Engineering Thermodynamics-second law of thermodynamics Mani Vannan M
This file consists of content which covers the basics of second law of thermodynamics,heat reservoir,heat source ,heat sink,refrigerator, heat pump,heat engine,carnot theorem,carnot cycle and reversed carnot cycle
this is my presentation about 2nd law of thermodynamic. this is part of engineering thermodynamic in mechanical engineering. here discussed about heat transfer, heat engines, thermal efficiency of heat pumps and refrigerator and its equation for perfect work done with best figure and table wise discription, entropy and change in entropy, isentropic process for turbines and compressor and many more.
Engineering Thermodynamics-second law of thermodynamics Mani Vannan M
This file consists of content which covers the basics of second law of thermodynamics,heat reservoir,heat source ,heat sink,refrigerator, heat pump,heat engine,carnot theorem,carnot cycle and reversed carnot cycle
this is my presentation about 2nd law of thermodynamic. this is part of engineering thermodynamic in mechanical engineering. here discussed about heat transfer, heat engines, thermal efficiency of heat pumps and refrigerator and its equation for perfect work done with best figure and table wise discription, entropy and change in entropy, isentropic process for turbines and compressor and many more.
A Proposal on Heat Engines, a topic in Chemical Engineering Thermodynamics.
This work aim at studying the process involved in the conversion of heat energy to mechanical work and in effect the principles which engine operate.
Heat engines are systems that convert heat or thermal energy to mechanical energy which can then be used to do mechanical work. This is done basically by bringing a working substance from a higher state temperature to a lower state temperature. The working substance is brought to a high temperature by a heat source which generates thermal energy. This energy is converted to work by exploiting the proportion of the working substance during which the heat is transferred to the colder destination until it reaches a lower temperature state.
The conversion of this heat to mechanical work follow certain routes which ends at the start point and hence are called cycles. This work will in essence focus on these cycles. Otto cycle, Atkinson cycle and brayton cycle are some of the cycle that represent models for heat engine operations. The condition to which the working fluid is subjected in the process, is what distinguishes one cycle from the other.
A Proposal on Heat Engines, a topic in Chemical Engineering Thermodynamics.
This work aim at studying the process involved in the conversion of heat energy to mechanical work and in effect the principles which engine operate.
Heat engines are systems that convert heat or thermal energy to mechanical energy which can then be used to do mechanical work. This is done basically by bringing a working substance from a higher state temperature to a lower state temperature. The working substance is brought to a high temperature by a heat source which generates thermal energy. This energy is converted to work by exploiting the proportion of the working substance during which the heat is transferred to the colder destination until it reaches a lower temperature state.
The conversion of this heat to mechanical work follow certain routes which ends at the start point and hence are called cycles. This work will in essence focus on these cycles. Otto cycle, Atkinson cycle and brayton cycle are some of the cycle that represent models for heat engine operations. The condition to which the working fluid is subjected in the process, is what distinguishes one cycle from the other.
This presentation briefly describes the Carnot cycle and the theorem associated with it. It also states about the Carnot reversible engine with the help of diagrams it illustrates the processes that occur inside the Carnot engine SOURCE: The source should be at a fixed high-temperature 𝑻_𝟏 from which the heat engine can draw heat. It has infinite thermal capacity and any amount of heat can be drawn from it at constant temperature 𝑻_𝟏.
SINK: The sink should be at a fixed lower temperature 𝑻_𝟐 to which any amount of energy can be rejected. It also has infinite thermal capacity and its temperature remains at a constant temperature 𝑻_𝟐.
WORKING SUBSTANCE: A cylinder with non-conducting sides and a conducting bottom contains the perfect gas as a working substance. A perfect non-conducting and frictionless piston are fitted into the cylinder. The working substance undergoes a complete cyclic operation. A perfect non-conducting stand is also provided so that the working substance can undergo an adiabatic operation.The most efficient heat engine cycle is the Carnot cycle, consisting of two isothermal processes and two adiabatic processes. The Carnot cycle can be thought of as the most efficient heat engine cycle allowed by physical laws. When the second law of thermodynamics states that not all the supplied heat in a heat engine can be used to do work, the Carnot efficiency sets the limiting value on the fraction of the heat which can be so used.
