Radiology at a Glance

Rajat Chowdhury, Iain Wilson, Christopher Rofe, Graham Lloyd-Jones

• Publisher: Wiley-Blackwell
• Year: 2017
• Print ISBN: 9781118914779
• eBook ISBN: 9781118914786
• Edition: 2
• Topic: Medicine
• Subtopic: Radiology, Radiotherapy & Nuclear Medicine

Radiology at a Glance

The market-leading at a Glance series is popular among healthcare students, and newly qualified practitioners for its concise and simple approach and excellent illustrations.

Each bite-sized chapter is covered in a double-page spread with clear, easy-to-follow diagrams, supported by succinct explanatory text.

Covering a wide range of topics, books in the at a Glance series are ideal as introductory texts for teaching, learning and revision, and are useful throughout university and beyond.

Everything you need to know about Radiology… at a Glance!

Addressing the basic concepts of radiological physics and radiation protection, together with a structured approach to image interpretation, Radiology at a Glance is the perfect guide for medical students, junior doctors and radiologists.

Covering the radiology of plain films, fluoroscopy, CT, MRI, intervention, nuclear medicine and mammography, this edition has been fully updated to reflect advances in the field and now contains new spreads on cardiac, breast and bowel imaging, as well as further information on interventional radiology.

Radiology at a Glance:

• Assumes no prior knowledge of radiology
• Addresses both theory and clinical practice through theoretical and case-based chapters
• Provides structured help in assessing which radiological procedures are most appropriate for specific clinical problems
• Includes increased image clarity

Supported by 'classic cases' chapters in each section, and presented in a clear and concise format, Radiology at a Glance is easily accessible whether on the ward or as a quick revision guide.

For more information on the complete range of Wiley medical student and junior doctor publishing, please visit: www.wileymedicaleducation.com

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Part 1
Radiology physics

Chapters

1. Plain X-ray imaging
2. Fluoroscopy
3. Ultrasound
4. Computed tomography
5. Magnetic resonance imaging

1
Plain X-ray imaging

Plain X-ray physics

On 8 November 1895, the German physicist Wilhelm Conrad Röentgen discovered the X-ray, a form of electromagnetic radiation which travels in straight lines at approximately the speed of light. X-rays therefore share the same properties as other forms of electromagnetic radiation and demonstrate characteristics of both waves and particles. X-rays are produced by interactions between accelerated electrons and atoms. When an accelerated electron collides with an atom two outcomes are possible:

1. An accelerated electron displaces an electron from within a shell of the atom. The vacant position left in the shell is filled by an electron from a higher level shell, which results in the release of X-ray photons of uniform energy. This is known as characteristic radiation.
2. Accelerated electrons passing near the nucleus of the atom may be deviated from their original course by nuclear forces and thereby transfer some energy into X-ray photons of varying energies. This is known as Bremsstrahlung radiation.

The resultant beam of X-ray photons (X-rays) interacts with the body in a number of ways:

• Absorption – this prevents the X-rays reaching the X-ray detector plate. Absorption contributes to patient dose and therefore increases the risk of potential harm to the patient.
• Scatter – scattering of X-rays is the commonest source of radiation exposure for radiological staff and patients. It also reduces the sharpness of the image.
• Transmitted – transmitted X-rays penetrate completely through the body and contribute to the image obtained by causing a uniform blackening of the image.
• Attenuation – an X-ray image is composed of transmitted X-rays (black) and X-rays which are attenuated to varying degrees (white to grey). Attenuation can be thought of as a sum of absorption and scatter and is determined by the thickness and density of a structure. In the chest, structures such as the lungs are relatively thick but contain air, making them low in density. The lungs therefore transmit X-rays easily and appear black on the X-ray image. Conversely, bones are not thick but are very dense and therefore appear white. Attenuation can be controlled by varying the power or ‘hardness’ of the X-ray beam.

The X-ray machine (tube)

Most modern radiographic machines use electron guns to generate a stream of high energy electrons, which is achieved by heating a filament. The high energy electrons are accelerated towards a target anode. The electrons hit the anode, thereby generating X-rays as described above. This process is very inefficient with 99% of this energy transferred into heat at 60 kV. The dissipation of heat is therefore a key design feature of these machines to sustain their use and maintain their longevity. The material for the target anode is selected depending on the chosen task and the energy of the X-ray beam can be modified by filtration to produce beams of uniform energy.

Most modern radiology departments now employ digital imaging techniques and there are two principal methods in everyday use: computed radiography (CR) and digital radiography (DR). CR uses an exposure plate to create a latent image, which is read by a laser stimulating luminescence, before being read by a digital detector. DR systems convert the X-ray image into visible light, which is then captured by a photo-voltage sensor that converts the light into electricity, and thus a digital image. The final digital images are stored in medical imaging formats and displayed on computer terminals.

Applying physics to practice

• If the subject to be imaged is placed further from the detector, the image created will be magnified. This is based on the principle that X-ray beams travel in diverging straight lines.
• Scatter from the patient and other objects degrades the resolution. This will cause the image to be blurred.
• Beams of lower energy are absorbed more than beams of higher energy. This affects the difference in clarity between the soft tissue detail and artefact.

Image quality

The clarity of the image can be expressed as ‘unsharpness’. This can be classified into:

• Inherent unsharpness – this is caused by the structures involved not having sharp, well-defined edges.
• Movement unsharpness – this can be reduced by using short exposures, as with light photography.
• Photographic unsharpness – this is dependent on the quality and type of imaging equipment and the method of capturing the image.

Newer digital imaging systems now allow the postprocessing of data to enhance various aspects of the image.

Contrast

The contrast of an image is dependent on the variation of beam attenuation within the subject. There are five principal densities that can be seen on a plain radiographic image.

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Plain X-ray densities

Black Dark grey Light grey White Bright white

Air/gas Fat So...

Table of contents

• Cover
• epigraph
• Title Page
• Copyright
• Contributors
• Foreword
• Preface
• Abbreviations
• Terminology
• About the companion website
• Part 1: Radiology physics
• Part 2: Radiology principles
• Part 3: Plain X-ray imaging
• Part 4: Fluoroscopic imaging
• Part 5: Ultrasound imaging
• Part 6: Computed tomography imaging
• Part 7: Specialised imaging and magnetic resonance imaging
• Part 8: Interventional radiology
• Part 9: Nuclear medicine
• Index
• EULA