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Viterbi School of Engineering
The Impact of Information The Impact of Information on Supply Chain on Supply Chain
OscillationsOscillations
Ken Dozier & David ChangKen Dozier & David ChangWestern Research Application CenterWestern Research Application Center
IRMA International , IncIRMA International , Inc
Washington D.C.Washington D.C.May 23, 2006May 23, 2006
USC Viterbi School of Engineering
BioBio
USC Viterbi School of Engineering
A System of Forces in A System of Forces in OrganizationOrganization
Efficiency
Direction
Proficiency
Competition
Concentrat\ion Innovation
Cooperation
Source: “The Effective Organization: Forces and Form”,Sloan Management Review, Henry Mintzberg, McGill University 1991
USC Viterbi School of Engineering
Make & Sell vs Sense & Make & Sell vs Sense & RespondRespond
Chart Source:“Corporate Information Systems and Management”, Applegate, 2000
USC Viterbi School of Engineering
Theoretical EnvironmentTheoretical Environment
Seven Organizational Change Propositions Framework, “Framing the Domains of IT Management” Zmud 2002
Business Process Improvement
Business Process Redesign
Business Model Refinement
Business Model Redefinition
Supply-chain Discovery
Supply-chain Expansion
Market Redefinition
USC Viterbi School of Engineering
Supply Chain (Firm)Supply Chain (Firm)
Source: Gus Koehler, University of Southern California Department of Policy and Planning, 2002
USC Viterbi School of Engineering
Supply Chain (Government)Supply Chain (Government)
Source: Gus Koehler, University of Southern California Department of Policy and Planning, 2002
USC Viterbi School of Engineering
Supply Chain (Framework)Supply Chain (Framework)
Source: Gus Koehler, University of Southern California Department of Policy and Planning, 2002
USC Viterbi School of Engineering
Supply Chain (Interactions)Supply Chain (Interactions)
Source: Gus Koehler, University of Southern California Department of Policy and Planning, 2002
USC Viterbi School of Engineering
Why statistical physics?Why statistical physics?
► Proven formalism for “seeing the forest past the Proven formalism for “seeing the forest past the trees”trees” Well established in physical and chemical sciencesWell established in physical and chemical sciences Our recent verification with data in economic realmOur recent verification with data in economic realm
► Simple procedure for focusing on macro-parametersSimple procedure for focusing on macro-parameters Most likely distributions obtained by maximizing the Most likely distributions obtained by maximizing the
number of micro-states corresponding to a measurable number of micro-states corresponding to a measurable macro-statemacro-state
Straightforward extension from original focus on energy Straightforward extension from original focus on energy to economic quantitiesto economic quantities
► Unit cost of productionUnit cost of production► ProductivityProductivity► R&D costsR&D costs
Self-consistency check provided by distribution functionsSelf-consistency check provided by distribution functions
USC Viterbi School of Engineering
Plasma theories Plasma theories
► Advanced Advanced plasmaplasma theories are extremely important theories are extremely important when one tries to explain, for example, the various when one tries to explain, for example, the various waveswaves and and instabilitiesinstabilities found in the plasma found in the plasma environment. Since plasma consist of a very large environment. Since plasma consist of a very large number of interacting particles, in order to provide number of interacting particles, in order to provide a macroscopic description of plasma phenomena it a macroscopic description of plasma phenomena it is appropriate to adopt a is appropriate to adopt a statisticalstatistical approach. This approach. This leads to a great reduction in the amount of leads to a great reduction in the amount of information to be handled. In the information to be handled. In the kinetic theorykinetic theory it it is necessary to know only the is necessary to know only the distribution distribution functionfunction for the system of particles. for the system of particles.
