PRODUCTION & USE OF X-RAYS
Production of X-rays
- X-rays are short wavelength, high-frequency part of the electromagnetic spectrum
- They have wavelengths in the range $10^{-8}$ to $10^{-13} \mathrm{~m}$
- X-rays are produced when fast-moving electrons rapidly decelerate and transfer their kinetic energy into photons of EM radiation
Producing X-rays
- At the cathode (negative terminal), the electrons are released by thermionic emission
- The electrons are accelerated towards the anode (positive terminal) at high speed
- When the electrons bombard the metal target, they lose some of their kinetic energy by transferring it to photons
- The electrons in the outer shells of the atoms (in the metal target) move into the spaces in the lower energy levels
- As they move to lower energy levels, the electrons release energy in the form of $\mathbf{X}$-ray photons
- When an electron is accelerated, it gains energy equal to the electronvolt; this energy can be calculated using:
$
\mathbf{E}_{\max }=\mathbf{e V}
$
- This is the maximum energy that an X-ray photon can have
- Therefore, the maximum X-ray frequency $f_{\max }$, or the minimum wavelength $\lambda_{\min }$, that can be produced is calculated using the equation:
$
\mathrm{E}_{\max }=\mathrm{eV}=\mathrm{hf}_{\max }=\frac{h c}{\lambda_{\min }}
$
Maximum frequency: $\mathrm{f}_{\max }=\frac{e V}{h}$
Minimum wavelength: $\lambda_{\min }=\frac{h c}{e V}$
- Where:
- $\mathrm{e}=$ charge of an electron (C)
- $\mathrm{V}=$ voltage across the anode (V)
- $\mathrm{h}=$ Planck’s constant $(\mathrm{J}$ s)
- $c=$ speed of light $\left(\mathrm{m} \mathrm{s}^{-1}\right)$
Worked example: Production of X-rays
A typical spectrum of the X-ray radiation produced by electron bombardment of a metal target is shown below.
Explain why:
a) A continuous spectrum of wavelengths is produced.
b) The spectrum has a sharp cut-off at short wavelengths.
Answer/Explanation
Part (a)
- Photons are produced whenever a charged particle is accelerated towards a metal target
- The wavelength of the photons depends on the magnitude of the acceleration
- The electrons which hit the target have a distribution of accelerations, therefore, a continuous spectrum of wavelengths is observed
Part (b)
- The minimum wavelength is equal to
$
\lambda_{\min }=\frac{h c}{E_{\max }}
$
- This equation shows the maximum energy of the electron corresponds to the minimum wavelength
- Therefore, the higher the acceleration, the shorter the wavelength
- At short wavelengths, the sharp cut-off occurs as each electron produces a single photon, so, all the electron energy is given up in one collision
Using X-rays in Medical Imaging
- X-rays have been highly developed to provide detailed images of soft tissue and even blood vessels
- When treating patients, the aims are to:
- Reduce the exposure to radiation as much as possible
- Improve the contrast of the image
Reducing Exposure
- X-rays are ionising, meaning they can cause damage to living tissue and can potentially lead to cancerous mutations
- Therefore, healthcare professionals must ensure patients receive the minimum dosage possible
- In order to do this, aluminium filters are used
- This is because many wavelengths of X-ray are emitted
- Longer wavelengths of $\mathrm{X}$-ray are more penetrating, therefore, they are more likely to be absorbed by the body
- This means they do not contribute to the image and pose more of a health hazard
- The aluminium sheet absorbs these long wavelength X-rays making them safer
Contrast & Sharpness
- Contrast is defined as:
The difference in degree of blackening between structures
- Contrast allows a clear difference between tissues to be seen
- Image contrast can be improved by:
- Using the correct level of X-ray hardness: hard X-rays for bones, soft X-rays for tissue
- Using a contrast media
Sharpness is defined as:
How well defined the edges of structures are
- Image sharpness can be improved by:
- Using a narrower X-ray beam
- Reducing X-ray scattering by using a collimator or lead grid
- Smaller pixel size
ATTENUATION OF X-RAYS IN MATTER
Attenuation of X-rays in Matter
- Bones absorb X-ray radiation
- This is why they appear white on the X-ray photograph
- When the collimated beam of X-rays passes through the patient’s body, they are absorbed and scattered
- The attenuation of X-rays can be calculated using the equation:
$
I=I_0 e^{-\mu x}
$
- Where:
- $10=$ the intensity of the incident beam $\left(\mathrm{W} \mathrm{m} \mathrm{m}^{-2}\right)$
- $I=$ the intensity of the reflected beam $\left(\mathrm{W} \mathrm{m} \mathrm{m}^{-2}\right)$
- $\mu=$ the linear absorption coefficient $\left(\mathrm{m}^{-1}\right)$
- $x=$ distance travelled through the material $(\mathrm{m})$
- The attenuation coefficient also depends on the energy of the X-ray photons
- The intensity of the X-ray decays exponentially
- The thickness of the material that will reduce the X-ray beam or a particular frequency to half its original value is known as the half thickness
Worked example: Attenuation of X-rays in matter
A student investigates the absorption of X-ray radiation in a model arm. A cross-section of the model arm is shown in the diagram.
