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And one man in his time plays many parts, His acts being seven ages…

And one man in his time plays many parts, His acts being seven ages…. For his shrunk shank; and his big manly voice, Turning again toward childish treble, pipes And whistles in his sound. Last scene of all, That ends this strange eventful history, Is second childishness and mere oblivion,

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And one man in his time plays many parts, His acts being seven ages…

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  1. And one man in his time plays many parts, His acts being seven ages… For his shrunk shank; and his big manly voice, Turning again toward childish treble, pipes And whistles in his sound. Last scene of all, That ends this strange eventful history, Is second childishness and mere oblivion, Sans teeth, sans eyes, sans taste, san everything. Stochastic models of aging and mortality …The sixth age shifts Into the lean and slipper'd pantaloon, With spectacles on nose and pouch on side, His youthful hose, well saved, a world too wide A nonstochastic model of aging and mortality by W. Shakespeare and Titian

  2. What is aging? • J. M. Smith (1962): Aging processes are “those which render individuals more susceptible as they grow older to the various factors, intrinsic or extrinsic, which may cause death.” • P. T. Costa and R. R. McCrae (1995): “What happens to an organism over time.”

  3. “Force of mortality” (hazard rate) increases with age

  4. Increasing mortality as a proxy for aging • We can’t measure aging processes directly, particularly since we can’t define them. • Mortality rates are easy to measure. In most metazoans, mortality rates increase with age.

  5. Increasing mortality as a proxy for aging • We can’t measure aging processes directly, particularly since we can’t define them. • Mortality rates are easy to measure. In most metazoans, mortality rates increase with age. • This includes us.

  6. This is not a trivial observation! • Implicit in Roman annuity rates. • 17th C. annuity and life-insurance rates were generally age-independent. • Annuity as gamble: Who is the best bet? • Very old (for whom the increased hazard would be most clear) rare, uncertain age. • Extreme haphazardness of plagues, wars.

  7. Some questions about aging: • Why do creatures age?

  8. Some questions about aging: • Why do creatures age? Old (and recurrent) idea: Improper nutrition. • “Unto the woman he said, I will greatly multiply thy sorrow and thy conception; in sorrow thou shalt bring forth children; and thy desire shall be to thy husband…In the sweat of thy face shalt thou eat bread, till thou return unto the ground; for out of it wast thou taken: for dust thou art, and unto dust shalt thou return.”

  9. Some questions about aging: • Why do creatures age? THINGS FALL APART

  10. Some questions about aging: • Why do creatures age? Problems with this naïve answer • Repair. • Not universal.

  11. Aging not universal. • Negligible senescence: prokaryotes, bristlecone pine, tortoises, lobster • Gradual senescence: mammals, birds, fish, yeast • Rapid senescence: flies, bees (workers), nematodes

  12. Some questions about aging: • Why do creatures age? • Why does aging have the particular age-patterns that it does?

  13. Some questions about aging: • Why do creatures age? • Why does aging have the particular age-patterns that it does? • Why do different species have characteristic patterns of aging?

  14. Some questions about aging: • Why do creatures age? • Why does aging have the particular age-patterns that it does? • Why do different species have characteristic patterns of aging? • Why is aging so variable?

  15. Some questions about aging: • Why do creatures age? • Why does aging have the particular age-patterns that it does? • Why do different species have characteristic patterns of aging? • Why is aging so variable? • Why is aging so constant?

  16. The Gompertz-Makeham mortality law • Gompertz (1825): “we observe that in those tables the numbers of living in each yearly increase of age are from 25 to 45 nearly, in geometrical progression.” • Makeham (1867): “Theory of partial forces of mortality”. Diseases of lungs, heart, kidneys, stomach, liver, brain associated with “diminution of the vital power”.

  17. log hazard rate in Japan 1981-90

  18. log infectious disease hazard rate in Japan 1981-90

  19. log cancer hazard rate in Japan 1981-90

  20. log suicide hazard rate in Japan 1981-90

  21. log auto accident hazard rate in Japan 1981-90

  22. log breast cancer hazard rate in Japan 1981-90

  23. log homicide hazard rate in Japan 1981-90

  24. MRDT seems to be species-characteristic

  25. Mortality plateaus Female mortality at ages 80+ (Japan + 13 W. European countries (1980-92)

  26. Mediterranean fruit fly mortality

  27. Is this about biology? Lifetimes of electrical relays “Force of junking” for automobiles in various periods

  28. What is a Markov process? A stochastic process Xt (where t is time, usually taken to be the positive reals) such that if you know the process up to a given time t, the behavior after time t depends only on the state at time t. The process may be killed, either randomly (at a rate depending on the current position) or instantaneously when it hits a certain part of the state space.