Source: University of Oulu, FInland
USC Viterbi School of Engineering
Applications of statistical physics to economicsApplications of statistical physics to economics
► Quasistatic phenomenaQuasistatic phenomena
Approach: Constrained maximization of Approach: Constrained maximization of microstates corresponding to a macrostatemicrostates corresponding to a macrostate
Applications to date: unit cost of production Applications to date: unit cost of production & productivity& productivity
► Time-dependent phenomenaTime-dependent phenomena
Approach: normal mode analysis Approach: normal mode analysis Current application: supply chain oscillationsCurrent application: supply chain oscillations
USC Viterbi School of Engineering
Comparison of Statistical Formalism in Physics and Economics
Variable Physics Economics
State (i) Hamiltonian eigenfunction Production site
Energy Hamiltonian eigenvalue Ei Unit prod. cost Ci
Occupation number Number in state Ni Output Ni = exp[-βCi+βF]
Partition function Z ∑exp[-(1/kBT)Ei] ∑exp[-βCi]
Free energy F kBT lnZ (1/β) lnZ
Generalized force fξ ∂F/∂ξ ∂F/∂ξ
Example Pressure TechnologyExample Electric field x charge Knowledge
Entropy (randomness) - ∂F / ∂T kBβ2∂F/∂
Quasi-staticQuasi-static
USC Viterbi School of Engineering
Comparison of U.S. economic census cumulative number of companies vs shipments/company (blue diamond points) in LACMSA in 1992 and the statistical physics cumulative distribution curve (square pink points) with β = 0.167 per $106
Quasi-staticQuasi-static
0
500
1000
1500
2000
2500
3000
3500
4000
0 10 20 30 40 50 60
USC Viterbi School of Engineering
Productivity: Ratio (‘97/’92) of the statistical parametersProductivity: Ratio (‘97/’92) of the statistical parameters
Company size: Company size: Large Large Intermediate Intermediate Small Small
IT rankIT rank 59 59 7070 81 81## 0.86 0.86 1.0 1.0 0.90 0.90E(1000s)E(1000s) 0.78 0.78 0.98 0.98 1.08 1.08#/company#/company 0.91 0.91 1.0 1.0 1.21 1.21Sh ($million)Sh ($million) 1.53 1.53 1.24 1.24 1.42 1.42Sh/E ($1000)Sh/E ($1000) 1.66 1.66 1.34 1.34 1.35 1.35 ββ 1.11 1.11 0.90 0.90 0.99 0.99
Findings:Findings:
Sectors with large companies spend a larger percentage on IT.Sectors with large companies spend a larger percentage on IT.Largest % increases in shipments are in large & small company sectors.Largest % increases in shipments are in large & small company sectors.Small companies increased in size while large companies decreased.Small companies increased in size while large companies decreased.Number of large and small companies decreased by 10%.Number of large and small companies decreased by 10%.Employment decreased 20% in large companies, but increased 8% in small Employment decreased 20% in large companies, but increased 8% in small
companies.companies.Largest productivity occurred in large companies.Largest productivity occurred in large companies.
USC Viterbi School of Engineering
Oscillations in Supply ChainsOscillations in Supply Chains
► ObservationsObservations Cyclic phenomena in economics ubiquitous & Cyclic phenomena in economics ubiquitous &
disruptivedisruptive Example: Wild oscillations In supply chain Example: Wild oscillations In supply chain
inventoriesinventories► MIT “beer game” simulationMIT “beer game” simulation
Supply chain of only 4 companies for beer Supply chain of only 4 companies for beer production, distribution, and salesproduction, distribution, and sales
► Results of observations and simulationsResults of observations and simulations Oscillations Oscillations Phase dependence of oscillations on position in Phase dependence of oscillations on position in
chainchain Spatial instabilitySpatial instability
USC Viterbi School of Engineering
IRMA 2006 ObjectivesIRMA 2006 Objectives
►To show with a simple product-flow To show with a simple product-flow model of a supply chain that universal model of a supply chain that universal information exchangeinformation exchange Changes the character of oscillations from Changes the character of oscillations from
those of nearest neighbor information those of nearest neighbor information exchangeexchange
Causes an increase in the damping of Causes an increase in the damping of oscillationsoscillations
USC Viterbi School of Engineering
Local Exchange of InformationLocal Exchange of Information
► Instead of designating each level in the chain by a discrete label nInstead of designating each level in the chain by a discrete label n the position in a chain was designated by a continuum variable x. the position in a chain was designated by a continuum variable x. Flow of production units through each position in the chain was Flow of production units through each position in the chain was
designated by a velocity variable v. designated by a velocity variable v.
