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BASIC PHYSICS OF DIGITAL RADIOGRAPHY By : Maisa Alhassoun [email protected]

B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun [email protected]

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Page 1: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

BASIC PHYSICS OF DIGITAL RADIOGRAPHY

By : Maisa [email protected]

Page 2: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

IMAGING WITH FILM The greatest challenge

of film radiography is to get the range of exposure to fit into the dynamic range of the film.

If the exposure falls outside the latitude, there will be little or no image contrast formed.

Page 3: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

IMAGING WITH FILM There are two

conditions that contribute to receptor exposure outside the film latitude: Error in setting the

correct exposure factors. Some regions of the

body have wide dynamic of exposure that exceeds the latitude of the film.

Using a wider latitude film can correct this but results in lower image contrast.

Page 4: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

THE ADVANTAGE OF A WIDE DYNAMIC RANGE

Here we can see the advantages of a digital receptor that has a wide dynamic range.

Even when there is a wide range of exposure coming from the body (wide histogram) and exposure at different levels (exposure errors) they still fit within the dynamic range.

Page 5: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL IMAGE CONTRAST

In a digital image, contrast is represented by different pixel values.

A typical digital receptor will have a linear relationship between exposure and resulting pixel value.

Page 6: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL IMAGE CONTRAST

We have seen that this relationship extends over a relatively wide range of exposures.

This is contrasted with the non-linear relationship seen with film.

Page 7: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

OPTIMUM EXPOSURE IN DIGITAL RADIOGRAPHY

The wide dynamic range and linear response of digital receptors is like a double edged sword.

The advantage is a wide range of exposures and exposure errors will still produce an image with good contrast.

Page 8: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

OPTIMUM EXPOSURE IN DIGITAL RADIOGRAPHY

So, what is the problem? There are two that we can see here.

Even though good contrast with low exposure is obtained. Due to the low exposure, we have high noise.

Page 9: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

OPTIMUM EXPOSURE IN DIGITAL RADIOGRAPHY

With film the image would be light.

The other problem is that exceptionally good images are obtained with high exposure ( very low noise).

With film the image would be dark or over exposed

Page 10: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

OPTIMUM EXPOSURE IN DIGITAL RADIOGRAPHY

In general, the challenge is to make sure the exposure factors are set for optimum image quality.

Page 11: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

MONITORING EXPOSURE LEVELS

One of the challenges is to know when the digital image is properly exposed since it is unlike film where under and over exposure is obvious.

Each manufacturer of digital receptors will provide an approach to calculate the image exposure information.

Page 12: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

MONITORING EXPOSURE LEVELS

Some will display the “S” number. This displayed value generally indicates the speed of the receptor that would match the actual exposure.

Page 13: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

MONITORING EXPOSURE LEVELS

A low exposure would result in a high calculated S number (like S=1000) and a high exposure would produce a low number (like s=50).

This is opposite of screen-film speed.

Page 14: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

MONITORING EXPOSURE LEVELS

The operator should determine the appropriate range of values for optimum exposure and monitor the values.

The method varies by manufacturer and clinical procedure.

Page 15: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL EXPOSURE

Proper exposure Over exposure

Page 16: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL RADIOGRAPHY IMAGE QUALITY

Like all x-ray images, there are 5 specific quality characteristics. Spatial detail Detail Contrast Noise Artifacts

We will now see how 3 of these, contrast, detail and noise are effected by the operation of digital radiography.

Page 17: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL RADIOGRAPH CONTRAST

Contrast sensitivity of digital procedures and image contrast depend upon several factors.

Two are:X-ray beam

spectrumScattered radiation Similar to film.

Page 18: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL RADIOGRAPH CONTRAST

What is different is the ability to adjust and optimize contrast after the image is recorded.

This is done through the digital processing of the image and then the adjustment of the window when the image is being viewed.

Page 19: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL RADIOGRAPHIC DETAIL

Visibility of detail is reduced and limited by the blurring that occurs at different stages of the imaging process.

Some are common to both film and digital radiography.

Page 20: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

COMMON SOURCES OF BLURRING

Common sources of blurring;The focal spot

(depends upon size and object location.)

Motion if presentThe receptor (generally

due to light spreading within the fluorescent or phosphor screen)

Page 21: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL SOURCES OF BLURRING

Additional blurring is the result of dividing the image into pixels.

The size of a pixel (amount of blurring) is the ratio of the image size (image size relative to the anatomy) and the matrix size.

Page 22: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL SOURCES OF BLURRING Pixel size is another

factor that must be considered because it limits the detail of the image.

1024 x 1280 on a 18cm x 24 cm image would be sharper than on a 35 cm x 43 cm image.

Generally, digital images lack the spatial detail of film images due to the digital processing.

Page 23: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

NOISE IN DIGITAL RADIOGRAPHS

The most predominate source of noise in digital imaging is quantum noise associated with the random distribution of the x-ray photons received by the image receptor.

Page 24: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

NOISE IN DIGITAL RADIOGRAPHS

The level of noise depends upon the amount of receptor exposure used to produce the image.

With digital imaging, it can be adjusted over a wide range due to the wide dynamic range.

Page 25: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

NOISE IN DIGITAL RADIOGRAPHS

Noise is controlled by using the appropriate exposure factors.

Page 26: B ASIC P HYSICS OF D IGITAL R ADIOGRAPHY By : Maisa Alhassoun maisa@inaya.edu.sa

DIGITAL IMAGE NOISE

Underexposed Proper exposure