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On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research [email protected] [This is joint work with J. Doyle and D. Alderson (Caltech)]

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Page 1: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

On Internet Traffic Dynamics and Internet Topology I

High Variability Phenomena

Walter Willinger

AT&T Labs-Research

[email protected]

[This is joint work with J. Doyle and D. Alderson (Caltech)]

Page 2: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Topics Covered

Motivation A working definition Some illustrative examples Some simple constructions Some key mathematical results Resilience to ambiguity Heavy tails and statistics A word of caution

Page 3: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Motivation

Internet is full of “high variability”– Link bandwidth: Kbps – Gbps

– File sizes: a few bytes – Mega/Gigabytes

– Flows: a few packets – 100,000+ packets

– In/out-degree (Web graph): 1 – 100,000+

– Delay: Milliseconds – seconds and beyond

How to deal with “high variability”– High variability = large, but finite variance

– High variability = infinite variance

Page 4: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

A Working Definition

A distribution function F(x) or random variable X is called heavy-tailed if for some

where c>0 and finite F is also called a power law or scaling distribution The parameter is called the tail index 1< < 2, F has infinite variance, but finite mean 0 < < 1, the variance and mean of F are infinite “Mild” vs “wild” (Mandelbrot): 2 vs < 2

xcxxFxXP ,)(1][

Page 5: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Some Illustrative Examples

Some commonly-used plotting techniques– Probability density functions (pdf)– Cumulative distribution functions (CDF)– Complementary CDF (CCDF)

Different plots emphasize different features– Main body of the distribution vs. tail– Variability vs. concentration– Uni- vs. multi-modal

Page 6: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Probability density functions

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 50

0.5

1

1.5

x

f(x

)

Lognormal(0,1)Gamma(.53,3)Exponential(1.6)Weibull(.7,.9)Pareto(1,1.5)

Page 7: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Cumulative Distribution Function

0 2 4 6 8 10 12 14 16 18 200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

x

F(x

)

Lognormal(0,1)Gamma(.53,3)Exponential(1.6)Weibull(.7,.9)Pareto(1,1.5)

Page 8: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Complementary CDFs

10-1

100

101

102

10-4

10-3

10-2

10-1

100

log(x)

log

(1-F

(x))

Lognormal(0,1)Gamma(.53,3)Exponential(1.6)Weibull(.7,.9)ParetoII(1,1.5)ParetoI(0.1,1.5)

Page 9: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

20th Century’s 100 largest disasters worldwide

10-2

10-1

100

100

101

102

US Power outages (10M of customers)

Natural ($100B)

Technological ($10B)

Log(size)

Log(rank)

Most events are

small

But the large events are huge

Page 10: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Why “Heavy Tails” Matter …

Risk modeling (insurance) Load balancing (CPU, network) Job scheduling (Web server design) Combinatorial search (Restart methods) Complex systems studies (SOC vs. HOT) Towards a theory for the Internet …

Page 11: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Some First Properties

Heavy-tailed or “scaling” distribution– – Compare to exponential distribution:

Linearly increasing mean residual lifetime– – Compare to exponential distribution

xcwXPxXPwXxXP 1/|

cxxXxXE |

))(exp(| wxwXxXP

| constxXxXE

Page 12: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Some Simple Constructions

For U uniform in [0,1], set X=1/U– X is heavy-tailed with

For E (standard) exponential, set X=exp(E)– X is heavy-tailed with

The mixture of exponential distributions with parameter 1/having a (centered) Gamma(a,b) distribution is a Pareto distribution with a

The distribution of the time between consecutive visits of a symmetric random walk to zero is heavy-tailed with

Page 13: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Key Mathematical Properties of Scaling Distributions Invariant under aggregation

– Non-classical CLT and stable laws

(Essentially) invariant under maximization– Domain of attraction of Frechet distribution

(Essentially) invariant under mixture– Example: The largest disasters worldwide

Page 14: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Linear Aggregation: Classical Central Limit Theorem A well-known result

– X(1), X(2), … independent and identically distributed random variables with distribution function F (mean and variance 1)

– S(n) = X(1)+X(2)+…+X(n) n-th partial sum

More general formulations are possible Often-used argument for the ubiquity of the normal

distribution

nNnnnS as ),1,0(/))((

Page 15: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Linear Aggregation: Non-classical Central Limit Theorem A not so well-known result

