bme slide(remedial).ppt
TRANSCRIPT
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Thermodynamics
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Therme - HeatDynamis - Power
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System
A quantity of matter or regionin space chosen for study
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Surroundings
The matter or region outside thesystem
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Boundary
The real or imaginary surface thatseparates the system from itssurroundings
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System
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Types of thermodynamic system
Open System
Closed SystemIsolated System
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Open System
Transfer of matter and energyacross the boundary
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Closed System
No mass transfer across theboundary of the system, energytransfer is possible
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Isolated system
No energy and mass transfer
No interaction b/w system &surroundings
Energy & mass are fixed
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Thermodynamic Properties
Every system has certaincharacterestics by which its
physical condition may bedescribed They are macroscopic in nature
Properties are co-ordinates todescribe the state of the system
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Intensive properties
Extensive properties
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Thermodynamic State Path
Process Cycle
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Thermodynamic State
When all the properties need to
describe the condition of thesystem, have defenite values,the system is said to exist in
defenite state
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Path
The succession of state passedthrough, during a change ofstate is called path
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Process
When the path is completelyspecified, the change of state iscalled process
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Thermodynamic Cycle
A series of state changes suchthat, the final state is identicalwith initial state
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Thermodynamic Equilibrium
A system is said to be exist in
thermodynamic equilibrium, whenno change in any macroscopicproperty is registered, if the system
is isolated from its surroundings
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Conditions for thermodynamicequilibrium
Mechanical equilibriumChemical equilibriumThermal equilibrium
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Mechanical equilibriumIf there is no unbalanced force withinthe system itself and also b/w system
& surroundings, the system is said tobe in mechanical equilibrium
If an unbalanced force exists, either thesystem or both the system &surroundings will undergo a changeof state till mechanical eqbm isattained
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Chemical equilibrium
If there is no chemical reaction or
transfer of matter from one part ofthe system to another. Such asdiffusion or solution, the system issaid to exist in chemical eqbm.
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Thermal equilibrium
When a system is in mechanical &chemical equilibrium, is seperated
from its surroundings by diathermicwall & if there no spontaneouschange in any property of the
system, the system is said to existin thermal equilibrium
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Quasi static process
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Temperature
It is hotness or coldness of a body
When a body brought into contactwith another body, at differenttemperature, heat is transfered frombody at higher temperature to bodyat lower temperature
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Zeroth law thermodynamics
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Zeroth law thermodynamics
If two bodies are in thermalequilibrium with a third body, theyare also in thermal equilibrium witheach other
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Zeroth law thermodynamics
When a body A is in thermal eqbm
with body B, and also seperatelythermal eqbm with body C, then thebodies B & C will be in thermaleqbm
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Temperature scaleIt is a way to measure temperature quantitatively
Celcius scale (water)Freezing point 0 CBoiling point 100 C
Kelvin scale (water)Freezing poitn 273 KBoiling point 373 K
Fahrenheit scale (water)Freezing point 32 FBoling point 212 F
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Heat (Q)
Energy transfer across the boundaryof the system on account of thetemperature differenceHeat is a path function
Heat transfered to the system (+) veHeat transfered from the system(-) ve