DOC.
380
APRIL
1912 283
The initial
posits
Z
=
F(T,
p)
.i1V
Z'
=
G(T,
p)
.
ri2ri3V
(2)
(3)
next
generalize
your
initial
posits
for
the
widest
possible
range.
(1)
(2) (3)
combined
yield
Nz
F(T,
P)
= e
RTs
G(T,
p)a
(4)
or:
1
kTs
1
(F(T,
p))
Ģ
lg
{a(T)
.
G(T,p)
}
(5)
on
the other
hand,
the
displacement
law
{-J
p
=
yv3f
}
yields:
kTS
1
kTs,
=
hv
U(P
\
yv3
)
(6)
To
be
sure, according
to
(
0
^
(7a)
W.
Wien:
D
hv3)
=
-
lg
p
yv
3
;
(7b)
Planck: Q
r
^
\
P
\
hv3
=
lg
p
+
yv3
3\
y
(7c)
Rayleigh-Jeans:
q
P
\
hv3
/
yv
~P
P
)
From
(5)
and
(6)
it follows
that
lg{
(F(T, p))
a(T)G(T,p)
} =
-
e
P
O
\
hv
yV3
(8)