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    Himanshu Vasistha

    Thermodynamics-1

    for UPSC IES and GATE 2014 Mechanical Engineering

    By

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    Thermodynamics

    The branch of science that deals with the relations

    between heat and other forms of energy, and ofthe relationships between all forms of energy.

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    System and Surroundings

    !A system is a finite quantity of matter or a

    prescribed region of space.

    ! The actual or hypothetical envelope

    enclosing the system is called Boundary.

    ! Boundary may be fixed or moveable.

    ! Everything external to the system is

    called Surroundings.

    !A System and its Surroundings together

    comprise a Universe.

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    Types of System

    ! Open System- In this matter and

    energy flow in or out of the

    system. Most of the Engineering

    Systems are Open Systems.

    ! Closed System- In this theboundary is impervious to the

    flow of matter. A mass of gas and

    vapour in an engine cylinder, with

    a continuous boundary may be

    regarded as a Closed System.

    ! Isolated System- In this the

    system neither exchanges energy

    nor matter with another system

    or surroundings.

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    Properties, Processes and Cycles

    When properties like, volume, pressure, temperature etc. of

    a system have definite values, then the system is said to

    exist at a definite State.

    Properties are the coordinates which describe the state of a

    system.

    An operation in which one or more properties of a system

    changes is called change of state.

    The succession of States passed during a change of state is

    called aprocess.

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    Process and Cycle

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    Thermodynamic Equilibrium

    Thermodynamic equilibrium exists in a system when no change of

    macroscopic properties is registered, if the system is isolated from

    its surroundings.

    An isolated system always reaches in course of time a state ofthermodynamic equilibrium and can never depart from it

    spontaneously.

    If a system is in equilibrium, no spontaneous change in

    macroscopic property can occur.

    Thermodynamic equilibrium exists when, Mechanical, Thermal and

    Chemical equilibrium exist simultaneously.

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    Zeroth Law of Thermodynamics

    When a body A is in thermal equilibrium with a body B, and

    also separately with a body C, then B and C will be in thermal

    equilibrium with each other.

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    ! Zeroth law is the basis of

    temperature measurement.

    ! There are five kinds of

    thermometer, each with its own

    thermometric property.

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    Thermometer Thermometric property

    Constant vol. gas

    thermometerPressure

    Constant pressure gas

    thermometerVolume

    Electrical Resistance

    ThermometerResistance

    Thermocouple Thermal e.m.f

    Mercury in glass

    thermometerLength

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    Work transfer

    Work is done by a force as it acts upon a body moving in

    the direction of the force.

    When work is done by a system, it is taken to be positive,and if work is done on a system, it is taken to be negative.

    Work is one of the forms in which a system and its

    surroundings interact.

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    Displacement work

    ! When the piston moves, the

    volume changes, and the workdone can be calculated as

    described in the figure.

    ! The magnitude of the work doneis the area under the P-V diagram.

    ! The path shown on the P-V

    diagram must pass through

    equilibrium states; i.e. must be

    Quasi Static.

    ! The integration to calculate the

    work done can be performed onlyif the process is quasi static.

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    Path Function and Point Function

    Area under the PV curve gives the amount of work done,

    so it is not a function of the end states of a process, but

    depends upon the path the process takes. Therefore,

    work is called apath function.

    Thermodynamic properties arepoint functions, since for a

    given state, there is a definite value for each property.

    Path Functions are called inexact or imperfect differential.

    Point Functions are called exact or perfect differential.

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    Work in various Quasi

    Static Processes

    PVk= constant

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    Open and closed

    system work

    ! The open system work is

    calculated by plotting it on

    volume axis.

    ! The closed system work is

    calculated by plotting it on

    pressure axis.

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    Zero work transfer

    Work transfer is ONLY identified at the boundaries of a

    system. Therefore, it can be termed as a boundary

    phenomenon.

    The expansion of a gas against vacuum is called free

    expansion. In this case the work done by the system is

    zero, as no work crosses the boundary.

    This free expansion process is not a quasi static process,

    although the initial and end states are in equilibrium.

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    Heat Transfer

    It is defined as a form of energy that is transferred across

    a boundary due to a temperature difference.

    The direction of heat transfer is from a body at hightemperature to a body at lower temperature.

    Heat flow into a system is taken to be positive, and heat

    flow out of a system is taken to be negative.

    Heat transfer is a transit, and occurs only at the boundary.

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    Important points for a Heat and Work Transfer

    Heat and work transfer are energy interactions.

    The same e#ect in a closed system can be brought

    about either by heat transfer or work transfer.

    Both transfers are boundary phenomena, and both

    represent energy crossing the boundaries of the system.

    It is wrong to say 'total heat' of a closed system as heat and workare not a property of a system. They cannot be stored in the

    system. Both are energies in transit

    Heat transfer is the energy interaction due to temperature di#erence

    only. All other energy interactions can be termed as work transfer

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