l
‘
.
‘
_
'
'—
162
_
'
G… H. PARKER
'
be slipped Over a glass plate more easily forward than backward,
_
just as an earthworm can‘ be drawn over an appropriate surface Î
'
'
more easily headward than tailward.
I must confess that i have
not been able to
myself that there is any difference
in this respect, in Helix pomatia or Limax maximus; both
î
to slip over the glass forWard and backward with equal :
_
,
case.
»
“
…
'
?
.
_
Moreover, the view advanced by von Uexküll is based upon
_
what I believe to be a somewhat erroneous conception of the pedal
_
wave.
Biedermann (’05, p. 11) pointed out that the foot of Helix
'
pomatia has great advantages over that of many other
p0ds for studies of this kind because of the numerous small specks '
:
,
contained in its outer layer. These specks can be discerned clearly
,
by means of a hand lens and they give a true picture of the move—
=
'
ments of the foot;
As watched through a plate of glass over which
,
=
_
the_animal is creeping, they can be seen, as Biedermann has de—
'scribed, to move momentar—ily forward, then come to rest, and then I
.
again-to move forward.
This is best demonstrated on a sheet of
_
_
'
.
glass on which there are numerous scratches. - Such scratches
serve as landmai*ks and— by them it canbe seen that the minute _
-
specks in the foot do remain essenti”ally xed in position and then;
momentarily move:
for a brief period a
'
position of rest, When
in relation to the“
_
foot-as a whole, it is ev1dentthatthef0rward motion
_
.
in the dark W&VGS andtha’oquïescencelscha1actensmc of the
—
=
"
intermediate ghterfporüonsezofthefeetEach Wave—them 1sa
.
'
pulse- Of -:forward' motion
rest@fthef@0t » _ Ï is momentauly
‘
quiesœnt- ;The area @@V6‘1ïedbythewaves1spmbablya fourth
“
«
01? & f‘fth _of
therefore
,;
f00t18
‘
.
‘
_
'
'—
162
_
'
G… H. PARKER
'
be slipped Over a glass plate more easily forward than backward,
_
just as an earthworm can‘ be drawn over an appropriate surface Î
'
'
more easily headward than tailward.
I must confess that i have
not been able to
myself that there is any difference
in this respect, in Helix pomatia or Limax maximus; both
î
to slip over the glass forWard and backward with equal :
_
,
case.
»
“
…
'
?
.
_
Moreover, the view advanced by von Uexküll is based upon
_
what I believe to be a somewhat erroneous conception of the pedal
_
wave.
Biedermann (’05, p. 11) pointed out that the foot of Helix
'
pomatia has great advantages over that of many other
p0ds for studies of this kind because of the numerous small specks '
:
,
contained in its outer layer. These specks can be discerned clearly
,
by means of a hand lens and they give a true picture of the move—
=
'
ments of the foot;
As watched through a plate of glass over which
,
=
_
the_animal is creeping, they can be seen, as Biedermann has de—
'scribed, to move momentar—ily forward, then come to rest, and then I
.
again-to move forward.
This is best demonstrated on a sheet of
_
_
'
.
glass on which there are numerous scratches. - Such scratches
serve as landmai*ks and— by them it canbe seen that the minute _
-
specks in the foot do remain essenti”ally xed in position and then;
momentarily move:
for a brief period a
'
position of rest, When
in relation to the“
_
foot-as a whole, it is ev1dentthatthef0rward motion
_
.
in the dark W&VGS andtha’oquïescencelscha1actensmc of the
—
=
"
intermediate ghterfporüonsezofthefeetEach Wave—them 1sa
.
'
pulse- Of -:forward' motion
rest@fthef@0t » _ Ï is momentauly
‘
quiesœnt- ;The area @@V6‘1ïedbythewaves1spmbablya fourth
“
«
01? & f‘fth _of
therefore
,;
f00t18
