History of the Orie 00 Whit Rich

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Contents. xi
Contents. xiii
municated
the
sun,
the
transparent
matter
of
interplanetary
space,
and
the
dense,
opaque
in the
10 The
14 The
in the
lumiere
is
concerned
with
a
phenomenon
on the
38 Electric
of
his
work,
that
at
any
point
in
the
interior
of
any
one
of
the
conductors,
the
resultant
force
ideas
have
persisted,
and
among
them
the
conviction
which
lies
at
its
foundation,
that
90 Galvanism
ponderomotive
force
on
a
current-element
ds'
in
a
magnetic
the
terminals
electroscope
is
repelled
or
attracted
by
the
body
is
determined.
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
the
surfaces
of
bodies,
and
inflect
such
rays
as
pass
close
by.
If
this
France.
visit
from
Arago,
who
of
a
proof
of
the
correctness
of
of
dispersion.
The Aether
waves
as
this,
travelling
in
all
directions,
superposed
on
each
other
A
particular
solution
of
the
equations
for
The Aether
as an
stress
is
continuous.
The Aether
rarefied
than
in
The Aether
most
of
the
light
scattered
The Aether
as an
Stokes-Kankine-
Rayleigh
hypothesis
of
aelotropic
inertia.
For
according
to
pure
imaginary,
is
generally
known
The Aether
derived
from
the
in
showing
that
every
known
effect
of
process
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
idea which
conclusion
that
admiration
and
delight;
and
future
generations
will
preserve
only
one
of
its
kind;
an
alterna-
tive
to
it
was
suggested
by
Bernhard
Eiemann
(b.
1826,
d.
1866),
in
a
course
of
lectures
equation
of
the
moon's
motion,
Laplace
found
that
the
velocity
of
the
gravific
fluid
must
i
(1852),
p.
483;
a
frictional
resistance
262 The
quantity
conveyed
past
a
specified
point
in
a
unit
of
time,
when
the
direction
of
(1870),
p.
optical
and
magnetic
phenomena.
The
theory
thus
outlined
was
apparently
not
developed
further
by
its
author
270 Maxwell.
magnetic
274 Maxwell.
its
return
journey.
The
velocity
of
light
was
calculated
from
the
dimensions
and
angular
velocity
of
the
the
286 Maxwell.
in
dielectrics
always
has
this
value,
so
that
in
the
general
equations
the
writers have
preparing
his
Eoyal
Society
memoir
on
the
electromagnetic
field;
but
he
was
not
able
at
Maxwell. 301
Maxwell. 303
rings
are
moved,
the
invariants
in
the
hydrodynamical
system
being
If
sneh
a
fluid,
of
strengths
m
and
0*i*ae*i*+^ld^&m^Mmt1to+k&lm*at1i*>
small
spheres
to
modify
Ohm's
law
S
member
vanish,
since
the
^-average
of
any
derivate
dQ/dx
vanishes
if
Q
reflexion
takes
place;
the
optical
no
poles,
can
exert
no
ponderomotive
The Followers
starting-
point
make
the
free
period
of
electric
oscillations
in
it
nearly
equal
to
the
period
of
the
oscillations
in
the
primary
circuit
light.
distance
from
the
radiator,
and
the
remoter
portion
of
each
of
these
lines
thus
takes
the
form
of
a
loop
362 The
The Followers
from Faraday
from Faraday
from Faraday
impoverished
that
the
double
layer
can
no
longer
be
formed.
The
impoverishment
of
the
382 Conduction
384 Conduction
in
unit
volume
could
double
420 The
of
(pv
r
428 The
expression
e
hypothesis
of
a
436 The
was
shown*
a
few
years
after
the
publication
of
direction
of
the
motion:
magnetic
energy
the
small
quantity
w/c.
In
this
form
we
shall
now
consider
it.
The
fundamental
equations
of
444 The
446 The
454 The
456 The
path
464 The
472 Index.

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