We answered only on one question about corpuscles. Но
внимательный читатель, вероятно, уже спрашивает- изменилось ли
уравнение Эйнштейна для фотоэффекта и как теперь обойтись без
произведения
hv?
Эти и другие вопросы мы осветим здесь. Напоминаю, что
But
the
attentive reader may
have
already asked
whether
the Einstein
equation for the photoelectric effect was changed, and
how
we do now without
the
product of
hv?
These and
other questions we
shall
discuss here. I recall that
How is it happens?
Pressure wave
amplitude
P of the
light source covers the
structure
of free electrons
by a
broad front. Therefore,
each cell
of free
electrons ( let
it be
a conditional
cube with
sides z)
is
subject to the action
of the
waves
as
pressure
increment to the existing pressure .
The resulting
pressure
in the
cells increases
K times
If
you
are
familiar with the source
[3],
the
previous material, you know
that
(J*m)
.
Therefore,
with
increasing energy of free
electrons
by the K times
their
radius decreases by the same factor .
Accordingly, the
period
T0 is
reduced also , that is
-
frequency
v growing proportional showing
the
change in energy. Now
Einstein's
formula for the photoelectric effect
will
be almost correct.
Why
"almost"? Bbecause
now, finally, the meaning
of the
index (max) is defined.
Remember, after all, the corpuscular
interpretation
of the photoelectric effect
bypassed
in silence
this
fact.
That's
because the corpuscles
had to
have the same energy
and
the
energy spread is impossible.
In Figure 3
of the
preceding article we see
a sine
wave, "modulated by light
energy."
We can
therefore use the mean
value of
energy, omitting the index
Этим мы не только максимумы
учитываем, а охватываем весь спектр энергий электронов, выбитых из
фотокатода. Настало время не
только издеваться над эйнштейновским попаданием в "глаз" электронам
фотокатода, но и объяснить процесс и физику выбивания. Действительно,
корпускула может и промахнуться в электрон, а выбивание по факту строго
функциональное. Чтобы понять, как это происходит, напомню, что
свободные электроны есть везде, а не только в металлах или воздухе. В
общем случае, их плотность
пропорциональна объемной плотности среды. Зная их объемную плотность
для воздуха м, можно приближенно вычислить величину
zk
в фотокатоде. Так, например,
для цезия, имеющего объемную плотность 1873 (
кг/м.
куб)
In
this way we not only
take into
account the peaks,
but
cover the
entire energy spectrum
of
electrons ejected from the
photocathode.
It's time
to not
only
mock
Einstein
hit to the
"eye" of
the
photocathode electrons,
but also to explain the process
and the
physics of ejection.
Indeed,
the corpuscle
may miss the
electron
and knocking
on the
fact is strictly
functional.
To
understand how this happens,
I remind you that free electrons
are
everywhere,
not only in metals
or
air.
In
general, their
density
is proportional to the volume density of
the
medium. Knowing the
bulk
density of
the air
m,
we can approximately calculate the value of
zk
in
the
photocathode.
For
example, for cesium,
which has a bulk density of
1873 (kg
/ cubic meter)
m.
Consequently,
between
two free electrons
of air
could be
placed 11.3
electrons
of the
cathode (in vacuum
more).
On the
site "The
Real physics" one cn aquaint
with the
optical effects stipulated by
the
structure of free electrons
(including
the coefficient of refraction of
the
medium).
Fig.1. Confrontation of free electrons of space and photocathode.
Рисунок 1 иллюстрирует это
противостояние, а также прием энергии поверхностными электронами
фотокатода. Видно, что они получают приращение давления, которое
относительно глубинных слоев является избыточным. Вот оно-то и
выдавливает поверхностные электроны из фотокатода (Рис.2). Именно
выдавливает - слово более подходящее.
Figure
1
illustrates this opposition, as well as
receiving
energy
by
surface electrons of photocathode.
One can
see that they get
the
pressure increment, which is relative
to deep
layers is redundant.
It pushes
the
electrons from the photocathode
surface
(Fig. 2).
Just "pushes"
-
the most
appropriate word for
this process.
Fig.2. The illustration of pushing the electrons from the body of
photocathode.
A
fragment of the picture
at right
shows the initial
pressure
distribution in metals.
The
electrons in the periphery
are not
balanced in the interactions
with the
atoms, so
there
cn be
seen a energy surface BOWL.
It
determines
the work function
of
electrons from the photocathode.
The
reader can easily
verify
that all the signs of
the
photoelectric effect observed,
there are
no violations of classical physics, and
there
were not involved hypothesis to the analysis.
Thus,
portionality
of the
light inspired the
creation
of false theories,
it isn't
created by a light source,
but by
spatial
free-electrons.
The light
source can generate
both
constant level
of
pressure,
and
changing
over time.
That's why
we
see the
light of burning match
(where
would photons come from?)
and
an
intense magnetic field and
even
a heated
metal.
The
reason for it all is a simple rising
of energy
density.