– X(1), X(2), … independent and identically distributed with common distribution function F that is heavy-tailed with 1<<2

– S(n) = X(1)+X(2)+…+X(n) n-th partial sum

The limit distribution is heavy-tailed with index More general formulations are possible Rarely taught in most Stats/Probability courses!

nnnnS as law, stable /))((

Page 16: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Maximization:Maximum Domain of Attraction A not so well-known result (extreme-value theory)

– X(1), X(2), … independent and identically distributed with common distribution function F that is heavy-tailed with 1<<2

– M(n)=max(X(1), …, X(n)), n-th successive maxima

G is the Fréchet distribution G is heavy-tailed with index

nGnnM as ,/)(

)exp( x

Page 17: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Intuition for “Mild” vs. “Wild”

The case of “mild” distributions– “Evenness” – large values of S(n) occur as a

consequence of many of the X(i)’s being large– The contribution of each X(i), even of the

largest, is negligible compared to the sum The case of “wild” distributions

– “Concentration” – large values of S(n) or M(n) occur as a consequence of a single large X(i)

– The largest X(i) is dominant compared to S(n)

Page 18: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Weighted Mixture

A little known result– X(1), X(2), … independent and identically distributed

with common distribution function F that is heavy-tailed with 1<<2

– p(1), p(2), …, p(n) iid in [0,1] with p(1)+…p(n)=1

– W(n)=p(1)X(1)+…+p(n)X(n)

Invariant “distributions” are Condition on X(i) >a>0

xlargefor ,)( xcxnWP W cuuFW 1)(

Page 19: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

100

101

102

20th Century’s 100 largest disasters worldwide

US Power outages (10M of customers,1985-1997)

Natural ($100B)

Technological ($10B)

Slope = -1(=1)

10-2

10-1

100

Page 20: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

8/14/0310

0

101

102 US Power outages

(10M of customers, 1985-1997)

10-2

10-1

100

Slope = -1(=1)

A large event is not inconsistent with statistics.

Page 21: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Resilience to Ambiguity

Scaling distributions are robust under– … aggregation, maximization, and mixture– … differences in observing/reporting/accounting– … varying environments, time periods

The “value” of robustness– Discoveries are easier/faster– Properties can be established more accurately– Findings are not sensitive to the details of the data

gathering process

Page 22: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

On the Ubiquity of Heavy Tails

Heavy-tailed distributions are attractors for averaging (e.g., non-classical CLT), but are the only distributions that are also (essentially) invariant under maximizing and mixing.

Gaussians (“normal”) distributions are also attractors for averaging (e.g., classical CLT), but are not invariant under maximizing and mixing

This makes heavy tails more ubiquitous than Gaussians, so no “special” explanations should be required …

Page 23: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Heavy Tails and Statistics

The traditional “curve-fitting” approach “Curve-fitting” by example Beyond “curve-fitting” – “Borrowing strength” “Borrowing strength” by example What “science” in “scientific modeling”? Additional considerations

Page 24: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

“Curve-fitting” approach

Model selection– Choose parametric family of distributions

Parameter estimation– Take a strictly static view of data– Assume moment estimates exist/converge

Model validation– Select “best-fitting” model– Rely on some “goodness-of-fit” criteria/metrics

“Black box-type” modeling, “data-fitting” exercise

Page 25: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

“Curve-fitting” by example

Randomly picked data set– LBL’s WAN traffic (in- and outbound)– 1:30, June 24 – 1:30, June 25 (PDT), 1996– 243,092 HTTP connection sizes (bytes)– Courtesy of Vern Paxson (thanks!)

Illustration of widely-accepted approach

Page 26: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

CCDF plot on log-log scale

0 1 2 3 4 5 6 7 8-6

-5

-4

-3

-2

-1

0HTTP Connections (Sizes)

log10(x)

log1

0(1-

F(x)

)

Page 27: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitted 2-parameter Lognormal distribution (=6.75,=2.05)

0 1 2 3 4 5 6 7 8-6

-5

-4

-3

-2

-1

0HTTP Connections (Sizes)

log10(x)

log1

0(1-

F(x)

)

Page 28: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitted 2-parameter Pareto distribution

(=1.27, m=2000)

0 1 2 3 4 5 6 7 8-6

-5

-4

-3

-2

-1

0HTTP Connections (Sizes)

log10(x)

log1

0(1-

F(x)

)

Page 29: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

The “truth” about “curve-fitting”

Highly predictable outcome– Always doable, no surprises

• Cause for endless discussions (“Which model is better?”)

