nRT∫ dv/V V1 W2 Wmax = -nRT ln (V/V1) Wmax = -nRT ln (V2-V1)/V1 Wmax = -nRT ln V2/V1 Wmax = -2.303 *nRT log V2/V1 Also P1V1 = P2V2 P2/ P1 = V2/V1 Wmax = -2.303 *nRT log P1/P2 ## # Internal Energy: It is made up of kinetic & potential energies of individual particles of the system ΔU = U2-U1 ## # FIRST LAW OF THERMODYNAMICS: ΔU = Q+W ## # St law of Thermodynamics for Various Processes 1. **Isothermal Process:** Temp is constant : ΔU = 0 0 = Q + W or W=-Q 2. **Adiabatic Process** Φ=0 -ΔV=-W 3. **Isochoric Process** W= - Pext ΔV ΔU = Q-Pext ΔV - ΔU = Qv 4. **Isobaric Process** ΔV≠0 Qp = AU + Pext ΔV ## # Enthalpy: Enthalpy of a system is the sum of internal energy of a system & the energy is equivalent to PV work. H = U + PV - (1) ΔH = H2-H1 - H1 = U1+P1V1 - (3) H2 = U2 + P2V2 - (4) Substituting eqn (3) & (4) in (2) ΔH = U2+P2V2-U1+P1V1 = (U2-U1) + (P2V2-P1V1) -ΔH = ΔU+PΔV Qp = ΔU+PΔV ΔΗ=Qp ## # Relationship btn ΔΗ & Δυ ΔH = ΔU + PΔV ΔH = ΔU+P(V2-V1) ΔH = ΔU + PV2-PV1 But PV = nRT PV2 = n2RT .: ΔH = ΔU+ (n2RT-n1RT) ΔH = ΔU + (n2-n1) RT "ΔH = ΔH + Δng RT ## # klork done in chemical Reactn: W=-Pext ΔV = -PΔV = -P(V2-V1) W = -PV2 + PV1 By Ideal gas eqn, PV1=n1RT PV2 = n2RT W1 = -n2RT+n1RT = -(n2-n1) RT W = - ΔngrT ## # BOND ENTHALPY: The enthalpy change required to break particular covalent bond in one mole of gaseous molecule to produce gaseous atoms /radicals. ## # HESS LAW: Overall enthalpy change for the reaction is equal to the sum of enthalpy changes of individual steps in the reaction. * 2H2 + N2 → N2H4 * N2H4 + H2 → 2NH3 * 3H2 +N2 → 2NH3 ## # Entropy: The disorder of randomness is measured by entropy Enthropy is a measure of molecular disorder or randomness. ## # 2nd Law of Thermodynamics: Total entropy of a system and it's surrounding increases in a spontaneous process. AS total = AS sys + ASsurr> 0 * **i** AS total > 0 → Spontaneous * **ii** AS total < 0 → Nonspontaneous. * **iii** AS total = 0 → At equilibrium. ## # Gibbs Energy: Gibbs energy is defined as G=H-TS Change in Gibbs energy ΔG = ΔH-TAS * **Relation 6th ΔG & ΔStotal** ΔStotal = AS sys + Assurr - (1) But ΔStotal = AS + AS surr - ASSurr = ΔH/T - (2) .: ΔStotal = AS - ΔH/T .- from 2 .. TΔStotal = ΔH-TAS ΔG = -TAS total ## # Gibbs function & equilibrium constant: AG= AG°+ RTen Q Consider a A+bB→CC+dD ΔG = ΔG° + R T ln QC or = ΔG°+RTen [C]c [D]d / [A]a[B]b ΔG = AG° + R T en Qp = AG° + RTen PCx PD^d / PA^a PB^b At Equilibrium, AG°=0 Qc = Kc Qp = Kp 0 = AG° + RTlnge & 0 = AG° + R.T Inkp or AG° = -RT In Kc & AG° = -RT Inkp .: AG°= -2.303RTlogo Kc & AG°=-2-303 RTlogiokp

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