Physics
Home > Physics > Core > From ideas to implementation > From ideas to implementation: 1. Cathode rays
9.4 From ideas to implementation: 1. Cathode rays
| Syllabus reference (October 2002
version) |
|
1. Increased understandings of cathode rays led to
the development of television
|
Students learn to:
|
Students:
F = qE
and

|
Extract from Physics Stage 6 Syllabus
(Amended October 2002). © Board of Studies, NSW
[Edit: 14 Aug 08]
Prior Learning: Preliminary modules 8.2
(subsections 1 and 3) 8.3 (subsections 2 and 5)
identify
that moving charged particles in a magnetic field experience
a force
- Any moving charged particles that move in a magnetic
field will experience a force.

perform an
investigation and gather
first-hand information to observe the occurrence of different
striation patterns for different pressures in discharge
tubes
- You may be performing an investigation
that has been planned by your teacher. One suitable
investigation is described below. Take note of the safe
work practices required when any discharge apparatus is
operating.
- Gather information by observing and
recording observations in accurate summary form. Simple
diagrams can assist your recollection of phenomena
observed.
Using discharge tubes
A common piece of apparatus used for this investigation
is a set of glass discharge tubes at different pressures,
arranged side-by-side on a board. The tubes have been
sealed after having had varying amounts of air pumped out
of them (the more air pumped out, the lower the air
pressure).
Each tube contains an electrode at each end to allow the
application of a large voltage, which is provided by an
induction coil. The high voltage causes an electrical
discharge through the air in the tube, causing the air to
glow. Different discharge patterns are formed at different
pressures.
Sample observations
- At 5% of atmospheric pressure, long, thin red-purple
streamers appear between the two electrodes.
- At lower pressure, these streamers give way to a soft
red glow.
- Upon further pressure reduction, the glow is broken
into striations, bands of light and dark. The amount of
dark space between the glowing bands increases with
further reductions.
- At 0.01% of atmospheric pressure, the dark space
extends throughout the tube. At this very low pressure,
the glass near the anode glows a yellow-green
colour.
The following web site has some simple diagrams showing
various striation patterns and also provides information on
the properties of cathode rays.
Investigating new rays
Dr. E.P. Scarlett High School, Calgary Board of Education,
Canada
The following web site has an example of alternative
apparatus that can be used to show the above effects.
Gases that emit light
Chemical of the week, Science is Fun in the Lab of Shakhashiri

explain
that cathode ray tubes allowed the manipulation of a stream
of charged particles
- A cathode ray tube is a highly evacuated glass tube
containing two electrodes. A high voltage applied across
the electrodes causes cathode rays, streams of negatively
charged particles (electrons), to flow from the cathode
towards the anode, with little obstruction from the few
remaining gas particles.
- Structures built into or around the cathode ray tube
allow the cathode rays to be manipulated. Further
electrodes can be built into the cathode ray tube to create
an electric field to change the path of the cathode rays.
Magnetic fields can be applied to the cathode rays through
the glass from outside the tube. Solid objects can also be
placed inside the tube to block the path of the rays.

perform an
investigation to demonstrate
and identify
properties of cathode rays using discharge tubes:
- containing a Maltese cross
- containing electric plates
- with a fluorescent display
screen
- containing a glass wheel
and analyse the
information gathered to determine the sign of the charge on
cathode rays
- You may be performing an investigation
that has been planned by your teacher. Make sure you
identify and use safe work practices with induction coils
and discharge tubes during this investigation.
A table would be a suitable format for recording your
observations. List each feature of the various cathode ray
tubes you use and describe how each demonstrates a property
of cathode rays.
- Analyse the information gathered by
using your observations to justify inferences and
conclusions about the sign of the charge on cathode
rays.
The cathode ray tubes used to demonstrate the properties
of cathode rays are fairly standard across schools and below
are some web sites that outline common procedures you may
follow:
Investigating new rays
Dr E.P. Scarlett High School, Calgary Board of Education,
Canada
Cathode Ray Tube
Catharine H Colwell, Physics LAB online
Sample information
The Maltese cross is placed in the path of the cathode
rays, causing a clearly defined shadow at the end of the
tube. This effect is used to infer that cathode rays travel
in straight lines and are blocked by solid objects.
Pairs of electric plates cause the cathode rays to bend
towards the positive plate. This shows that cathode rays
are associated with negative charges.
A fluorescent screen shows that cathode rays can cause
fluorescence. This demonstrates that cathode rays have
energy. A fluorescent screen can also be used to trace the
path of cathode rays being manipulated by other means.
A lightweight glass paddle wheel, able to rotate freely,
is placed in the path of the cathode rays so that the rays
strike one edge of the wheel at a tangent. The cathode rays
cause the wheel to spin and move away from the cathode.
This demonstrates that the cathode rays must have momentum,
and therefore mass, and that they are emitted from the
cathode.

explain
why the apparent inconsistent behaviour of cathode rays
caused debate as to whether they were charged particles or
electromagnetic waves
- Early experiments with cathode rays provided apparently
inconsistent evidence about the nature of cathode rays,
which seemed to behave both as waves and as streams of
particles.
- Heinrich Hertz performed an experiment in 1883 that
appeared to show that cathode rays were not deflected by
electric fields. His experimental results were incorrect,
however his result was used as evidence that cathode rays
were electromagnetic waves, just like light which is not
deflected by electric fields.
- J. J. Thomson performed an experiment that showed that
a cathode ray beam was visibly deflected by an electric
field. This was interpreted as indicating that cathode rays
were charged particles.
- In 1892, Hertz also showed that cathode rays penetrated
thin metal foils. This was interpreted to mean that cathode
rays were electromagnetic waves.
- These apparently conflicting results arose from
inadequacies in experimental design and the then current
state of knowledge about the nature of atoms. The
properties of cathode rays were clarified by later
experiments.