When “more” means “better” …– 2-parameter distributions (Pareto, Lognormal, …)

• 3-parameter distributions (Weibull, Gamma, …)– 5-parameter distribution (Double-Pareto, -Lognormal, …), etc.

Inadequate “goodness-of-fit” criteria due to– Voluminous data sets

• Data with strong dependencies (LRD)– Data with high variability (heavy tails)

» Data with non-stationary features

Page 30: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

“Borrowing strength” approach

Mandelbrot & Tukey to the rescue– Sequential moment plots (Mandelbrot)

– Borrowing strength from large data (Tukey)

“Borrowing strength” – dynamic view of data– Rely on traditional approach for initial (small) subset of

available data

– Consider successively larger subsets

– Look out for inherently consistent models

– Identify “patchwork “ of “fixes”

Page 31: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Lognormal?

0 1 2 3 4 5 6 7 8-6

-5

-4

-3

-2

-1

0HTTP Connections (Sizes)

log10(x)

log1

0(1-

F(x)

)

Page 32: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Pareto?

0 1 2 3 4 5 6 7 8-6

-5

-4

-3

-2

-1

0HTTP Connections (Sizes)

log10(x)

log1

0(1-

F(x)

)

Page 33: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

“Borrowing strength” (example 1)

Use same data set as before Illustration of Mandelbrot-Tukey approach (1)

– Sequential standard deviation plots– Lack of robustness– A case against Lognormal distributions

More on sequential standard deviation plots Scaling distributions to the rescue

Page 34: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting lognormal: n=20,000

0 20000 2400005.5

6

6.5

7

7.5

8

8.5

9

9.5

10

10.5

11x 10

4 Sequential Standard Deviation (std) Plot

n

sd

t(n

)

std = 93626 (2LN

4.8)

Page 35: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting lognormal: n=40,000

0 40000 2400005.5

6

6.5

7

7.5

8

8.5

9

9.5

10

10.5

11x 10

4 Sequential Standard Deviation (std) Plot

n

sd

t(n

)

std(20000) = 93626 (2LN

4.8)

std = 72744 (2LN

4.5)

Page 36: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting lognormal: n=80,000

0 80000 2400005.5

6

6.5

7

7.5

8

8.5

9

9.5

10

10.5

11x 10

4 Sequential Standard Deviation (std) Plot

n

sd

t(n

)

std = 66322 (2LN

4.4)

std(20000) = 93626 (2LN

4.8)

std(40000) = 72744 (2LN

4.5)

Page 37: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting lognormal: n=160,000

0 160000 2400005.5

6

6.5

7

7.5

8

8.5

9

9.5

10

10.5

11x 10

4 Sequential Standard Deviation (std) Plot

n

sd

t(n

)

std = 61883(2

LN 4.3)

std(20000) = 93626 (2LN

4.8)

std(40000) = 72744 (2LN

4.5)

std(80000) = 66322 (2LN

4.4)

Page 38: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting lognormal: All data

0 2400005.5

6

6.5

7

7.5

8

8.5

9

9.5

10

10.5

11x 10

4 Sequential Standard Deviation (std) Plot

n

sd

t(n

)

std(20000) = 93626 (2LN

4.8)

std(40000) = 72744 (2LN

4.5)

std(80000) = 66322 (2LN

4.4)

std(160000) = 61883 (2LN

4.3)

std(all data) = 57569 (2LN

4.2)

Page 39: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

The case against lognormal

The lognormal model assumes– existence/convergence of 2nd moment– parameter estimates are inherently consistent

However, sequential std plot indicates– non-existence/divergence of 2nd moment – inherently inconsistent parameter estimates

What “science” in “scientific modeling”?– Curve/data fitting is not “science”– “Patchwork” of “fixes” (Mandelbrot)

Page 40: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Randomizing observations

0 0.5 1 1.5 2

x 105

4

4.5

5

5.5

6

6.5

7

7.5

8x 10

4 Sequential std Plots

n

std

(n)

original datarandom permutation of original data

Page 41: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Matching “mild” distributions

0 0.5 1 1.5 2

x 105

4.5

5

5.5

6

6.5

7

7.5

8

8.5x 10

4 Sequential std Plots

n

std

(n)

original datasample from matching"mild" (normal) distribution

Page 42: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Lognormal or scaling distribution

0 0.5 1 1.5 2

x 105

0

2

4

6

8

10

12

x 104 Sequential std Plots

n

std

(n)

original dataLognormal samplePareto sample

Page 43: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Pareto?

