Download presentation
Presentation is loading. Please wait.
Published byNándor Pataki Modified over 6 years ago
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
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.