In order to approach the Carnot efficiency, the processes involved in the heat engine cycle must be reversible and involve no change in entropy. This means that the Carnot cycle is an idealization, since no real engine processes are reversible and all real physical processes involve some increase in entropy.The working substance is subjected to the following cycle or quasi-static operations known as Carnot’s cycle to obtain a continuous supply of work.
ISOTHERMAL EXPANSION: The cylinder is first placed on the source so that the gas acquires the temperature T1 of the source. It is then allowed to undergo quasi-static expansion. As the gas expands, its temperature tends to fall. Heat passes into the cylinder through the perfectly conducting base which is in contact with the source. The gas, therefore, undergoes slow isothermal expansion at the constant temperature T1. Let the working substance during isothermal expansion goes from its initial state A(𝑷_𝟏,𝑽_𝟏,𝑻_𝟏) to the state B(𝑷_𝟐,𝑽_𝟐,𝑻_𝟏) at constant temperature T1 and does work W1 given by
ADIABATIC EXPANSION: The cylinder is now removed from the source and placed on the insulating stand. The gas is allowed to undergo slow adiabatic expansion, performing external work at the expense of its internal energy, until its temperature falls to T2, the same as that of the sink.
This process is represented by the adiabatic BC, starting from state B (𝑷_𝟐,𝑽_𝟐,𝑻_𝟏) to the state C(𝑷_𝟑,𝑽_𝟑,𝑻_𝟐) . In this process, there is no tras
The second law of thermodynamics is explored in this lecture. Topics covered include:
Introduction to the second law
Thermal energy reservoirs
Heat engines
Thermal efficiency
The 2nd law: Kelvin-Planck statement
Refrigerators and heat pumps
Coefficient of performance (COP)
The 2nd law: Clasius statement
Perpetual motion machines
Reversible and irreversible processes
Irreversibility's, Internal and externally reversible processes
The Carnot cycle
The reversed Carnot cycle
The Carnot principles
The thermodynamic temperature scale
The Carnot heat engine
The quality of energy
The Carnot refrigerator and heat pump
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http://sandymillin.wordpress.com/iateflwebinar2024
Published classroom materials form the basis of syllabuses, drive teacher professional development, and have a potentially huge influence on learners, teachers and education systems. All teachers also create their own materials, whether a few sentences on a blackboard, a highly-structured fully-realised online course, or anything in between. Despite this, the knowledge and skills needed to create effective language learning materials are rarely part of teacher training, and are mostly learnt by trial and error.
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Letter from the Congress of the United States regarding Anti-Semitism sent June 3rd to MIT President Sally Kornbluth, MIT Corp Chair, Mark Gorenberg
Dear Dr. Kornbluth and Mr. Gorenberg,
The US House of Representatives is deeply concerned by ongoing and pervasive acts of antisemitic
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5. In thermodynamics, a heat engine is a system
that converts heat or thermal energy to
mechanical energy, which can then be used to do
mechanical work. It does this by bringing a
working substance from a higher state
temperature to a lower state temperature.
6. Parts Of Heat Engine
Hot Body
(source of heat)
Q1
Cold Body
(absorbs heat)
Q2
W
Working
substance
7. Defination:
Carnot’s Engine: In order to express an
explanation of the convertion of heat into
work , Sadi Carnot imagines an idle heat engine
which is known as Carnot’s Engine.
Heat
source
sink
Heat
instractor
deck
Cylender With piston
9. Carnot’s Cycle:
cycle in which the working substance starting a state of
certain temperature, pressure and volume is made to
undergo two successive expansions (isothermal &
adiabatic) and then two successive compressions and then
brought back finally to its initial state is called Carnot
cycle.
10. Adiabatic process: The process in which a system neither
receives heat nor rejects heat is called adiabatic process.
In this process a gas undergoes changes in pressure,
volume and temperature under thermal isolation.
IsoThermal Process: When a gas undergoes a change in
pressure and volume at constant temperature, the gas
is said to undergo an isothermal change, and the
process in which the change takes place is called
isothermal process.
17. Isothermal process is possiable if it is very slow and
Adiabatic process is possiable if it is very fast. This
Alternate Combination of very fast very slow process is
not posiable to achieve in actual practice.