X-ray Tube and X-ray Production Flashcards

1
Q

What are X-rays?

A

Type of electromagnetic radiation

Form part of the electromagnetic spectrum

Photons of energy travelling through space at a specific frequency and wavelength

Wavelength of x-rays ranges from 0.01 to 10 nanometers

Fairly high frequency and short wavelengths so x-ray photons have high a penetrative power

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2
Q

Ionising Radiation

A

High enough energy to strip electrons from an atom, or in the case of very high-energy radiation, break up the nucleus of the atom

Ionisation - the process in which an electron is given enough energy to break away from an atom

Results in the formation of two charged particles or ions: the molecule with a net positive charge, and the free electron with a negative charge

Results in chemical changes by breaking chemical bonds. This effect can cause damage to living tissue

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3
Q

Ionisation

A

Before:
1 atom containing 6 electrons, 6 protons and 6 neutrons

After:
1 positively charged ion containing 5 electrons, 6 protons and 6 neutrons + 1 free electron

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4
Q

Modern X- Ray Tube - what does it contain

A

Glass tube containing a vacuum

Functions as an energy converter

Receives electrical energy and converts it into two other forms of energy: x-radiation and heat

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5
Q

Rotating Anode X-Ray Tube

A

anode disc
anode stem

rotor support
rotor

bearings

vacuum

focusing cup

filament

cathode

glass envelope

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6
Q

stationary anode xray tube

A

glass envelope
copper anode
cathode
window
tungsten target

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7
Q

Cathode

A

Coiled filament wire which acts as a source of electrons

(-ve side of tube)

Two main parts:
coiled tungsten filament
nickel focusing cup

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8
Q

Cathode – Tungsten Filament

A

Why Tungsten?

Has a low work function – is a good thermionic emitter at lower temperatures

Does not easily evaporate

Will stay the same diameter therefore provides constant thermionic emission

Can be wound into a spiral (flexible) and is tough (high tensile strength)

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9
Q

Cathode Assembly

A

Most x-ray tube cathodes have two tungsten filaments to provide a large and a small focal spot size

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10
Q

Cathode – Focusing Cup

A

Nickel Focusing Cup

Negatively charged to keep the cloud of electrons from spreading apart

Designed to condense the electron beam to a small area on a focal track

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11
Q

Anode

A

A tungsten alloy target disc for the electrons which produces the x-ray photons

+ve side of tube

Two types of anode:
Rotating (found in most x-ray tubes)
Stationary (less common
eg. in dental x-ray machines)

Components
Anode Disc
Anode Stem
Motor

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12
Q

Anode Disc

A

Target anodes discs are made of tungsten alloy

Why Tungsten?

Tungsten is sufficiently dense to stop the electrons abruptly on its surface and thus produce maximum conversion of kinetic energy to X-ray energy

The tungsten nucleus has a high positive charge in its nucleus (Z=74) which causes greater deceleration of the electrons passing in vicinity of the nucleus

Has a high melting point of over 3000oC (highest melting point of all metals)

Low vapour production

Can be machined to give a smooth target track

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13
Q

Anode Stem

A

Made of molybdenum

Has to support the anode rotating at +3000rpm

Needs to resist heat flowing to the bearings

Must conduct electricity

In most tubes, the stem is short but thin

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14
Q

Anode Motor

A

Induction Motor

When the exposure button is pressed, a current is applied to the tube that produces a electromagnetic field that starts the rotation of the anode

This will cause the anode to spin to 3400 RPM

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15
Q

Envelope

A

Can be glass or metal
Contains the vacuum

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16
Q

Housing

A

Designed to limit the x-ray beam through the primary window

Minimise leakage of radiation with steel and lead

Insulating oil for heat dissipation

Provides mechanical support and damage protection

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17
Q

Power Source

A

High voltage generator – supplies the necessary electrical energy required to operate the x-ray tube

The x-ray tube requires electric energy to
To ‘boil’ electrons from the cathode filament
To accelerate these electrons from the cathode to anode

