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Productivity for Infonomos

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Preparation of the basic mathematical and statistical concepts ... Acknowledged by Christian Kerckhoffs and Huub Meijers. For 'free' Dates: Monday 22nd 16-18 ... – PowerPoint PPT presentation

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Title: Productivity for Infonomos


1
Productivity for Infonomos
  • Presented for the IES-Network by
  • Heiko Lampe

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Overview
  • Just for Infonomos, not part of the official
    program
  • Two sessions with unknown length
  • Preparation of the basic mathematical and
    statistical concepts for Productivity
  • Some repetition of old QM1 and QM2 stuff, many
    might have forgotten by now
  • Acknowledged by Christian Kerckhoffs and Huub
    Meijers
  • For free
  • Dates
  • Monday 22nd 16-18
  • Wednesday 24th 13.30 ???

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3
Disclaimer
  • All the explanations are meant as a supportive
    act. I try to be as correct as possible, but
    obviously mistakes can happen. I do not take any
    responsibilities for these mistakes. I cannot
    possibly teach you everything of 4 weeks QM3
    within 2 sessions! Nevertheless, I try my best.

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Agenda Meeting 1/1
  • Easy stuff (math)
  • - Derivatives and Leibniz (differential)
    notation
  • - ln rules
  • - Taylor approximation (1st order)
  • - Elasticities and Eulers Theorem (Homogeneity)
  • - Growth formula
  • - Implicit differentiation

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Agenda Meeting 1/2
  • Easy stuff (stats) Mostly intuition
  • Unbiasedness of the OLS Estimator
  • Omitted Variable Bias
  • F-Test
  • Indirect t-test (teta-trick)
  • Harder stuff 1 and 2 (QM3)
  • Discrete Dynamics and difference equations
  • Continuous Dynamics and differential equations
  • Easy stuff (QM3)
  • Phase Diagrams and Equilibria

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Agenda Meeting 2
  • All the stuff we did not make in the first
    meeting
  • Lecture 1 for productivity from Kerkhoffs

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Easy stuff (math) 1/4
  • Rules for derivatives
  • Power rule
  • Product rule
  • Quotient rule
  • Chain rule (important)
  • Leibniz (differential) notation

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Easy stuff (math) 2/4
  • Ln rules
  • General rule
  • Multiplication
  • Division
  • Taylor approximation (first order)
  • f(x0) about a f(a) f (a) (x0- a)

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Easy stuff (math) 3/4
  • Elasticities
  • The El. of a multiplication is equal to the sum
    of the partial El.
  • General
  • Degree of homogeneity (k) from Eulers Theorem
    and alternative way (t-trick)

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Easy stuff (math) 4/4
  • Growth formula
  • A K (1g)t
  • Time to double t ln2/ln (1g)
  • Implicit Differentiation
  • Regard y as a function of x
  • yx2 y2 x3
  • f(x)x2 (f(x))2 x3 gt now derive
  • f (x)x2 f(x)2x 2(f(x))f (x) 3x2
  • yx2 y2x 2yy 3x2

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Easy stuff (stats) - Intuition 1/4
  • OLS Estimators
  • Based on a sample, estimators for the coefficient
    of the population are calculated.
  • Unbiasedness of the OLS Estimator
  • Needs to be established to properly use these
    estimators on average we hit the true value
  • 4 Assumptions SLR 1 4
  • SLR1 Linear in parameters
  • SLR2 Random sampling
  • SLR3 Sample Variation (not all the same)
  • SLR4 Zero Conditional Mean error unrelated to x

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Easy stuff (stats) - Intuition 2/4
  • Omitted Variable Bias
  • The bias in a model caused by omitting a variable
    with an effect. Example (thx. to Tobi)
  • Take a random sample of 2 people
  • They differ in basic ability, approximated by IQ
  • Examine the relation of years of education to
    wage

IQ140
wage
IQ90
educ
10
13
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Easy stuff (stats) - Intuition 3/4
  • F-test
  • Used to test, whether a bunch (or all) of the
    coefficients are unimportant (ß0 ß1 ß2 0) or
    alternatively, to compare models.
  • For the second purpose, one needs a restricted
    and one unrestricted model.
  • The higher the F-score, the better for the
    validity of the model overall and also in favor
    of the unrestricted model.
  • Distribution is non-quadratic and uses df
  • Table in Bowerman

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Easy stuff (stats) - Intuition 4/4
  • Indirect t-test (Teta-trick)
  • Test for linear restriction
  • Y ß0 ß1x1 ß2x2
  • Define ? ß1 ß2
  • Solve for ß1 and plug in
  • Y ß0 (? - ß2)x1 ß2x2
  • Shuffle and run regression
  • Y ß0 ?x1 ß2(x2-x1)
  • The t-score of the ?-coefficient can be used to
    evaluate joint significance

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Harder stuff 1 (QM3) 1/15
  • Discrete Dynamics and Difference Equations
  • General Idea Find a function that allows us to
    calculate the value of a series that changes over
    time at a specific point in time, where the
    periods of time are discrete
  • ?K is the basis for this function!!
  • e.g. Value of a depot after t years with g
    interest
  • Growth formula relation

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Harder stuff 1 (QM3) 2/15
  • General Notation
  • Index-notation Kt, Kt-1
  • Domain N 0,1,2,3, ...
  • Kt Kt-11.05 Kt-2 (starts getting useful
    after the second period)
  • Easy to do in Excel
  • However, the example equation does not provide an
    answer to the question posted earlier!

