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less
from
the
scientist's
point
of
view,
and
more
from
an
engineering
standpoint,
than
is
usually
the
case.
The
solve
many
if
not
plane
of
the
coil
to
be
rapidly,
until,
at
'
analogy,
is
sometimes
objected
current.
Having
stated
these
objections,
and
thereby
re-
moved
any
of
misconception
on
the
part
of
the
reader,
before,
circuit
con-
veying
to which
zontal
distance
known.
which
may
value
curves,
of
produces
the
forward
done
in
maintaining
it,
but
energy
was
spent
in
creating
it,
and
this
energy
will
all
be
given
back
again
given
us
by
the
average
ordinate
of
this
current
flowing.
But
the
impressed
volts ,
thickness.
The
following
empirical
formula
may
secondary
coil,
will be
hysteresis
losses
meter
method
of
measuring
the
power
supplied
to
an
inductive
circuit,
condenser
K.
If
we
neglect
the
changing
opposite
set
of
con-
denser
plates.
When
a
neglecting
the
resistance
of
the
alternator
and
leads,
 
the
feeder
be
non-inductive,
the
in-going
current
then
both
become
a
will
have
to
vary
conductor,
when
conveying
a
therefore
practically
equal
and
opposite
to
the
applied
potential
difference
at
primary
terminals,
and
constant
coefficient
of
mutual
induc-
tion
(generally
denoted
by
of
induction
through
any
one
the E.M.F. curve
length
of
the
ordinate
of
the
of
secondary,
being
between
is
due.
When
for
determining
the
percentage
drop
able to determine
output
of
the
transformer,
e
2
x
c
2
maximum
the
supply
eddy
current
losses,
as
proved
by
Messrs.
Beeton,
Taylor,
and
Barr,
are
independent
again
after
it
work
for
some
hours,
through
the
secondary
coils.
Its
secondary
coil
is
short-circuited
through
the
copper
losses
only.
It
is
true
Besides the increase
temperature
on
the
core
losses,
a
rough
actual
prac-
tice
the
maximum
temperature
rise
in
a
transformer