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ENERGY ANALYSIS GROUP THREE THERMODYNAMICS SHARAFATU BADARU

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Presentation on theme: "ENERGY ANALYSIS GROUP THREE THERMODYNAMICS SHARAFATU BADARU"— Presentation transcript:

1 ENERGY ANALYSIS GROUP THREE THERMODYNAMICS SHARAFATU BADARU
UGWU CHINYERE AUGUSTINE EMEKA EKENE INNOCENT

2 Energy Balance Concerned with energy changes and energy flow in a chemical process. Conservation of energy – first law of thermodynamics i.e. accumulation of energy in a system = energy input – energy output

3 Energy balance W system mass out mass in Hin Hout Q

4 Uses Heat required for a process Rate of heat removal from a process
Heat transfer/design of heat exchangers Process design to determine energy requirements of a process Pump power requirements (mechanical energy balance) Pattern of energy usage in operation Process control Process design & development etc

5 Energy balance techniques
Complete mass balance/molar balance Calculate all enthalpy changes between process conditions and standard/reference conditions for all components at start (input) and finish (output). Consider any additional enthalpy changes Solve enthalpy balance equation

6 Laws of Thermodynamics and Energy Balance
Energy cannot be created nor destroyed but can change from one form to another therefore energy accumulation =input-output Kinetic→ Motion → 1/2mv2 Potential → Position → mgh Internal→ Due to molecular interaction Q heat ∆T- between system + surrounding energy transfer as a result of temp difference Q - + when transfer to system from surrounding w- work is response to driving force W is +ve when done on the system by the surrounding –ve when system does work on surrounding Enthalpy is a relation for U +PV

7 For a closed system

8 Energy balance for an open system

9 For an open system

10 CLOSED AND OPEN SYSTEM Open-mass crosses the boundary Closed-mass does crosses the boundary Closed ∆U + ∆Ep + ∆Ek = Q-W + Q= heat transfer to system W= work done on system no acceleration ∆E No change in height ∆Ep System T= surrounding T, insulated →Q=O adiabatic no moving parts, electric current or radiation at the boundry, then w=o

11 CLOSED AND OPEN SYSTEM contd
Open ∆H + ∆Ep + ∆Ek= Q-W (per unit time) ∆H→Hfinal – Hinitial Q,W- depends on boundary Consider a cylinder with a movable piston moves slowly to compress the gas Neglecting ∆Ep, what is the energy balanced? (closed system) Q-W = ∆U Isothermally Q=W Adiabatic Q=O ∆U=-W

12 Thank you for listening
References The Properties of Gases and Liquids, R. Reid Elementary Principles of Chemical Processes, R.M.Felder and R.W.Rousseau Thank you for listening


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