Parallel X-ray beams are directed along the line MM and along the line BB. The linear absorption coefficients of the muscle and the bone are $0.20 \mathrm{~cm}^{-1}$ and $12 \mathrm{~cm}^{-1}$ respectively.
Calculate the ratio:
intensity of emergent $X$-ray beam from model intensity of incident $X$-ray beam on model for a parallel X-ray beam directed along the line
a) $\mathrm{MM}$
b) $\mathrm{BB}$
and state whether the X-ray images are sharp, or have good contrast.
Answer/Explanation
Part (a)
Step 1:
Write out the known quantities
Linear absorption coefficient for muscle, $\mu=\mathbf{0 . 2 0} \mathbf{~ c m}^{-1}$
Distance travelled through the muscle, $x=\mathbf{8 . 0} \mathbf{~ c m}$
Step 2:
Write out the equation for attenuation and rearrange
$
I=I_0 e^{-\mu x}
$
$
\frac{\text { intensity of emergent } X-\text { ray beam from model }}{\text { intensity of incident } X-\text { ray beam on model }}=\frac{I}{I_0}=e^{-\mu \mathrm{x}}
$
Step 3:
Substitute in values and calculate the ratio
$
\frac{I}{I_0}=\mathrm{e}^{-(0.20 \times 8)}=0.2
$
Part (b)
Step 1:
Write out the known quantities
Linear absorption coefficient for bone, $\mu_b=12 \mathbf{c m}^{-1}$
Distance travelled through the muscle, $x_m=\mathbf{4 . 0} \mathbf{~ c m}$
Distance travelled through the bone, $x_b=\mathbf{4 . 0} \mathbf{~ c m}$
Step 2:
Write out the equation for attenuation for two media and rearrange
$
\frac{I}{I_0}=e^{-\mu_m x_m} \times e^{-\mu_b x_b}
$
Step 3:
Substitute in values and calculate the ratio
$
\frac{I}{I_0}=\mathrm{e}^{-(0.20 \times 4)} \times \mathrm{e}^{-(12 \times 4)}=6.4 \times 10^{-22} \approx 0
$
Step 4:
Write a concluding statement
Each ratio gives a measure of the amount of transmission of the beam
A good contrast is when:
- There is a large difference between the intensities
- The ratio is much less than 1.0
Therefore, both images have a good contrast
COMPUTED TOMOGRAPHY SCANNING
Computed Tomography Scanning
- A simple X-ray image can provide useful, but limited, information about internal structures in a 2D image
- When a more comprehensive image is needed, a computerised axial tomography (CAT or CT) scan is used
- The main features of the operation of a CT scan are as follows:
- An X-ray tube rotates around the stationary patient
- A CT scanner takes X-ray images of the same slice, at many different angles
- This process is repeated, then images of successive slices are combined together
- A computer pieces the images together to build a 3D image
- This 3D image can be rotated and viewed from different angles
Advantages & Disadvantages of CAT Scans
- Advantages:
- Produces much more detailed images
- Can distinguish between tissues with similar attenuation coefficients
- Produces a 3D image of the body by combining the images at each direction
- Disadvantages:
- The patient receives a much higher dose than a normal X-ray
- Possible side effects from the contrast media
Worked example
An X-ray image is taken of the skull of a patient. Another patient has a CT scan of his head. By reference to the formation of the image in each case, suggest why the exposure to radiation differs between the two imaging techniques.
Answer/Explanation
X-ray
The simple X-ray image involves taking a single exposure
This produces a single $2 D$ image
CT scan
The $\mathrm{CT}$ scan requires taking several exposures of a slice from many different angles
This is then repeated for different slices before being combined together to build a 3D image
This involves taking a much greater exposure than the simple X-ray