1993 Invited entry for McGraw Hill Scientific
Encyclopedia 8th Edition 1997
(deleted and replaced)
Biological clocks:
On the 25-hour circular horizontal axis, New York night-time phases are
on the frontside: * tan(reset subjective phase when exposure
ends) = sin(subjective phase when exposure starts),
with the measure of exposure size tailored
to light intensity and duration and color for each species.
For very long dim exposures (which constitute
the only data for humans thus far) the whole diagram may
turn out to be twisted somewhat along the vertical
axis.
To shift phase to a new time zone means shifting
from the contour line
Living organisms of almost all kinds show fluctuations of leaf movement,
of cell division, of
stomatal opening and closing, of alertness, of cell division, of serum composition,
and so on.
These are called circadian ('roughly daily') rhythms. In the absence of
environmental cues (in
'temporal isolation') these activities repeat at intervals close to 24 hours
(different in
different species and in mutants of a given species) with hardly any change
of period at different
temperatures. In an outdoor environment the interval is adjusted daily through
a sensitivity to
visible light, with the result that rhythms keeps pace with the day/night
cycle. In no instance
has the underlying mechanism --- the 'biological clock' --- yet been deciphered.
There may be
multiple mechanisms: diverse organs and tissues often have distinct autonomous
rhythms but
they mutually synchronize or one tissue dominates. In some insects the left
and right optic lobes
of the brain dominate; in others, cells of the 'pars intercerebralis'. Transferring
brains
between individuals whose clocks were removed or set to different time zones
transfers the
behavioral phase setting. In birds of different species the pineal gland
and/or the
suprachiasmatic nuclei (SCN) of the brain's hypothalamus dominate. In mammals
the SCN
dominates. In primates including man, internal circadian rhythms originate
both from the
brain's two SCN, patches of about 50,000 cells of several types in a 1/4
mm3 volume. The SCN
mechanism is photosensitive through the eyes, specifically through nerve
fibers from ganglion
cells in the retina which enter the SCN near the optic chiasm. Neural activity
in the SCN has
natural period about 25 hours; at each peak it suppresses the pineal gland's
secretion of a
hormone called melatonin, which regulates sleep. Another indicator of body
clock phase is core
body temperature, which waxes and wanes within a range of one degree C (to
which additional
variations are added if the subject exercises, eats ice cream, etc., but
without effect on the
timing and amplitude of the underlying clock.) Other physiological rhythms
driven by 'clock'
tissues include plasma cortisol concentration and (less directly) the tide
of sleepiness and of
waking.
See Nervous System (Invertebrate); Nervous System (Vertebrate).
Though the physiological mechanism of circadian clocks remains to be deciphered,
something of apparently universal scope is now known about how it works.
This experimentally
proven principle is strangely un"clock"like, but it has direct
applications, even to control of
human jet lag by sunlight. If any stimulus (e.g., an hour of sunlight) fleetingly
disturbs any
cycling mechanism in a way that resets its phase, then its new phase will
depend on the size of the
stimulus and on the initial phase of the clock. The dependance reveals something
about the
underlying mechanism. A smooth biochemical oscillator, for example, typically
resets to a new
phase that varies smoothly with the initial phase, and with the amount of
some chemical added in
a resetting pulse in the pattern represented qualitatively in the accompanying
figure and formula.
The figure is a contour map: at any combination of initial phase (on the
cylinder's circular axis)
and stimulus size (on its downward long axis) you read the resulting new
phase by following a
nearby contour line back to the circular phase axis. Contours are sampled
only at 4-hour
intervals to minimize clutter. You might think of the cylinder as being
colored: red along one
contour, orange along the next, yellow, green, blue, violet, and red again.