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Harder stuff 1 (QM3) 3/15
  • Assume a depot is growing with 5 each year. How
    much money do you get after t years, if you put
    in 1000 once?
  • Kt 1000 (1.05)t gt growth formula
  • Assume that you put in 1000 each year ... ?
  • Kt Kt-1 (1.05) 1000
  • That is the rule, lets try to solve it

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Harder stuff 1 (QM3) 4/15
  • Classification
  • Autonomous system (t does not occur as a factor,
    just as an index)
  • Order of a system the highest time lag
  • e.g. Kt Kt-1 1.05 Kt-3 is 3rd order
  • Homogeneous system Discrete, 1st order,
    Autonomous

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Harder stuff 1 (QM3) 5/15
  • Coming back
  • Kt Kt-1 (1.05) 1000
  • This is not easy to solve, due to the 1000,
    thus we ignore them for the moment, searching for
    the solution of the homogeneous equation first.
  • This is, as we know, Kt K0 (1.05)t, with K0
    being the initial amount saved
  • The solution of homogeneous equations always
    works like this!

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Harder stuff 1 (QM3) 6/15
  • Lets try the inhomogeneous equation (IHE)
  • Kt Kt-1 (1.05) 1000
  • Solution to the homogeneous equation
  • Kt K0 (1.05)t
  • For the IHE, we need a different starting point,
    so we choose c and add a particular solution
    (pt)
  • Kt c (1.05)t pt
  • The c will be determined from a given K0, but
    first we need to find a pt

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Harder stuff 1 (QM3) 7/15
  • Remember the original equation
  • Kt Kt-1 (1.05) 1000
  • The pt will always be similar to the stuff that
    makes the equation inhomogeneous ... so a
    constant in this case. Lets choose d
  • Furthermore, remember it is a solution, so it can
    be plugged in for Kt. Since a constant does not
    vary in time, Kt Kt-1 d
  • d d (1.05) 1000

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Harder stuff 1 (QM3) 8/15
  • Solving for d gives us 20.000 as pt
  • Kt c (1.05)t pt
  • Kt c (1.05)t 20.000
  • Remarks
  • If I had K0, I could plug in t 0 and calculate
    c!
  • pt can be a constant, a linear or quadratic
    equation with t as a variable, but is always
    similar to the part that makes the equation
    inhomogeneous

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Harder stuff 1 (QM3) 9/15
  • Lets reconsider
  • We wanted to solve an IHE
  • Solved homogeneous system first (easy)
  • Exchanged K0 with c and added a pt
  • Choose a pt, similar to the thing that makes the
    homogeneous equation inhomogeneous (here d)
  • Calculate pt, have complete solution (with K0
    even unique one)
  • gt 1st order linear Difference Equation

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Harder stuff 1 (QM3) 10/15
  • Example 2
  • Kt 0.25 Kt-1 150 with K0 100
  • Solution to the homogeneous Equation
  • Kt K0 (0.25)t
  • Substitute c and add pt
  • Kt c (0.25)t pt
  • pt like a constant, choose d for original
  • d 0.25 d 150
  • Solve for d and plug in
  • d 200 gt Kt c (0.25)t 200
  • Use K0
  • 100 c (0.25)0 200 gt c 100
  • Kt 100 (0.25)t 200

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Harder stuff 1 (QM3) 11/15
  • Example 3
  • Kt 1.5 Kt-1 10t 5
  • Solution to the homogeneous equation
  • Kt K0 (1.5)t
  • Substitude c and add pt
  • Kt c (1.5)t pt
  • pt is like a linear equation, say at b
  • at b 1.5 (a ( t-1) b) 10t 5
  • at b (1.5a 10)t 5 1.5a 1.5b
  • a 1.5a 10 and b 5 1.5a 1.5b
  • a 20 , b 70
  • Kt c (1.5)t 20t 70
  • No K0 given

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Harder stuff 1 (QM3) 12/15
  • Sidestep for equilibria
  • An equilibrium point is a constant x, which will
    fulfill the original equation
  • Kt Kt-1 (1.05) 1000
  • Hence in this case x x (1.05) 1000, which
    turned out to be 20000
  • An equilibrium is stable, if the difference
    equation moves towards this point, given any
    initial K0
  • Kt c (1.05)t 20.000 gt not stable
  • Kt c (0.05)t 20.000 gt -20.000

