X-ray tube

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An x-ray tube functions as a specific energy converter, receiving electrical energy and converting it into two other forms of energy: x-radiation (1%) and heat (99%). Heat is considered the undesirable product of this conversion process; therefore x-radiation is created by taking the energy from the electrons and converting it into photons. This very specific energy conversion takes place in the x-ray tube.

Construction of the x-ray tube

The x-ray tube contains two principal elements:

  1. filament (also the cathode): electronboils off electrons by thermionic emission
  2. target (also the anode): material in which electron beam conversioninteracts to produce x-rays

Additional components include:

  • expansion bellows (provide space for oil to expand)
  • tube envelope (evacuated)
  • tube housing
  • cooling dielectric oil
  • rotor
  • induction stator
  • tube window: usually made from beryllium, not glass

The filament/cathode and target/anode are contained in the envelope, which provides vacuum, support and electrical insulation. The envelope is most often made from glass, although some tubes contain envelopes formed from ceramic or even metal. For some demanding application such as dual energy CT rotating envelope tubes (RET) are used. Unlike conventional x-ray tubes, in rotating envelope tubes, not only the anode, but the entire vacuum tube rotates, furthermore, the anode is in direct contact with the liquid coolant, resulting in improved heat conduction and increased performance 4

The energy used for this process is provided from thea generator, connected by an electrical circuit connected to the systemx-ray tube. The generator also needs to convert the mains supplied alternating current (AC), from the power supply, into direct current (DC), as needed by the x-ray tube. The reason for this is to ensure a constant unidirectional flow of electrons from the positive charged cathode to negatively charged anode.

The quality and the quantity of the x-radiation are controlled by adjusting the electrical parameters (kV – tube voltage (potential difference applied across the tube), mA – tube current (flows through the tube) and exposure time, usually a fraction of a second.

To summarise, x-rays are produced in a standard way: by heating a filament, which releases electrons by thermionic emission, accelerating electrons with a high voltage and allowing them to collide with the focal spot on the target/anode. X-rays are produced whenvia two interactions in the anode :

a) Bremsstrahlung X-rays (German for "Braking") - electrons lose kinetic energy as they pass through atoms in the anode because they are attracted to the positively charges nuclei. The closer to the nucleus the electron passes, the more kinetic energy it loses and it is deflected to continue moving in another direction at a lower energy, or stopped altogether. This is where maximum kinetic energy is transferred to the production of an x-ray that is emitted from the anode.

b) Characteristic X-rays - If electrons possess an energy that is equivalent to, or greater than, the binding energy of the orbiting electrons in target atoms, these electrons are suddenly decelerated upon collision withlikely to be ejected from the metal targetatom. TheseThis most often occurs in the inner electron shell (K-shell). The ejected electron is known as a photoelectron. The vacancy left in the K-shell must be filled in order for the atom to remain stable (law of conservation of energy) so outer shell electrons drop down to fill the shell. This process of electron transfer between shells produces x-rays that are called “braking radiation” (bremsstrahlung). If the electrons have high energy, they can expel an electron out"characteristic" of the atomic shellbinding energies of the bombardedthat particular atom. Electrons from a higher energy level fill/material, hence the place of the expelled electron, emitting x-ray photons with quantized (precise) energies, determined by the respective electron energy levels. The x-rays produced in this way are called “characteristic x-raysname.