► A differential distribution function f(x,v,t)dxdv denotes the number of A differential distribution function f(x,v,t)dxdv denotes the number of production units in the intervals dx and dv at x and v at time t. production units in the intervals dx and dv at x and v at time t.
► ∂ ∂f/ ∂t + ∂[fdx/dt]/ ∂x + ∂[fdv/dt]/ ∂v = 0f/ ∂t + ∂[fdx/dt]/ ∂x + ∂[fdv/dt]/ ∂v = 0 [1][1]► A thermodynamic force F that gives the rate at which v changes in A thermodynamic force F that gives the rate at which v changes in
time, this equation can be rewritten time, this equation can be rewritten ► ∂ ∂f/ ∂t + ∂[fv]/∂x +[∂fF]/ ∂v = 0f/ ∂t + ∂[fv]/∂x +[∂fF]/ ∂v = 0 [2][2]
USC Viterbi School of Engineering
Nearest neighbor information exchangeNearest neighbor information exchange
This becomes Vlasov-like equation for f(x,v,t)This becomes Vlasov-like equation for f(x,v,t)∂∂f/∂t + v∂f/∂x + F∂f/∂v = 0f/∂t + v∂f/∂x + F∂f/∂v = 0 [5] [5]
This is the equation for collisionless plasmasThis is the equation for collisionless plasmas
When the inventory of the level below the level of interest is less When the inventory of the level below the level of interest is less than normal, the production rate (v) will be diminished because than normal, the production rate (v) will be diminished because of the smaller number of production units being introduced to of the smaller number of production units being introduced to that level. At the same time, when the inventory of the level that level. At the same time, when the inventory of the level above the level of interest is larger than normal, the production above the level of interest is larger than normal, the production rate will also be diminished because the upper level will rate will also be diminished because the upper level will demand less input so that it can “catch up” in its production demand less input so that it can “catch up” in its production through-put. Both effects give production rate changes through-put. Both effects give production rate changes proportional to the gradient of n. It is resonable also that the proportional to the gradient of n. It is resonable also that the fractional changes are related rather than the changes fractional changes are related rather than the changes themselves, since deviations are always made from the themselves, since deviations are always made from the inventories at hand.inventories at hand.
∂∂f/∂t + v∂f/∂x - 2ξv2(1/n)(dn/dx) ∂f/∂v = 0f/∂t + v∂f/∂x - 2ξv2(1/n)(dn/dx) ∂f/∂v = 0 [13] [13]
USC Viterbi School of Engineering
Nearest neighbor dispersion relationNearest neighbor dispersion relation
Perturbed distributionPerturbed distribution
f(x,v,t) = ff(x,v,t) = f00(v) + f(v) + f11(v) exp[-i((v) exp[-i(t – kx)]t – kx)][15][15]-i(-i(-kv)f-kv)f11 - ik 2ξv2(1/n - ik 2ξv2(1/noo)n)n11∂f∂foo/∂v = 0 /∂v = 0 [16b][16b]ff11 = -2ξk(1/n = -2ξk(1/noo) ∫dv’f) ∫dv’f11(v’) v2∂f(v’) v2∂foo/∂v(/∂v(-kv)-kv)-1-1 [17][17]
This leads to the dispersion relation between This leads to the dispersion relation between and k and k
1+ 2ξk (1/n1+ 2ξk (1/noo) ∫dvv2∂f) ∫dvv2∂foo/∂v(/∂v(-kv)-kv)-1-1 =0 =0 [18][18]Principal and imaginary partsPrincipal and imaginary parts
∫∫dvv2∂fdvv2∂foo/∂v(/∂v(-kv)-kv)-1-1 = PP∫dvv2∂f = PP∫dvv2∂foo/∂v/∂v ((-kv)-kv)-1-1 - iπ( - iπ(/k)2(1/k)∂f/k)2(1/k)∂foo((/k) /∂v/k) /∂v [19][19]
USC Viterbi School of Engineering
Nearest neighbor dispersion relation (cont)Nearest neighbor dispersion relation (cont)
Solving for Solving for = 4ξkV= 4ξkVoo [1+ [1+
(1/n(1/n00)iπ(4ξV)iπ(4ξVoo )2∂f )2∂foo(4ξV(4ξVoo ) /∂v] ) /∂v] [23][23]
SignificanceSignificance
ff00(v) peaked around V(v) peaked around V00, ∂f, ∂f00(4ξV(4ξV00 ) / ∂v <0. ) / ∂v <0.