18
Q

High Voltage Generators

A

Main components:
Transformers
Autotransformer
Filament circuit
Rectifiers
Separate control/console panel circuit
All connected in a high voltage circuit

Three phase generator (combination of 3 single phase generators)

Used by heavy duty industrial, professional and medical equipment where an intensive, constant power supply is required

19
Q

Control Panel

A

Allows the radiographer to select the appropriate kVp, mA and exposure time

The exposure button readies the x ray tube for exposure by heating the filament and rotating the anode

Pressing the button further starts the exposure

The timing mechanism terminates the exposure

20
Q

Transformers

A

A device to either increase or decrease the voltage in a circuit through electromagnetic induction

Consists of two wire coils wrapped around a closed iron core

Step-up transformers
Step-down transformers

A transformer can not create energy

An increase in the voltage must be accompanied by a corresponding decrease in current

21
Q

Rectifier

A

Changes alternating current output of high voltage transformer to direct current

Allows current flow in one direction only at a steady constant rate

AC power will supply x-ray units with sinusoidal currents, resulting in ‘peaks and troughs’, limiting an x-ray tube to produce x-rays only half of the time during a cycle

A single-phase high voltage generator converts this AC power into a half or full wave rectified supply

22
Q

Half- Wave Rectification

A

Half wave rectification results in a peak voltage that will dip to zero in a reoccurring manner
This will consequently have an effect on the behaviour of radiation produced, hence the name kilovoltage peak (kVp)

23
Q

Full-Wave Rectification

A

Full wave rectification is more efficient

Bothe the +ve and –ve half cycles of the high tension transformer are used

The circuit reverses the –ve half cycle and applies it to the x-ray tube

24
Q

Constant Potential Generator

A

The advancement of high voltage generators from single-phase to three-phase to constant potential generators have overcome this ‘voltage ripple’ creating a continuous, uninterrupted voltage

Modern x-ray units that utilise constant potential generators, do not have ‘voltage ripple’ and consequently employ the term kV rather than kVp