  29. Lessons for young scientists from reviewing the Markov mortality model literature • It’s easy to get your work published if your model reproduces known phenomena…

  30. Lessons for young scientists from reviewing the Markov mortality model literature • It’s easy to get your work published if your model reproduces known phenomena… • … even if you put them in (decently concealed) with your assumptions…

  31. Lessons for young scientists from reviewing the Markov mortality model literature • It’s easy to get your work published if your model reproduces known phenomena… • … even if you put them in (decently concealed) with your assumptions… • … and even if the mathematics is wrong.

  32. “Challenge to homeostasis” (B. Strehler, A. Mildvan 1960) • “The rate of decrease of most physiologic functions of human beings is between 0.5 and 1.3 percent per year after age 30, and is fit as well by a straight line as by any other simple mathematical function”. • “Challenges” come at constant rate. • Death occurs when a challenge exceeds the organism’s “vital capacity”. • “Challenges” follow the Maxwell-Boltzmann distribution: Exponentially distributed.

  33. “Challenge to homeostasis” (B. Strehler, A. Mildvan 1960) • “Predicts” the Gompertz curve. • “Predicts” the “nonintuitive” fact that initial mortality and rate of aging are inversely related. • Problem: The exponential rate was built into the assumptions, for which there is no external basis.

  34. Extreme-value theory • J. D. Abernethy (J. Theor. Biol. 1979): Model organisms by independent “systems”, which all fais at the same random rate. “Death” is the time of the first failure. • Proves that such an organism could have exponentially increasing death rates. • Claims (in the nonmathematical introduction and conclusion) that this is the generic situation, which will arise whenever the hazard rates of the components are nondecreasing, which is untrue. (In fact, the individual components would also have to have exponential hazard rates.) • Still gets cited.

  35. Reliability theory • M. Witten (1985): large number (m) of critical components; death comes when all fail. • Components are independent. Fail with constant rate. • Derives hazard rate approximately m·exp(t).

  36. Reliability theory • M. Witten (1985): large number (m) of critical components; death comes when all fail. • Components are independent. Fail with constant rate. • Derives hazard rate approximately m·exp(t). • Unmentioned:  is negative, so the hazard rate decreasesexponentially

  37. More reliability theory: Gavrilov & Gavrilova (1990) • m critical organs, each with n redundant components. • Organ fails when all components fail. • Death comes when any organ fails. • Components fail independently with constant exponential rate. • Derive Weibull hazard rates (power law). • Want Gompertz hazard rates. • Declare that biological systems have most of their components nonfunctioning from the beginning: Number of functioning components in each organ is Poisson. • The exponential of the Poisson then provides the exponential hazard rates.

  38. Biological problems with G&G • Arbitrary. • Where are the missing components? • What are the missing components? • Theory seems to predict that nearly all organisms should be born dead, with Gompertz mortality only conditioned on the rare survivors.

  39. Small mathematical problem with G&G model:

  40. Big mathematical problem with G&G model: The computation is wrong.

  41. Hazard rate for the G & G series-parallel process with k=1 and ==1 (solid) or =2, =3 (dotted).

  42. H. Le Bras’s “cascading failures” model • Start at senescence state Xt=1. • Rate of jumps to next higher state is Xt. • Rate of dying is Xt. • Le Bras (1976) pointed out that when >>, the mortality rate is about et for small t. • True… but a little cheap. When >>, the system behaves like a deterministic system d Xt/dt= Xt. State is Xt et.

  43. H. Le Bras’s “cascading failures” model • In fact, as Gavrilov & Gavrilova pointed out (1990) the result is even better when you don’t assume >>. By this time, mortality plateaus had been recognized. The general hazard rate is (+)e(+)t(+e(+)t)-1, which is a nice logistic Gompertz curve, with plateau at +.

  44. H. Le Bras’s “cascading failures” model • But… the exponential is still in the assumptions. • Also, the assumptions are quite specific and arbitrary.

  45. Attempts to explain the Gompertz curve with Markov models have been successful only when: • The exponential increase was built into the assumptions in a fairly transparent way or • The computations were wrong.

  46. What about mortality plateaus? Suggested explanations: • Heterogeneity in the population: selection. (Analyzed in DS: “Estimating mortality rate doubling time doubling times”. Available as preprint.) • Individuals actually deteriorate more slowly at advanced ages.

  47. What about mortality plateaus? • J. Weitz and H. Fraser (PNAS 2001) did explicit computation for Brownian motion with constant downward drift, killed at 0. It shows “senescence” and “plateaus” -- hazard rates increase rapidly (though not exponentially) at first, but eventually converge to a finite nonzero constant.

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