Transcript of History of the Orie 00 Whit Rich
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Contents. xi
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Contents. xiii
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municated
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the
sun,
the
transparent
matter
of
interplanetary
space,
and
the
dense,
opaque
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in the
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10 The
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14 The
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in the
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lumiere
is
concerned
with
a
phenomenon
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on the
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38 Electric
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of
his
work,
that
at
any
point
in
the
interior
of
any
one
of
the
conductors,
the
resultant
force
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ideas
have
persisted,
and
among
them
the
conviction
which
lies
at
its
foundation,
that
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90 Galvanism
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ponderomotive
force
on
a
current-element
ds'
in
a
magnetic
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the
terminals
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electroscope
is
repelled
or
attracted
by
the
body
is
determined.
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determined
from
the
eclipses
of
Jupiter's
satellites. *
With
the
exception
of
Bradley's
discovery,
which
was
primarily
astronomical
rather
than
optical,
the
eighteenth
century
was
decidedly
barren,
as
regards
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the
surfaces
of
bodies,
and
inflect
such
rays
as
pass
close
by.
If
this
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France.
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visit
from
Arago,
who
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of
a
proof
of
the
correctness
of
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of
dispersion.
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The Aether
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waves
as
this,
travelling
in
all
directions,
superposed
on
each
other
A
particular
solution
of
the
equations
for
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The Aether
as an
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stress
is
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continuous.
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The Aether
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rarefied
than
in
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The Aether
most
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of
the
light
scattered
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The Aether
as an
Stokes-Kankine-
Rayleigh
hypothesis
of
aelotropic
inertia.
For
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according
to
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pure
imaginary,
is
generally
known
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The Aether
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derived
from
the
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in
showing
that
every
known
effect
of
process
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electricity
it
sets
in
motion,
is
never
expended,
and
continues
to
be
exerted
with
undi-
minished
power,
in
the
production
of
a
never-ceasing
effect.
Against
the
truth
of
such
a
supposition
the
probabilities
are
all
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idea which
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conclusion
that
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admiration
and
delight;
and
future
generations
will
preserve
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only
one
of
its
kind;
an
alterna-
tive
to
it
was
suggested
by
Bernhard
Eiemann
(b.
1826,
d.
1866),
in
a
course
of
lectures
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equation
of
the
moon's
motion,
Laplace
found
that
the
velocity
of
the
gravific
fluid
must
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i
(1852),
p.
483;
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a
frictional
resistance
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262 The
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quantity
conveyed
past
a
specified
point
in
a
unit
of
time,
when
the
direction
of
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(1870),
p.
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optical
and
magnetic
phenomena.
The
theory
thus
outlined
was
apparently
not
developed
further
by
its
author
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270 Maxwell.
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magnetic
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274 Maxwell.
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its
return
journey.
The
velocity
of
light
was
calculated
from
the
dimensions
and
angular
velocity
of
the
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the
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286 Maxwell.
in
dielectrics
always
has
this
value,
so
that
in
the
general
equations
the
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writers have
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preparing
his
Eoyal
Society
memoir
on
the
electromagnetic
field;
but
he
was
not
able
at
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Maxwell. 301
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Maxwell. 303
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rings
are
moved,
the
invariants
in
the
hydrodynamical
system
being
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If
sneh
a
fluid,
of
strengths
m
and
0*i*ae*i*+^ld^&m^Mmt1to+k&lm*at1i*>
small
spheres
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to
modify
Ohm's
law
S
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member
vanish,
since
the
^-average
of
any
derivate
dQ/dx
vanishes
if
Q
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reflexion
takes
place;
the
optical
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no
poles,
can
exert
no
ponderomotive
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The Followers
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starting-
point
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make
the
free
period
of
electric
oscillations
in
it
nearly
equal
to
the
period
of
the
oscillations
in
the
primary
circuit
light.
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distance
from
the
radiator,
and
the
remoter
portion
of
each
of
these
lines
thus
takes
the
form
of
a
loop
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362 The
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The Followers
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from Faraday
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from Faraday
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from Faraday
impoverished
that
the
double
layer
can
no
longer
be
formed.
The
impoverishment
of
the
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382 Conduction
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384 Conduction
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in
unit
volume
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could
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double
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420 The
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of
(pv
r
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428 The
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expression
e
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direction
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the
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444 The
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472 Index.
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