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Published byCornelius Warren Modified over 9 years ago
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Something “feels the same” regardless of scale 4 What is that???
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Something “feels the same” regardless of scale 5 Self-similar in nature
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Something “feels the same” regardless of scale 6 The Koch snowflake fractal
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Something “feels the same” regardless of scale 7 The Koch snowflake fractal
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Something “feels the same” regardless of scale 8 The Koch snowflake fractal
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Something “feels the same” regardless of scale 9
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10 Categories: Exact self-similarity: Strongest Type Approximate self-similarity: Loose Form Statistical self-similarity: Weakest Type
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11 Approximate self-similarity: Recognisably similar but not exactly so. e.g. Mandelbrot set Statistical self-similarity: Only numerical or statistical measures that are preserved across scales
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In case of Stochastic Objects e.g. time-series Self-similarity is used in the distributional sense 12
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Recently, network packet traffic has been identified as being self-similar. Current network traffic modeling using Poisson distributing (etc.) does not take into account the self-similar nature of traffic. This leads to inaccurate modeling of network traffic. 13
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A Poisson process When observed on a fine time scale will appear bursty When aggregated on a coarse time scale will flatten (smooth) to white noise A Self-Similar (fractal) process When aggregated over wide range of time scales will maintain its bursty characteristic 14
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15 packets per time unit Ethernet traffic August’89 trace
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19 Bursty Data Streams Aggregation Smooth Pattern Streams Bursty Data Streams Aggregation Bursty Aggregate Streams Reality (self-similar): Current Model: Consequence: Inaccuracy
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Long-range Dependence autocorrelation decays slowly Hurst Parameter Developed by Harold Hurst (1965) H is a measure of “burstiness” ▪ also considered a measure of self-similarity 0 < H < 1 H increases as traffic increases ▪ i.e., traffic becomes more self-similar 20
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X = (X t : t = 0, 1, 2, ….) is covariance stationary random process (i.e. Cov(X t,X t+k ) does not depend on t for all k) Let X (m) ={X k (m) } denote the new process obtained by averaging the original series X in non-overlapping sub-blocks of size m. Mean , variance 2 Suppose that Autocorrelation Function r(k) k -β, 0<β<1 21 e.g. X(1)= 4,12,34,2,-6,18,21,35 Then X(2)=8,18,6,28 X(4)=13,17
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X is exactly second-order self-similar if The aggregated processes have the same autocorrelation structure as X. i.e. r (m) (k) = r(k), k 0 for all m =1,2, … X is asymptotically second-order self-similar if the above holds when [ r (m) (k) r(k), m Most striking feature of self-similarity: Correlation structures of the aggregated process do not degenerate as m 22
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23 lag ACF
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Correlation structures of their aggregated processes degenerate as m i.e. r (m) (k) 0 as m for k = 1,2,3,... Short Range Dependence Processes: Exponential Decay of autocorrelations i.e. r(k) ~ p k, as k , 0 < p < 1 Summation is finite 25
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Processes with Long Range Dependence are characterized by an autocorrelation function that decays hyperbolically as k increases Important Property: This is also called non-summability of correlation 26
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The intuition behind long-range dependence: While high-lag correlations are all individually small, their cumulative affect is important Gives rise to features drastically different from conventional short-range dependent processes 27
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Hurst Parameter H, 0.5 < H < 1 Three approaches to estimate H (Based on properties of self-similar processes) Variance Analysis of aggregated processes Rescaled Range (R/S) Analysis for different block sizes: time domain analysis Periodogram Analysis: frequency domain analysis (Whittle Estimator) 28
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Variance of aggregated processes decays as: Var(X (m) ) = am -b as m infinite, For short range dependent processes (e.g. Poisson Process): Var(X (m) ) = am -1 as m infinite, Plot Var(X (m) ) against m on a log-log plot Slope > -1 indicative of self-similarity 29
