It does not hit the nucleus interaction, near the nucleus the interaction change spot will release energy called x-ray
Points to remember:
X-ray beam is not a solid beam
Electrical energy is converted to x-ray energy (1%) and heat (99%)
Millions of high-speed e- interact w/ uncountable number of atoms @ the target
The millions of x-rays produced are of different wavelength & energy
Production of x-ray
The kinetic energy of e- in the tube current converts to x-ray photons at the focal spot of an x-ray by the formation of Bremstrahlung radiation and Characteristic radiation.
2 mechanisms that explain x-ray production at the atomic level:
General radiation
Characteristic radiation
General Radiation (or Bremstrahlung radiation or Braking radiation)
Nucleus is very positive so it push the e- from Cathode out of the atom & changes the direction w/c produce x-ray
The incident photon from Cathode does not hit the nucleus, it sudden stop & changed its direction
Using 60-90 kVp (60,000-90,000 v)
Generation radiation can produce Heterogeneous radiation w/c is a radiation that consisting of different frequencies, various energies, or a variety of particles
Characteristic radiation:
The incident e- from Cathode hit the e- of the Anode and ejected the e- leaving a space / void rearrangement will occur w/c the e- near by will replace then the radiation is produced
Only 70 kVp is used
Primary beam: the x-ray beam produced at the focal spot of Anode & exits from Anode @ the tube head
2. Secondary radiation: X-ray produced when the primary beam interacts with matter
4. Attenuation: the reduction in the intensity of an x-ray beam as it interacts with atoms of an absorber (loss of energy beam)
6. Scattering: a form of attenuation where the x-ray is ejected out of the absorber
3. Scatter radiation : type pf secondary radiation that occurs when the x-ray beam deflected from its path due to it interacts w/ matter (change of path)
5. Absorption : a form of attenuation where the energy of the x-ray is imparted to the absorber (stay in the matter)
3 Possibilities when an x-ray photon interacts with matter
No interaction
Absorption of energy
Scatter of energy
Factors that affect the amount type of absorption
Energy of x-ray beam
Composition of absorber material
Atomic configuration of absorber material for aprons
4 interactions with matter
No interaction
No ionization - no scatter - no absorption
Photoelectric effect
Phenomenon in w/c e- are emitted from the matter due to their absorption of energy from electromagnetic radiation of very short wavelength (visible light or UV light)
e- emitted in this manner may be referred to as “Photoelectron”
The energy stay w/in the atom and be absorbed
ex. in radiograph; bone appears white because high density, high atomic number caused high absorption
Ionization - Absorption - No scatter
Coherent scattering
Also known as Thomson effect or Unmodified scatter
Dispersing of low-energy x-rays without the incident photon / x-ray losing its energy
Accounts for a practically negligible part of the total interaction between x- rays and matter
e- enters outer orbit but does not effected with any e- then it directed out from the atom in different direction
No change @ unmodified scatter
No ionization – No absorption – ONLY scatter
Compton scattering
Type of scatter that x-rays and gamma rays undergo in matter
The Inelastic scattering or Non-coherent scatter of photons in matter results in a decrease in energy of an x- ray or gamma ray photon
Energy of the scattered radiation is different from the incident radiation