The colors grade
smoothly between contours. Each phase of the clock is thus coded by hue
and you read the new,
reset phase by the cylinder's hue at any stimulus timing and size. The conspicuous
feature of this
pattern is its 'singularity' where all contours converge at a unique combination
of stimulus size
(1) and initial phase (0). This combination resets the phase ambiguously:
hues merge to hueless
white. No such pattern could possibly result from perturbing the speed of
a clock which executes
a fixed cycle of changes at rates that depend on time of day and exposure
to resetting cues... as in
some postulated mechanisms of circadian clocks. This discriminating test
was applied to a
representative sampling of circadian clocks, resetting them by a variable
dose of visible light or
of some metabolically active drug applied at various times in the cycle:
a clock governing the
timing of metamorphosis in fruitflies, one revealed in the timing of mosquito
flight and feeding
activity, one controlling the nocturnal bioluminescence of 'red tide' organisms
in sea water, one
revealed in the diurnal opening and closing of a flower. In every case the
results are nicely
summarized by a diagram resembling this figure. Following the singular pulse,
flies hatch at
random times, mosquitoes become insomniacs, seawater ceases ever to glow,
and the flower
thereafter stays closed.
The familiar discomfort of 'jet lag' stems from some combination of (a)'the'
clock remaining set to
your home time zone while activities are required on a different schedule,
and (b) possible loss of
synchrony among body rhythms while each adjusts toward the new time zone
at its own rate (even
in opposite directions, one advancing 9 hours, another delaying 15 hours,
for example.)
Adjustment to a shifted time zone typically takes several days during which
phase advances
and/or delays accumulate during each exposure to sunlight brightness, especially
if such
exposures are badly timed. The measured phase reset depends on timing and
magnitude of each
exposure, as in the Figure:
.
Caption: --------------------------
sunset is on the left, sunrise on the right, and zero represents a phase
in the wee hours of a
typical day/night cycle. Choose a phase of a travelling New Yorker's biological
clock when she
will take sunlight, e.g., A: when it is evening at home. Descend to B at
the magnitude of intended
sunlight exposure (in arbitrary units here, as a generic figure typifying
diverse animal and
plant species). Follow the contour line through B back up to the circular
phase scale and read
the new phase to which her clock will thus be instantly reset: C, a quarter-cycle
delay back to a
phase typical of mid-afternoon, optimal for places 6 time zones westward.
Were A on the right
side of 0 (before sunrise at home), the effect would be an advance, larger
for more light. Were
A during daytime at home, the phase change would be slight (contours near
vertical on backside
of cylinder). The dotted phase scale above the cylinder compares the 6-hour
earlier phase of
airport personnel in Hawaii with that of fresh arrivals from New York (the
shaded scale atop
the cylinder). New Yorkers need a quarter-cycle delay and can get it at
A during New York's
evening = Hawaiian mid-afternoon, resetting to C = the mid-afternoon phase
of people adjusted
to the local local light/dark cycle. Notice the origin of all contours at
the singular phase in the
wee hours (early evening in Hawaii for a traveller from New York) when a
unit dose can reset
the clock to any new phase, depending delicately on the exact timing and
dose. Any smaller dose
leaves the clock near the same new phase contour as a zero dose; any larger
dose sets it near the
opposite phase. Exposures near the singularity extinguish the clock's amplitude.