Oscillation resembles a sound-like waveOscillation resembles a sound-like wave
Oscillation exhibits small Landau damping that Oscillation exhibits small Landau damping that is because of distance of phase velocity from is because of distance of phase velocity from VVoo
USC Viterbi School of Engineering
Universal information exchangeUniversal information exchange
Introduce an Introduce an information exchange potential Φinformation exchange potential Φ
∂ ∂22Φ/∂xΦ/∂x22 = - [C/n = - [C/noo]∫dv f(x,v,t)]∫dv f(x,v,t) [24][24]
from which the thermodynamic force F is obtained from which the thermodynamic force F is obtained
F = - ∂Φ/∂xF = - ∂Φ/∂x [25][25]
This reduces to the former results for nearest This reduces to the former results for nearest neighbor interactions when we chooseneighbor interactions when we choose
C = ξVC = ξVoo22 / / ll22 [29] [29]
USC Viterbi School of Engineering
Universal information exchange dynamic Universal information exchange dynamic equationsequations
Introduction of potential into Vlasov equationIntroduction of potential into Vlasov equation
∂∂f/∂t + v∂f/∂x - ∂Φ/∂x ∂f/∂v = 0f/∂t + v∂f/∂x - ∂Φ/∂x ∂f/∂v = 0 [31][31]
Perturbation in distribution function caused by Perturbation in distribution function caused by ΦΦ
ff11 = -kΦ = -kΦ11∂f∂foo /∂v ( /∂v (-kv) -kv) -1-1 [33] [33]
Self-consistency conditionSelf-consistency condition
ΦΦ11 = (1/k = (1/k22) [ξV) [ξVoo22 /n /nooll22] ∫dv f] ∫dv f11(v)(v) [34] [34]
USC Viterbi School of Engineering
Dispersion relation for universal information Dispersion relation for universal information exchangeexchange
≈ ≈ kVkVoo + ξ + ξ1/21/2(V(Voo//ll) [1 + i {πξV) [1 + i {πξVoo22/(2k/(2k22ll22nnoo)}∂f)}∂foo/∂v ]/∂v ] [42][42]
where ∂fwhere ∂f00/∂v is evaluated at /∂v is evaluated at
v = v = /k ≈ V/k ≈ Vo o + (ξ+ (ξ1/21/2VVoo/k/kll)) [43][43]
SignificanceSignificance
Oscillations resemble plasma oscillationsOscillations resemble plasma oscillations
Oscillations always exhibit Landau damping. This Oscillations always exhibit Landau damping. This changes the form of the supply chain oscillation and in changes the form of the supply chain oscillation and in suppression of the resulting oscillationsuppression of the resulting oscillation
USC Viterbi School of Engineering
ConclusionsConclusions
► Supply chain oscillations can be described by a simple Supply chain oscillations can be described by a simple flow model of product through chainflow model of product through chain
► Flow model shows that Flow model shows that Character of oscillation changes from sound-like to Character of oscillation changes from sound-like to
plasma-like when information exchange becomes plasma-like when information exchange becomes universal rather than just between nearest universal rather than just between nearest neighborsneighbors
Damping of oscillation can be large when Damping of oscillation can be large when information exchange becomes universalinformation exchange becomes universal
Washington DC
USC Viterbi School of Engineering
Future WorkFuture Work
►Create a simulation that allows the study Create a simulation that allows the study of various IT architectures on the of various IT architectures on the optimization issues of supply chain optimization issues of supply chain managementmanagement
►[email protected]@usc.edu►Visit the Learning CenterVisit the Learning Center►http:wesrac.usc.eduhttp:wesrac.usc.edu►Google wesracGoogle wesrac►Google Ken DozierGoogle Ken Dozier