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Characteristic Radiation in Tungsten Targets Shell # of electrons Binding energy L Char M N O P Eff X-ray Energy K

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Presentation on theme: "Characteristic Radiation in Tungsten Targets Shell # of electrons Binding energy L Char M N O P Eff X-ray Energy K"— Presentation transcript:

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10 Characteristic Radiation in Tungsten Targets
Shell # of electrons Binding energy L Char M N O P Eff X-ray Energy K 2 69 57.4 66.7 68.9 69.4 69.5 8 12 9.3 11.5 12.1 18 3 2.2 2.7 2.8 32 1 0.52 0.6 0.1 0.08

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12 In a tungsten target, at any kVp less than 69.5 all x-rays are Brems.
At 100 kVp, 85% of photons are Brems and 15% are characteristic Only 15 different energy levels are possible with characteristic production in tungsten tube.

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21 determine energy of electrons  energy of X-ray photons
FIGURE 3. X-ray generator and x-ray tube components are illustrated. The x-ray generator provides operator control of the radiographic techniques, including tube voltage (kVp), tube current (mA), and exposure duration, and delivers power to the x-ray tube. The x-ray tube provides the environment (evacuated x-ray tube insert and high-voltage cable sockets), source of electrons (cathode), source of x-rays (anode), induction motor to rotate the anode (rotor/stator), transformer oil and expansion bellows to provide electrical and heat build-up protection, and the tube housing to support the insert and provide protection from leakage radiation. determine number of electrons  number of X ray photons Lecture 5: Patient Dose Management

22 Photons entering the human body will either penetrate, be absorbed,
X-ray tube Photons entering the human body will either penetrate, be absorbed, or produce scattered radiation Lecture 5: Patient Dose Management

23 Image Contrast No object image Object silhouette Object image
Image contrast. Differential absorption of the X-ray beam by different parts of an object renders its internal structure visible in an X-ray transmission image. X-ray photons are represented as arrows. The left-hand example shows an object that allows all X-ray photons to pass through it unattenuated. In this circumstance, no image of the object is generated. The center example shows an object, different parts of which absorb different fractions of the incident photons modulating the beam intensity and generating an X-ray image of the object. The right-hand example is completely opaque to X-ray photons and absorbs all of them. The X-ray image of this object would be a silhouette with no definition of the object’s internal structure. No object image is generated Object silhouette with no internal details Object image is generated Lecture 5: Patient Dose Management

24 Where do X-rays come from ?
Atom of the target element Characteristic X-ray Nucleus Bremsstrahlung Electrons


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