  • -<p>An <strong>x-ray tube</strong> functions as a specific energy converter, receiving electrical energy and converting it into two other forms of energy: <a href="/articles/x-rays-1">x-radiation</a> and heat. Heat is considered the undesirable product of this conversion process; therefore x-radiation is created by taking the energy from the <a href="/articles/electron">electrons</a> and converting it into <a href="/articles/photon">photons</a>. This very specific energy conversion takes place in the x-ray tube.</p><h4>Construction of the x-ray tube</h4><p>The x-ray tube contains two principal elements:</p><ol>
  • -<li>filament (also the <a href="/articles/cathode-x-ray-tube">cathode</a>): electron emission</li>
  • -<li>target (also the <a href="/articles/anode-x-ray-tube">anode</a>): electron beam conversion to x-rays</li>
  • +<p>An <strong>x-ray tube</strong> functions as a specific energy converter, receiving electrical energy and converting it into two other forms of energy: <a href="/articles/x-rays-1">x-radiation</a> (1%) and heat (99%). Heat is considered the undesirable product of this conversion process; therefore x-radiation is created by taking the energy from the <a href="/articles/electron">electrons</a> and converting it into <a href="/articles/photon">photons</a>. This very specific energy conversion takes place in the x-ray tube.</p><h4>Construction of the x-ray tube</h4><p>The x-ray tube contains two principal elements:</p><ol>
  • +<li>filament (also the <a href="/articles/cathode-x-ray-tube">cathode</a>): boils off electrons by thermionic emission</li>
  • +<li>target (also the <a href="/articles/anode-x-ray-tube">anode</a>): material in which electron beam interacts to produce x-rays</li>
  • -</ul><p>The filament/cathode and target/anode are contained in the envelope, which provides vacuum, support and electrical insulation. The envelope is most often made from glass, although some tubes contain envelopes formed from ceramic or even metal. For some demanding application such as dual energy CT <a href="/articles/rotating-envelope-tubes">rotating envelope tubes (RET)</a> are used. Unlike conventional x-ray tubes, in rotating envelope tubes, not only the anode, but the entire vacuum tube rotates, furthermore, the anode is in direct contact with the liquid coolant, resulting in improved heat conduction and increased performance <sup>4</sup>. </p><p>The energy used for this process is provided from the generator, connected by an electrical circuit connected to the system. The generator also needs to convert the alternating current (AC), from the power supply, into direct current (DC), as needed by the x-ray tube.</p><p>The quality and the quantity of the x-radiation are controlled by adjusting the electrical parameters (<a href="/articles/kilovoltage-peak">kV</a> – tube voltage (potential difference applied across the tube), <a href="/articles/tube-current">mA</a> – tube current (flows through the tube) and exposure time, usually a fraction of a second.</p><p>To summarise, x-rays are produced in a standard way: by heating a filament, which releases electrons by <a href="/articles/thermionic-emission">thermionic emission</a>, accelerating electrons with a high voltage and allowing them to collide with the <a href="/articles/focal-spot">focal spot</a> on the target. X-rays are produced when the electrons are suddenly decelerated upon collision with the metal target. These x-rays are called “braking radiation” (<a href="/articles/bremsstrahlung">bremsstrahlung</a>). If the electrons have high energy, they can expel an electron out of the atomic shell of the bombarded atom. Electrons from a higher energy level fill the place of the expelled electron, emitting x-ray photons with quantized (precise) energies, determined by the respective electron energy levels. The x-rays produced in this way are called “<a href="/articles/characteristic-radiation">characteristic x-rays</a>”.</p>
  • +</ul><p>The filament/cathode and target/anode are contained in the envelope, which provides vacuum, support and electrical insulation. The envelope is most often made from glass, although some tubes contain envelopes formed from ceramic or even metal. For some demanding application such as dual energy CT <a href="/articles/rotating-envelope-tubes">rotating envelope tubes (RET)</a> are used. Unlike conventional x-ray tubes, in rotating envelope tubes, not only the anode, but the entire vacuum tube rotates, furthermore, the anode is in direct contact with the liquid coolant, resulting in improved heat conduction and increased performance <sup>4</sup>. </p><p>The energy used for this process is provided from a generator, connected by an electrical circuit connected to the x-ray tube. The generator also needs to convert the mains supplied alternating current (AC), into direct current (DC), as needed by the x-ray tube. The reason for this is to ensure a constant unidirectional flow of electrons from the positive charged cathode to negatively charged anode.</p><p>The quality and the quantity of the x-radiation are controlled by adjusting the electrical parameters (<a href="/articles/kilovoltage-peak">kV</a> – tube voltage (potential difference applied across the tube), <a href="/articles/tube-current">mA</a> – tube current (flows through the tube) and exposure time, usually a fraction of a second.</p><p>To summarise, x-rays are produced in a standard way: by heating a filament, which releases electrons by <a href="/articles/thermionic-emission">thermionic emission</a>, accelerating electrons with a high voltage and allowing them to collide with the <a href="/articles/focal-spot">focal spot</a> on the target/anode. X-rays are produced via two interactions in the anode :</p><p>a) Bremsstrahlung X-rays (German for "Braking") - electrons lose kinetic energy as they pass through atoms in the anode because they are attracted to the positively charges nuclei. The closer to the nucleus the electron passes, the more kinetic energy it loses and it is deflected to continue moving in another direction at a lower energy, or stopped altogether. This is where maximum kinetic energy is transferred to the production of an x-ray that is emitted from the anode.</p><p>b) Characteristic X-rays - If electrons possess an energy that is equivalent to, or greater than, the binding energy of the orbiting electrons in target atoms, these electrons are likely to be ejected from the atom. This most often occurs in the inner electron shell (K-shell). The ejected electron is known as a photoelectron. The vacancy left in the K-shell must be filled in order for the atom to remain stable (law of conservation of energy) so outer shell electrons drop down to fill the shell. This process of electron transfer between shells produces x-rays that are "characteristic" of the binding energies of that particular atom/material, hence the name.</p>

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