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    CHAPTER 2

    THE FIRST LAW OF THERMOYNAMICS

    Group 5

    1. Riduan

    2. Novita Sari3. Putri Eka Nurhikmah Sari

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    SOME BASIC UNDERSTANDING

    Some basic understanding of thermoynamics is

    much related to:

    system and environment,

    the state of the system and the equation of

    state,

    State function, Changes in circumstances,

    Heat and work.

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    4

    system and environment :transfer of energy (E) & materr (m)

    System(Focus of attentoin)

    environment

    environment

    environment

    An open system Closed System Isolated System

    environment

    E

    &

    m E

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    5

    Open

    mass & energyShift:

    Closed

    Energy

    Isolated

    Di not happen anything

    SYSTEM

    ENVIRONMENT

    6.2

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    6

    The State of The System

    the state variabel system :

    n (the amount of substance)

    V (volume)

    p (pressure)

    T (temperature)

    E.g. Gas equation of state:pV = nRT

    p = p (n, T, V)

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    Condition function

    Condition function is each system

    characteristic which only concerned with

    beginning condition and final condition

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    In thermodinamic we know some

    condition function :

    In energy (u; U)

    Entalphy (h; H),

    Entropi (s; S),

    Gibbs free energy (g; G),

    Helmholtz free energy (a; A).

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    One of the important characteristic of

    differential condition function is total

    differential (differential ekstrak),some of total

    differrential characteristic are:

    2

    1. if dz = z2z1, so dz is a

    1

    Total diferenial

    2. If dz = 0, so dz is a total diferential

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    3. occurred Euler formula:

    if dz = M(x,y) dx + N(x,y) dy so

    M N

    = (2.1)

    y x x y

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    Changing condition :

    The process which occurred in a system can be

    consist of:

    1. Reversibel process is a process which

    system always in equilibrium condition or

    quasy-static

    2. Irreversibel process is process which cannt

    fulfil reversibel process

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    2.1.6 Work

    Work is a form of energy that is not ketiap heatexchanged between the system and theenvironment

    Figure 2.2. Work exchange between the systemwith its environment

    W (+) W(-)

    Environment

    System

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    Sorts of forms of work:

    1. electrical work2. mechanical work

    3. magnetic work

    4. work volume

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    work volume

    1. Expansion work one step

    Expansion work is the work that occurs whenthe system volume swell against pressure

    environment.

    Work performed by the system: W = mgh

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    Expansion work one step

    M

    M

    T.P1.V1

    T.P2.V2

    S

    S

    S

    S

    S

    S

    S

    Sh

    (a) Start state (b) Final state

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    W=-P1V

    W=-P1(V2-V1) (2.5)

    W = the total work that accompanies the system

    state changes

    P1 = pressure outside (environment) caused mass

    V2 = volume of the system at the final state

    V2 = volume of the system at the initial state

    (-) = Adjust system that works

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    P1.V1

    P2

    P1

    P2.V2

    }rentangP1V1 V2 V

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    P1P2

    Equation 2.5 is not just for work expansion,

    but also the work of compression

    In compression, V2

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    2. Two-step expansion work

    If the state of the system is determined on

    the state of his three so-called two-stepexpansion work (2-stroke)

    W = W + W first step second step (2.6)

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    Expansion work two step

    VV2

    P1

    P1

    P1

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    The shaded area stating the amount of

    work that occurs in a two-step expansion.objec changes to the system with more

    steps will be accompanied by greater job.

    The shaded area in the two-step systemthat works greater than the work one step.

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    P

    P

    P

    P1.V1

    P2.V2

    V1 V V2 V

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    Pl is the pressure of the environment outside

    the detention system can be consideredequal to the system pressure (P), Pl = P, so

    that equation (2.6) becomes

    dW = -P dV (2.7)

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    The total number of workers who produced

    the reversible expansion can be obtained byintegrating equation (2.7)