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Harder stuff 1 (QM3) 13/15
  • 2nd order linear Difference Equations
  • xt cxt-1 dxt-2
  • Solving via Characteristic Equation
  • ?2 c? d
  • Solve for ? via pq-formula or ABC
  • If you get two ?, the solution is
  • xt k1?1t k2?2t
  • If you get one ?, the solution is
  • xt k1?t k2t?t
  • If x0 and x1 are given, one can easiliy
  • calculate k1 and k2

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Harder stuff 1 (QM3) 14/15
  • If the original equation is an IHE
  • xt cxt-1 dxt-2 bt
  • Solve the homogeneous equation as usual
  • Search for pt choose something similar to bt,
    plug it into the original equation for xt,
    xt-1,and xt-2
  • The complete solution (second order linear
    difference equation) is the solution for the
    homogeneous equation pt (or further calculated
    with the help of x0 and x1)

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Harder stuff 1 (QM3) 15/15
  • From the Syllabus for Discrete Dynamics
  • 1.3 a), b) equilibria
  • 1.7 a), b), c)
  • 1.9 a), c)
  • 1.12

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Harder stuff 2 (QM3) 1/7
  • Continuous Dynamics and Differential Equations
  • Similar to discrete dynamics, but now t is
    continuous.
  • Again the basis of our analysis will be the
    change in K or x over time, denoted as and

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Harder stuff 2 (QM3) 2/7
  • Lets try to solve this
  • axt
  • This means we are searching for a function xt,
    which is itself multiplied by a after deriving
    it.
  • The e-function comes to mind
  • If xt Aeat, then aAeat axt
  • Remember, that is a derivative w.r.t. t!!

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Harder stuff 2 (QM3) 3/7
  • Two more general rules for first order (linear)
    difference equations
  • axt b gt xt Ae-at
  • axt bxt2 gt xt
  • Plus the third, which you already have seen
  • axt gt xt Aeat
  • Of course, knowing xo, will allow you to
    calculate A, since t 0 and provide a unique
    solution

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Harder stuff 2 (QM3) 4/7
  • What you just have seen was a solution for a
    homogeneous equation.
  • For IHE, the way to solve is the same as with
    discrete dynamics
  • Solve the homogeneous equation
  • Add a pt (related to the stuff that causes the
    IHE)
  • Choose a pt, plug it into the original and solve
    it
  • With a given x0 you can deduce the A for a unique
    solution

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Harder stuff 2 (QM3) 5/7
  • First order and second order differential
    equations can be distinguished as in the case of
    difference equations
  • First order xt axt-1, axt
  • Second order xt axt-1 axt-2, a bxt

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Harder stuff 2 (QM3) 6/7
  • Trying to solve 2nd order differential equation
  • This is very similar to difference equations
  • Take the differential equation and make the
    characteristic equation
  • a bxt gt ?2 a ? b
  • Solve this for ? by pq or ABC
  • With 2 ? xt Ae ?1t Be?2t
  • With 1 ? xt Ae ?t Bte ?t
  • A and B can be uniquely determined using an x0
    and x1

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Harder stuff 2 (QM3) 7/7
  • For IHE, the way of solving is again the same
    with solving the homogeneous equation, adding a
    pt, solving this with the usual trial and error
    approach and later on work on finding A and B.

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Easier stuff QM3 Equilibria 1/6
  • Lets refresh the equilibria for difference
    equations
  • An equilibrium point is a constant x, which will
    fulfill the original equation
  • It is stable, if no matter what x0 is you end up
    in this x if t? 8
  • For differential equations, the rules are the
    same
  • Remember that x is a constant, thus 0

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Easier stuff QM3 Equilibria 2/6
  • Consider (x-1)(x-3)
  • The resulting equilibria are x 1 and x 3
  • Graphically, this can be shown like this

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Easier stuff QM3 Equilibria 3/6
  • Conergences
  • And 1-dimensional

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Easier stuff QM3 Equilibria 4/6
  • For phase diagrams, just remember
  • Draw the graph of 0. The areas where the
    value of that function are gt 0, go right, else go
    left
  • If two arrows meet in an equilibrium, it is
    stable, otherwise it is not

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Easier stuff QM3 Equilibria 5/6
  • This also works for systems of differential
    equations with and , where both equations
    have to equal zero in order to have an
    equilibrium.
  • Set the equations each equal to zero and draw
    them sequentially, each time drwaing your arrows.
    For right (gt0) and left (lt0) and for up (gt0)
    or down (lt0)
  • Spiralling moves towards an intersection of your
    graphs will give you stable equilibria

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Easier stuff QM3 Equilibria 6/6
  • Lets draw together
  • x 1 and xy 2
  • x 2y and x y

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Lecture 1
  • by C. Kerkhoffs

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Announcement
  • Thank you for your attention and please
  • Come to our GMA tonight at 19.00 in A0.28

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