Worksheet - X-rays Solution

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Le Fevre High School
SACE Stage 2 Physics
X-rays Solution
1 (a)
K
Intensity
White
background
radiation
K
Intensity
Sharp peaks
Sharp peaks
K
Background
radiation
K
Cut-off
frequency
Frequency
fmax
Minimum
wavelength
Wavelength
Cut off frequency
fmax depends on the accelerating voltage but does not depend on the target material or the
filament current. The higher fmax the more penetrating the X-rays.
"White" background radiation
"Bremsstrahlung" radiation: A continuous range of X-ray frequencies present up to fmax. The
intensity of this background increases with filament current.
Sharp Peaks of Intensity.
The sharp peaks depend on the type of target. eg. tungsten different to gold.
(i) Peaks change in frequency and intensity. They may not be present if V too small for the
new target.
f max stays the same. Intensity of white radiation will remain the same. Note that the question does
not mention filament current, which is the factor effecting intensity.
(ii) fmax will change. Peaks may disappear if V drops below the minimum for peaks or may appear if
not previously present when V increased. Overall intensity of the radiation will increase if V is
increased and filament current kept constant.
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(b) K of electrons = W on electrons by E field
1
i.e.. mv2 = q V
2
2qV
v2 =
m
2qV
Therefore v =
m
2 x 1.6 x 10 19 x 48 x 10 3
9.11 x 10 31
= 1.3 x 108 m s-1
=
2 K of an electron hitting the target = work done on it by field
= q V
= 1.6 x 10-19 x 66,000 J
When producing an X-ray of maximum frequency, all this energy becomes converted to a single photon
of radiation, of energy hf.
E 66000 x 1.6 x 10 19
i.e.. f = =
h
6.63 x 10 34
= 1.6 x 1019 Hz
3.
(i). Increasing the filament current in a hot-cathode X-ray tube will raise the temperature of
the filament, and so cause a greater number of electrons to be emitted per second. Hence, a
greater quantity of X-radiation ( more photons) results, but with same wavelength
(frequency) distribution.
(ii). Increasing the applied voltage will increase the energy gained by each electron as it
moves from filament to target and so on striking the target it will give up more energy: and
therefore produce photons of greater energy content, that is, of higher frequency, hence
X-ray is of shorter wavelength and greater penetrating power. The minimum voltage is
obtained by assuming that for some electrons striking the target, ALL their K is converted
into a photon of radiation.
Now energy of photon = hf. = hc/, (from c = f)
Now energy of electron is that given to it by field (approx.)
hc
E = qV =

hc
Therefore
Vmin =
q
=
6.63 x 10 34 x 3 x 10 8
1.0 x 10 11 x 1.6 x 10 19
= 124312.5 volt
Le Fevre High School
4
(a)
copper anode (+)
X rays
cathode(-)
Collimating
Slit
cooling fins
heater
6 V AC
electrons
tungsten
insert
20,000 - 200,000 V AC
evacuated glass
container
step up transformer
240 V AC
(b) (i) Filament: heated wire produces thermal electrons, these electrons are refined to a narrow
beam by the collimating slit.
(ii) Target: a dense high melting point metal. When high energy electrons interact with this
metal, they are decelerated and lose kinetic energy as either heat or a high energy X-ray photon.
(iii) Theory considers that during the electron collisions with the nuclei in the target the electrons
undergo accelerations which cause them to lose energy in the form of photons. The photons have
energy
Loss of kinetic energy = Ephoton = hf. Where h = Planck's constant.
f = the frequency of X-rays produced.
Like the photoelectric effect theory this assumes a 1:1 relation between a photon and an
electron, ie. each photon originates from one electron not many. But in this case each electron
may produce many photons as it accelerates in stages. Since the interaction of the electron with
the nucleus is random then a continuous range of photons are produced.
5. (a) The degree of absorption of an X-ray in the human body depends on,
The density of the tissue
X-rays will penetrate further into soft tissue than bone due to the density of these materials.
That is, the attenuation of X-rays is greater in more denser tissue.
The thickness of the tissue
A given thickness of soft tissue attenuates a beam less than does the same thickness of bone.
The atomic number of the elements that make up that tissue
the higher the atomic numbers of the elements present (there are more 'heavy' elements in
bone than in muscle) the greater the attenuation.
(b)
When using X-rays on a person, it is important to keep exposure time to a minimum.
This can be done by using a very sensitive film, increasing the filament current (number of electrons
hitting the target) and increasing the Voltage (determines the quality of the X-rays).
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