0 1 2 3 4 5 6 7 8-6

-5

-4

-3

-2

-1

0HTTP Connections (Sizes)

log10(x)

log1

0(1-

F(x)

)

Page 44: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

“Borrowing strength” (example 2)

Use same data set as before Illustration of Mandelbrot-Tukey approach (2)

– Sequential tail index plots

– Strong robustness properties

– A case for scaling distributions

A requirement for future empirical studies

Page 45: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting Pareto: n=20,000

0 20000 2400000.8

0.9

1

1.1

1.2

1.3

1.4

1.5

1.6

1.7

1.8Sequential Tail Index ((n)) Plot

n

(n

)

1.22

Page 46: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting Pareto: n=40,000

0 40000 2400000.8

0.9

1

1.1

1.2

1.3

1.4

1.5

1.6

1.7

1.8Sequential Tail Index ((n)) Plot

n

(n

)

1.26

(20000) 1.22

Page 47: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting Pareto: n=80,000

0 80000 2400000.8

0.9

1

1.1

1.2

1.3

1.4

1.5

1.6

1.7

1.8Sequential Tail Index ((n)) Plot

n

(n

)

1.26

(20000) 1.22

(40000) 1.26

Page 48: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting Pareto: n=160,000

0 160000 2400000.8

0.9

1

1.1

1.2

1.3

1.4

1.5

1.6

1.7

1.8Sequential Tail Index ((n)) Plot

n

(n

) 1.32

(20000) 1.22

(40000) 1.26

(80000) 1.26

Page 49: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Fitting Pareto: All data

0 2400000.8

0.9

1

1.1

1.2

1.3

1.4

1.5

1.6

1.7

1.8Sequential Tail Index ((n)) Plot

n

(n

)

(20000) 1.22

(40000) 1.26

(80000) 1.26

(160000) 1.32

(all data) 1.30

Page 50: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

The case for scaling distributions

The “creativity” of scaling distributions– Data: Divergent sequential moment plots

– Mathematics: Allow for infinite moments

Re-discover the “science” in “scientific modeling”– Scientifically “economical” modeling (when more data

doesn’t mean more parameters)

– Statistically “efficient” modeling (when more data mean more model accuracy/confidence)

– Trading “goodness-of-fit” for “robustness”

Page 51: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Looking ahead …

Main objective of current empirical studies “The observations are consistent (in the sense of “curve

fitting”) with model/distribution X, but are not consistent with model/distribution Y.”

Requirement for future empirical studies “The observations are consistent (in the sense of

“borrowing strength”) with model/distribution X, and X is not sensitive to the methods of measuring and collecting the observations.”

Page 52: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

Some Words of Caution …

Not every “straight-looking” log-log plot means “heavy tails”!

Never use frequency plots to infer heavy tails – even though physicists do it all the time!

Page 53: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

100

101

102

103

10-2

10-1

100

x

1-F

(x)

Straight-looking log-log plot?

Page 54: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

0 20 40 60 80 100 120 140 160 18010

-2

10-1

100

x

1-F

(x)

No! 25 samples from Exp(50) – linear semi-log plot!

Page 55: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

=1

=0

-1 0 1 2 3 4

-1

-2

-3

-4

log10(x)

log10(p)

dx

dPxp )(

Slope = -(+1)

NEVER infer from frequency plots on log-log scale!

Page 56: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

-1 0 1 2 3 4

-1

-2

-3

-4

log10(x)

log10(p)

dx

dPxp )(

2)10(

10

x

Page 57: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

=1

=0

-1 0 1 2 3 4 5

0

-1

-2

-3

-4

log10(x)

log10(P)

)( xXP

ALWAYS infer from CCDF plots on log-log scale!

Page 58: On Internet Traffic Dynamics and Internet Topology I High Variability Phenomena Walter Willinger AT&T Labs-Research walter@research.att.com [This is joint

A Word of Wisdom …

In my view, even if an accumulation of quick “fixes”were to yield an adequately fitting “patchwork”, it would bring no understanding. – B.B. Mandelbrot, 1997