From
amplitude 0 any later exposure restarts the rhythm at a phase opposite to
0, viz. appropriate to
early afternoon; so it should be taken at that local time. This is the pattern
for all circadian
clocks probed to date with strong stimuli. Its quantitative expression was
first derived from
non-linear dynamics a quarter-century ago in the form:
(exposure size + cos(subjective phase when exposure starts))
------------------------------ end figure caption
you start at, to another that passes through a different phase on
the cycle. Given adequate
exposures, phase shifts are greatest (you change contour origin
most dramatically) for
stimuli beginning just before and just after the singular phase marked 0
in the figure, somewhat
after midnight. "Adequate" exposure means "below the singularity
on the Figure"; for humans this
requires eyes exposed to outdoor brightness for at least an hour. For simplicity,
suppose your
exposure suffices to take you to the bottom of the cylinder. You want to
pick an initial phase at
which a move to the bottom of the cylinder puts you on the hue contour of
some earler phase (for
eastward trips crossing up to 12 time-zones) or some later phase (for similar
westward
trips). This means starting your exposure when your brain's clock, still
on home time, is some
hours before or after singular phase 0: closer for larger shifts in either
direction. Phase 0 is
about 2 AM at home: leave your wristwatch on home time until after you take
your body-clock-
resetting exposure. In terms of local time at your destination, you can
work out from the
formula in the caption that to reset to any time zone (where local time
is that far advanced
relative to home) you would expose in the local morning for small advances
(eastward),
approaching local mid-day for almost 12 time zones, moving through noon
to early afternoon for
more than 12 (less than 12 westward), through late local afternoon for delays
(westward) of 6
hours or so, then back through noon to local morning for the shortest westward
trips. Do
everything a few hours later if your personal habits of sunlight exposure
timing make you a
'night owl' in your home time zone, with singular phase "0" for
onset of sunlight a few hours
later than normal, or a few hours earlier if you are an habitual 'early
bird'.
The timing of travel or of sleep has little or no influence on the resetting
of your biological
clock, though fatigue will of course result from missing too much sleep,
as on long north-south
flights with little time zone change. Dietary factors have not been shown
to play an important
role in man.
A feature in which circadian 'clocks' differ fundamentally from all technological
clocks
is that not only their phase, but also their amplitude or range of physiological
variation
is reset by stimuli. The amplitude is minimized by a light exposure closer
to the phase
singularity (initial phase =0, dose =1 in the figure). Resetting the human
clock to lower
amplitude has three effects: 1) the spontaneous rhythm of core body temperature
is
attenuated or disappears; 2) the clock becomes more sensitive to resetting
by subsequent
slight exposure to light; 3) subsequent exposures, regardless when given,
restart the
clock at normal amplitude near the phase opposite to 0, corresponding to
local early
afternoon. The resettability of amplitude in circadian rhythms might reflect
an aspect of
the dynamics of the clock mechanism, or might only reflect scattering of
phase among the
many cells that make up a clock tissue like the SCN. This could be resolved
by direct
observation after the singular stimulus. If cells remain synchronous, but
with
individually negligible amplitude (range of daily variation), then the clock
mechanism
can be deciphered by exposing such tissue to each of many biochemical agents,
e.g., cAMP
or various neurotransmitters: all those affecting the mechanism through
the same
channel must restart the attenuated cellular rhythm at the same phase, thus
enumerating and classifying the chemical parts of the cellular mechanism.
Cellular and physiological clocks affect responsiveness to stress. Survivorship
varies markedly
in animals exposed to a variety of stresses, e.g. chemotherapeutic drugs,
at diverse phases of the
biological clock. Implications for medical practice remain to be exploited.
Bibliography:
Annual Review of Physiology 54, 657-753, Special Topic: Circadian Rhythms
(1993).
Circadian Clocks and Their Adjustment, CIBA Foundation Symposium 183 (1994).
C.A. Czeisler, R.E. Kronauer, J.S. Allan, J.F. Duffy, M.E. Jewett, E.N.
Brown, and J.M. Ronda,
Science 244, 1328-1333 (1989).
M.E. Jewett, R.E. Kronauer, and C.A. Czeisler, Nature 350, 59-62 and 18,
and 351,193 (1991).
J.D. Miller, American Journal of Physiology 264, R821-R832 (1993).
M.C. Moore-Ede, F.M. Sulzman, and C.A.Fuller,The Clocks That Time Us, Harvard
Univ Press (1982).
N. Mrosovsky and P.A. Salmon, Nature 330, 372-373 and 311-312 (1987).
A.T. Winfree, The Timing of Biological Clocks, Scientific American Library
(1986).