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30 Slope=-1 Slope=-0.7
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31 where For a given set of observations, Rescaled Adjusted Range or R/S statistic is given by
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X k = 14,1,3,5,10,3 Mean = 36/6 = 6 W 1 =14-(1*6 )=8 W 2 =15-(2*6 )=3 W 3 =18-(3*6 )=0 W 4 =23-(4*6 )=-1 W 5 =33-(5*6 )=3 W 6 =36-(6*6 )=0 32 R/S = 1/S*[8-(-1)] = 9/S
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For self-similar data, rescaled range or R/S statistic grows according to cn H H = Hurst Paramater, > 0.5 For short-range processes, R/S statistic ~ dn 0.5 History: The Nile river In the 1940-50’s, Harold Edwin Hurst studied the 800-year record of flooding along the Nile river. (yearly minimum water level) Finds long-range dependence. 33
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34 Slope = 1.0 Slope = 0.5 Slope = 0.79
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Provides a confidence interval Property: Any long range dependent process approaches fractional Gaussian noise (FGN), when aggregated to a certain level Test the aggregated observations to ensure that it has converged to the normal distribution 35
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Self-similarity manifests itself in several equivalent fashions: Non-degenerate autocorrelations Slowly decaying variance Long range dependence Hurst effect 36
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Leland and Wilson collected hundreds of millions of Ethernet packets without loss and with recorded time-stamps accurate to within 100µs. Data collected from several Ethernet LAN’s at the Bellcore Morristown Research and Engineering Center at different times over the course of approximately 4 years. 38
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40 H=0.5 H=1 Estimate H 0.8
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41 Higher Traffic, Higher H High Traffic Mid Traffic Low Traffic 1.3%-10.4% 3.4%-18.4% 5.0%-30.7% Packets
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Observation shows “contrary to Poisson” Network UtilizationH 42 As number of Ethernet users increases, the resulting aggregate traffic becomes burstier instead of smoother
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Pre-1990: host-to-host workgroup traffic Post-1990: Router-to-router traffic Low period router-to-router traffic consists mostly of machine-generated packets Tend to form a smoother arrival stream, than low period host-to-host traffic 43
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Ethernet LAN traffic is statistically self-similar H : the degree of self-similarity H : a function of utilization H : a measure of “burstiness” Models like Poisson are not able to capture self-similarity 44
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The superposition of many ON/OFF sources whose ON-periods and OFF-periods exhibit the Noah Effect produces aggregate network traffic that features the Joseph Effect. 47 Also known as packet train models Noah Effect: high variability or infinite variance Joseph Effect: Self-similar or long-range dependent traffic
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Traditional traffic models: finite variance ON/OFF source models Superposition of such sources behaves like white noise, with only short range correlations 48
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Questions related to self-similarity can be reduced to practical implications of Noah Effect Queuing and Network performance Network Congestion Controls Protocol Analysis 49
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The Queue Length distribution Traditional (Markovian) traffic: decreases exponentially fast Self-similar traffic: decreases much more slowly Not accounting for Joseph Effect can lead to overly optimistic performance 50 Effect of H (Burstiness)
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How to design the buffer size? Trade-off between Packet Lose and Packet Delay 51
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52 Packet LosePacket Delay Short Range DependenceDecrease ExponentiallyFixed Limit Long Range DependenceDecrease SlowlyAlways Increase Compare SRD and LRD when increase buffer size
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Protocol design should take into account knowledge about network traffic such as the presence or absence of the self-similarity. 53 Parsimonious Models Small number of parameters Every parameter has a physically meaningful interpretation e.g. Mean , Variance 2, H Doesn’t quantify the effects of various factors in traffic
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Demonstrated the existence of self-similarity in Ethernet Traffic irrespective of time scales Proposed the degree of self-similarity can be measured by Hurst parameter H (higher H implies burstier traffic) Illustrated the difference between the self-similar and standard models Explained Importance of self similarity in design, control, performance analysis 54
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55 http://ita.ee.lbl.gov/html/contrib/BC.html
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