25
How Does an X-Ray Tube Work?
Current flows along a wire = electrons moving A potential difference is applied at both ends of the conductor As current flows through there is an increase mechanical vibrational energy Raises temperature of the conductor = increase in heat energy Energy conversion: from electrical to heat energy
26
Thermionic Emission
Emission of electrons from heated metal Current increases temperature of tungsten filament in the cathode to about 2000oC Increased energy overcomes binding energy of atom Electrons are freed forming a ‘cloud’
27
X-Ray Production
The current (mA) applied to the cathode filament and the duration (seconds) will determine the total number of electrons released (mAs) The released electrons are charged with high velocity towards the positive anode by the tube voltage (kVp) applied across the tube At the anode, 99% of the energy from the electrons is converted to heat, and only 1% is converted to x-ray photons The x-ray photons are targeted perpendicularly out of the x-ray tube through a window and towards the patient producing the x-ray beam
28
Heat Dissipation
Rotating anode Tungsten Focal spot Glass Envelope Insulating oil Steel housing / lead casing
29
X-Ray Tube Rating
The parameters (kVp, mAs) that can be safely used during its operation without causing damage to the x-ray tube itself Unique to each individual x-ray tube model The amount of heat produced depends on: Voltage (kV) Current (mA) Length of exposure (s) Type of voltage waveform Number of exposure taken in rapid sequence Energy and heat are usually measured in Joules (J) but this is not normally used to measure x-ray tube heat The heat unit (HU) was introduced when single-phase equipment was common to make it easy to calculate heat
30
X-Ray Production at the Anode
When the accelerated electrons hit the anode they interact with the atoms of the anode and produce x-ray photons via two mechanisms: Characteristic Radiation (10%-20%) Bremsstrahlung Radiation (80%-90%)
31
Characteristic Radiation
A high energy electron collides with an inner shell electron and both end up ejected from the tungsten atom leaving a ‘vacant’ electron space An outer shell electron moves to fill this inner space emitting energy in the form of an x-ray photon in the process. The energy of the emitted x-ray photon is equivalent to the energy level difference between the outer and inner shell electron involved in the transition This is called characteristic radiation because the energy of the emitted electrons is dependent upon the anode material, not on the tube voltage Energy is released in specific values corresponding to the binding energies of different shells
32
Bremsstrahlung (Braking) Radiation
When high energy electrons penetrate the anode target, some electrons travel close to the nucleus due to the attraction of its positive charge and are subsequently influenced by its electric field These electrons are slowed down or ‘braked’ and their path is deflected whilst loosing a portion of their kinetic energy The energy lost is emitted as Bremsstrahlung radiation and this ranges over a spectrum of energies
33
Characteristic vs Bremsstrahlung
Characteristic radiation Only accounts for small percentage of x-ray photons produced Bombarding electron interacts with inner shell electron Radiation released due to electron dropping down into lower energy state Radiation released is of a specific energy X-ray beam energy depends on element of target atoms not tube voltage Bremasstrahlung Accounts for 80% of photons in x-ray beam Bombarding electron interacts with whole atom Radiation released due to diversion of bombarding electron as a result of the atomic pull Radiation released is of a large range of energies X-ray beam energy depends on tube voltage
34
X-Ray Spectrum
As a result of characteristic and bremsstrahlung radiation generation, a spectrum of X-ray energy is produced within the X-ray beam
35
Altering the X-Ray Spectrum
There are different ways of altering the range of energies in an x-ray spectrum: Changing the intensity of the x-ray beam – this can be achieved by altering the kilovoltage peak (kVp) which is the peak voltage applied to the x-ray tube and determines the acceleration of the electrons from the cathode to the anode A low accelerating voltage will produce lower intensity x-ray photons across the spectrum whilst a high accelerating voltage will produce higher intensity x-rays including larger characteristic peaks
36
Altering the X-Ray Spectrum
Changing the amount of x-ray photons present – this can be achieved by altering the current over a set period of time at the cathode and across the x-ray tube An increase in current (mA) results in a higher production of electrons that are inside the x-ray tube which will increase the quantity of x-ray photons produced The amount of time (seconds) used for a set current will also determine the number of electrons produced A combination of current and time known as milliampere-seconds (mAs) is a measure of radiation produced over a set amount of time via an x-ray tube The number of x-ray photons increase but the size of the characteristic peaks stays the same
37
X-Ray Energies
Superficial X-rays: 35 to 60 kV (Mammography) Diagnostic X-rays: 20 to 150 kV( General X-rays) Orthovoltage X-rays: 200 to 500 kV (Superficial Therapy) Supervoltage X-rays: 500 to 1000 kV (Superficial Therapy) Megavoltage X-rays: 1 to 25 MV (Linac)
38
Therapeutic Energies
In radiotherapy, the required energy of the produced photons is much greater (usually 1-25MV) There is still a negative cathode, positive anode and vacuum The photons are produced by a linear accelerator A linear accelerator is a device that uses high Radio‐Frequency (RF) electromagnetic waves to accelerate charged particles (electrons) to high energies in a linear path, inside a tube like structure called the accelerator waveguide.
39
Therapeutic Energies
In radiotherapy, the required energy of the produced photons is much greater (usually 1-25MV) There is still a negative cathode, positive anode and vacuum The photons are produced by a linear accelerator A linear accelerator is a device that uses high Radio‐Frequency (RF) electromagnetic waves to accelerate charged particles (electrons) to high energies in a linear path, inside a tube like structure called the accelerator waveguide.
40
Linear Accelerator
Electrons are emitted from an electron gun and accelerated in a straight line (to about 40% of the speed of light) Radiofrequency waves generated by a magnetron or klystron pass through a waveguide, establishing an electric field The radiofrequency waves ‘carry’ the electrons and give them their energy Electrons strike the target (at approximately 98% of the speed of light)