Translog Production Function

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    Derivation of Translog form from CES form

    The constant elasticity of substitution form of production function can be written as:

    1

    1 1 2 2y A X X

    = + .(B1)

    The CE form shown abo!e has constant elasticity of substitution "i!en by#

    1

    1

    =

    Ta$in" the lo" on both sides of the e%uation (B1) it becomes#

    1 1 2 2

    1ln ln ln( )y A X X

    = + .(B2)

    &et 1 1 2 2( ) ln( )f X X = + ...(B')

    1 1 1 2 2 2

    1 1 2 2

    ln ln( )

    X X X X f

    X X

    =

    +

    ..(B)

    ( ) ( )

    ( )

    2

    1 1 2 2 1 1 1 1 1 1 2 2 2 1 1 1 2 2 2

    2

    1 1 2 2

    ( ) (ln ) ln ln ln ln( )

    X X X X X X X X X X X Xf

    X X

    + + + =+

    E*pandin" +f, in a Taylor series around - and ta$in" terms upto the second order:

    Taylor series around - upto second order can be "i!en as:

    2(-) (-)

    ( ) (-) 1. 2.

    f f

    f f = + + .. (B/)

    1 2(-) ln( )f = +

    1 2 2

    1 2

    ln ln(-)

    X Xf

    =

    +

    ( )( ) ( )

    2 21 21 2 1 22

    1 2

    (-) ln ln 2 ln lnf X X X X

    = + +

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    2

    ( )

    22 21 2 2 1 2

    1 2 1 2 1 221 2 1 2

    ln ln( ) ln( ) (ln ) (ln ) 2 ln ln

    2

    X Xf X X X X

    = + + + + + +

    ubstitutin" the !alue of ( )f in e%uation (B2)#

    ( )( )

    ( )( )

    ( ) ( )

    21 2 1 2 1 21 2 12

    1 2 1 2 1 2

    21 2 1 2 1 22 1 2 1 22 2 2

    1 2 1 2 1 2

    ln( ) 1ln ln ln ln ln

    2

    1 1 1ln ln ln ln ln

    2 2 2

    y A X X X

    X X X X X

    += + +

    + + +

    + ++ + +

    ( ) ( ) ( ) ( )2 2-- -1 1 -2 2 11 1 22 2 12 1 2 21 1 2ln ln ln ln ln ln ln ln lny a a X a X a X a X a X X a X X= + + + + + +

    0rom the e%uation some restrictions should be applied#

    ( ) ( )

    ( )

    ( )1 21 2

    -1 -2

    1 2 1 2 1 2

    1a a

    ++ = + = =

    + + +

    ( ) ( )1 2 1 2

    11 12 22 212 2

    1 2 1 2

    -a a a a

    + = + = + =

    + +

    ( )1 2

    12 21 2

    1 2

    a a

    = =

    +

    These are the conditions of homo"eneity of de"ree one in prices and they are necessary

    to maintain symmetry of cross effects.

    Testing of Stolper Samuelson Theorem using Translog Production

    Function Form:

    &et there be "oods and factors of production. The translo" function can be written

    as:

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    = = = =

    == = =

    +

    ++++=

    M

    k

    M

    l

    N

    i

    M

    k

    kiiklkkl

    M

    k

    kkj

    N

    i

    N

    i

    N

    j

    iijii

    VpcVVb

    VbppapaaG

    1 1 1 1

    1

    -

    1 1 1

    ---

    lnlnlnln2

    1

    lnlnln

    2

    1lnln

    3here iP is price ofthi "ood and kV is the supply of

    thk factor. ymmetry of cross

    effects re%uires:

    jiij aa =

    4nd lkkl bb =

    &inear homo"eneity in 5 and 6 re%uires#

    ==i k koi ba 1-

    ======i j k l i k ikikklklijij ccbbaa -

    4ssumin" output of "ood i :

    ( )ii Vfy =

    7utput is the function of factor inputs. 8ere ob9ecti!e is to ma*imise the ;6 function#

    =

    =N

    i

    iiypG1

    ub9ect to: VVi # where 5 is the total factor input. is ma*imum when ine%uality

    holds#

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    ( )

    ==

    N

    i

    ii VfpG1

    ( ) ( )=

    +=N

    i

    iii VfpVfp2

    1

    ( )==

    +

    =

    N

    i

    ii

    N

    i

    i VfpVVfp22

    1

    0rom the en!elope theorem# we can differentiate this with respect to p and V # holdin"

    the optimum input choices iV constant.

    i

    i

    yp

    G=

    iiii

    ii

    sGpy

    Gp

    pG

    pG === lnln

    This is share of "ood i in ;6.

    imilarly# kk

    wV

    G=

    This is price of ith factor.

    kkkk

    ki

    sG

    Vw

    G

    V

    V

    G

    V

    G==

    =

    ln

    ln

    This is share of ;6 de!oted to factor $.

    Derivation of Share Equation:

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    5

    ==

    ++=

    =

    M

    k

    ik

    N

    j

    jiji

    i

    i Vcpaa

    p

    Gs

    11

    - lnln

    ln

    ln

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    ==++++=

    N

    i

    kiik

    M

    l

    lklkkk pcpcVbVabs2

    11

    2

    11- lnlnlnln

    = == =

    ++=N

    i

    N

    i

    iikik

    M

    l

    M

    l

    klklkk pcpcVbVbbs2 2

    1

    2 2

    11- lnlnlnln

    = =

    +

    +=

    M

    l

    N

    i

    i

    ik

    l

    klikp

    pc

    V

    Vbbs

    2 2 11

    - lnln

    There are =1 independent e%uations.

    Derivation of Stolper Samuelson Elasticities:

    3a"es can be e*pressed as:

    k

    k

    k V

    Gs

    w =

    The tolper amuelson elasticities can be e*pressed as#

    k

    i

    i

    k

    i

    kki

    w

    p

    p

    w

    p

    we

    =

    =

    ln

    ln

    i

    k

    kk

    i

    pGs

    Vwp

    +

    =

    i

    k

    i

    k

    k

    i

    p

    sG

    p

    Gs

    Gs

    p

    0rom e%uation .. we ha!e ( )GsVw kkk =

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    i

    k

    k

    i

    i

    iki

    p

    s

    s

    p

    p

    G

    G

    pe

    +

    =

    i

    ii

    i

    ki sp

    G

    p

    G

    G

    pe =

    =

    =ln

    ln

    ++

    =

    = =

    M

    l

    M

    i

    iik

    i

    klok

    ii

    k

    p

    pc

    V

    Vbb

    pp

    s

    2 2 1

    1 lnln

    ;ifferentiatin" e%uation with respect to ip

    k

    ik

    i

    ik

    k

    i

    i

    k

    k

    i

    s

    c

    p

    c

    s

    p

    p

    s

    s

    p==

    ubstitutin" e%uation and in we "et

    k

    ik

    ikis

    cse +=

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