identify
that charged plates produce an electric field
- An electric field exists in any region in which an
electrically charged object experiences a force. The
observation that charged plates exert a force on other
charged objects brought close to them indicates that an
electric field is associated with charged plates.

discuss
qualitatively the electric field strength due to a point
charge, positive and negative charges and oppositely charged
parallel plates
- An electric field has both strength and direction.
|
The strength of the electric field due to a
positive point charge diminishes with distance from
the object. The direction of the field is defined
as pointing radially away from a positive point
charge.
|
|
|
The strength of the electric field due to a
negative point charge diminishes with distance from
the object. The direction of the field is defined
as pointing radially towards a negative point
charge.
|
|
|
The electric field between two oppositely charged
parallel plates is uniform in strength and
direction. The field direction is defined as at
right angles to the plates and away from the
positive plate.
|
|
|
The number of the lines drawn to represent a field
at any point indicates the electric field strength
at that point. The stronger the field, the more
lines are drawn in a given space.
|
|
The following web sites have simple interactive examples
of electric field strength. You may need to be patient if you
are using an early version computer.
Electric Force Fields
University of Colorado, Boulder, Colorado, USA.
Electric Field Shapes
David Hoult, Open Door Web Site, Ecole Active Bilingue
Jeannine Manuel in Paris, France.

describe
quantitatively the electric field due to oppositely charged
parallel plates
-
E = V/d, where
- E is electric field
strength between two oppositely charged parallel
plates,
- V is the potential
difference between the plates in volts, and
- d is the distance between
the plates in metres.
-
Electric field strength, E,
between two oppositely charged parallel plates is:
- proportional to the potential difference,
V, between the plates;
- inversely proportional to the separation,
d, between the plates;
- the same at all points in the region between the
plates; and
- at right angles to the plates everywhere in the
region between the plates.

describe
quantitatively the force acting on a charge moving through a
magnetic field 
-
, where
- F is the force on the
charged object,
- q is the charge in
coulombs,
- v is the velocity of the
charged object in m s-1,
- B is the magnetic field
flux density (or magnetic induction) in teslas,
and
is the angle between the velocity and
the magnetic induction.
-
Force, F, on a charge moving
through a magnetic field is:
- proportional to the size of the charge,
q;
- proportional to the velocity of the charge,
v;
- proportional to the magnetic induction,
B; and
- proportional to the sine of the angle,
, between the velocity and the magnetic
induction, being a maximum when
is 90° (that is, when the velocity
is at right angles to the field), and zero when
is zero (that is, when the velocity is
parallel to the field).

solve
problems and analyse
information using
F=qE
and 
- Solve problems by selecting the
appropriate equation, rearranging the equation where
necessary, substituting known data for the variables, and
computing the answer.
A sample problem:
A proton travelling at 5.0 x 104 m
s-1 enters a magnetic field of strength 1.0
Tesla at 90°. Determine the magnitude
of the force experienced by the proton.
Solution:
Another sample problem, requiring
rearrangement of the equation:
The path of a helium nucleus, travelling at 3.0 x
103 m s-1, makes an angle of 90°
to a magnetic field. The electron experiences a force of
1.2 x 10-15 N while in the field. Calculate the
strength of the field.
Solution:
Here is a sample problem for you to
try:
Two parallel plates, placed 0.1 m apart, are connected
to a 6-volt battery. Determine the electric field strength
between the plates.
Solution
-
Analyse information by
examining relationships between the variables in the
equations given.
Sample analysis questions:
- If the potential difference between two charged
parallel plates is kept the same, while the plates are
moved closer together, how will this affect the
electric field strength between the plates?
Analysis: E = V / d. Since E is inversely proportional
to d, if d is reduced E will be increased. For example,
if the separation is halved, the field strength will be
doubled.
- A proton and an alpha particle are travelling
parallel to each other with the same speed in the same
magnetic field. Which will experience the greater
force?
Analysis:
. Since F is directly
proportional to q, and v and B are equal for both
particles, the alpha particle, with two protons, will
experience a greater force than the proton alone.

outline
Thomson's experiment to measure the charge/mass ratio of
an electron
- Cathode rays were passed through two narrow slits to
make a thin parallel beam aimed at the centre of a
fluorescent screen. Electrodes were placed to create a
uniform electric field that exerted a downward force on the
beam. Electromagnets were placed to produce a uniform
magnetic field that exerted an upward force on the beam.
- Thomson manipulated the strengths of the two fields
until the beam passed through both fields undeflected. This
showed that the two forces on the particles (electrons) in
the beam were equal and opposite. By equating the
expressions for these two forces, Thomson calculated the
velocity of the particles.
- Thomson removed the electric field and calculated the
radius of the circular path followed by the particles in
the uniform magnetic field alone. By equating the force due
to the magnetic field to the centripetal force, he was able
to calculate that all cathode ray particles (electrons) had
the same charge / mass ratio of 1.76 x
1011 C kg-1.

- electrodes in the electron gun
- the deflection plates or coils
- the fluorescent screen
in the cathode ray tube of conventional TV displays and
oscilloscopes
- The electron gun produces a narrow beam of electrons.
The electrodes in the gun accelerate the electrons.
- The deflection plates or coils establish an electric
field that controls the deflection of the electron beam
from side to side and up and down.
- The fluorescent screen is coated with a material that
emits light when struck by electrons in the cathode ray.
This allows the position of the beam to be seen where it
strikes the screen.
