, Chapter I : The atom in modern Chemistry
Thomson 's apparatus
From Thomson 's separatus ( right )
E- time between
L Fe = CE Mates
e)Me could be determined The FEM -
oever
§ µ
.
.
. ,
by En
'
Electron is bend off
Ifield
the Electric 5 over =
averts-vv.t-vv.IT
'
✓ t
over
=
'
=
backstraight
ver
and bound
with a
Magnetic field
Ë=ÊE¥
.
Saai
Seeslides Lecture I
Millikan 's oil drop experiment .
Mist Oil Particle s are inserted and go through
Of Oil
"" ""
→ ; :
a hole to a detector
g. wagen
•
→ • oa .
•
Treron Outcome : The charge | the drop let
÷
↳
is
always a multiple of
" Electrical
The
droppletsgetcharged
%
field
.
charge e- so D= me
/ → van
detector
The Nucleus Scanning tunnel inz microscoop .
distance
remains
eigual
Thomson 's apparatus
From Thomson 's separatus ( right )
E- time between
L Fe = CE Mates
e)Me could be determined The FEM -
oever
§ µ
.
.
. ,
by En
'
Electron is bend off
Ifield
the Electric 5 over =
averts-vv.t-vv.IT
'
✓ t
over
=
'
=
backstraight
ver
and bound
with a
Magnetic field
Ë=ÊE¥
.
Saai
Seeslides Lecture I
Millikan 's oil drop experiment .
Mist Oil Particle s are inserted and go through
Of Oil
"" ""
→ ; :
a hole to a detector
g. wagen
•
→ • oa .
•
Treron Outcome : The charge | the drop let
÷
↳
is
always a multiple of
" Electrical
The
droppletsgetcharged
%
field
.
charge e- so D= me
/ → van
detector
The Nucleus Scanning tunnel inz microscoop .
distance
remains
eigual
