properties of x-rays 1 Flashcards

1
Q

what is the production of x-rays?

A

-x-rays and electron can be generated by machines
-diagnostic x-ray units create images using a beam of x-rays transmitted through a patient
-therapy x-ray units treat cancer and other diseases using a beam of x-rays absorbed in the patient

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2
Q

what is diagnostic radiology?

A

-a beam of x-rays is generate in an x-ray tube and directed at a patient
-the x-rays are attenuated by the patient’s tissues as the beam passes through the patient
-attenuate means to reduce intensity
-intensity is the number of x-rays per unit area per unit time (ex: number of x-rays per cm^2 per second)

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3
Q

what shows up on x-rays of diagnostic radiology?

A

less coming out will look whiter (bone is very white, air is dark)
-fat, soft tissue, air and bone in the patient attenuate the x-rays differently
-this produces a variation of the transmitted x-rays or a pattern
-the pattern of transmitted x-rays is converted into a visible image
-the greater the number of x-rays attenuated, the white the image

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4
Q

how are x-rays created?

A

-x-rays are created in an x-ray tube by accelerating electrons (to give them energy)
-the electrons interact with a target, producing x-rays

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5
Q

what does an x-ray tube consist of?

A

-a cathode (negative electrode) and anode (positive electrode) in an evacuated glass envelope (to prevent electron collisions with gas molecules)
-the cathode (filament) is the source of electrons
-the anode is the target of the electrons

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6
Q

how do we make the electrons at the cathode?

A

-as the cathode is heated by the filament current, electrons ‘boil’ off (thermionic emission)
-electrons are repelled by the negative cathode and attracted by the positive anode
-the electrons accelerate towards the anode because of the potential difference between the cathode and the anode

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7
Q

what is potential difference?

A

-potential, or potential difference, is the electrical pressure that us used to accelerate the electrons (measured in volts, V)
-the voltage setting on the x-ray machine (‘tube voltage’) corresponds to the potential difference applied between the anode and cathode (in kilovolt range, kV)

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8
Q

what happens as the electrons go down?

A

-as the electrons accelerate, they gain kinetic energy
-the energy acquired by the electrons is measured in electron volts eV
-1eV is the energy of an electron accelerated across a potential difference of 1V
-therefore, the energy of an electron accelerated across a potential difference of 100kV is 100eV
-the tube voltage (kV) applied therefore determines the maximum energy of the electrons hitting the target

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9
Q

what is the tube current flow?

A

-the tube current is the flow of electrons through the tube (measured in ampere A)
-increasing the tube current will increase the number of electrons hitting the target

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10
Q

as electrons interact with the target, their kinetic energy is ____________

A

converted into heat (99%) and x-rays (1%)
-the x-rays produced include characteristic x-rays and bremsstrahlung x-rays

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11
Q

what are the two x-rays produced?

A

-characteristic x-rays are produced when an incoming electron knocks an orbital electron in a target atom out of it shell
-bremsstrahlung x-rays are produced when an incoming electron interacts with a nucleus in a target atom

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12
Q

why do we use tungsten at the anode?

A

-in order to generate enough x-rays to acquire a radiograph, the anode will get very hot (anode rise in temperature for a 2 second exposure is 2900 C)
-tungsten is used for the target material because it has a melting point of 3370 celcius and is able to withstand the heat
-as well, the efficiency of x-ray production increases with increasing atomic number (Z) and Z=74 for tungsten

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13
Q

what is tube voltage, tube current and exposure time?

A
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14
Q

what is the graph of interactions of electrons with the target of characteristic x-rays?

A
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15
Q

when are characteristic x-rays produced?

A

-produced when an incoming electron knocks an orbital electron out of its shell
-the incoming electron is the accelerated electron directed at the target
-the orbital electron is from an atom in the anode material

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16
Q

what is the definition of characteristic x-rays?

A

-defined as the radiation produced when an electron shell vacancy is created and an outer shell electron fills the vacancy, emitting an x-ray with energy equal to the difference in shell binding energies
-possible characteristic x-ray energies found by taking energy differences between the K, L, M and N shells

17
Q

why are they called characteristic x-rays?

A

-each element has different shell binding energies (ex: K shell for tungsten is 69.5 keV and K shell for calcium is 4.0keV)
-x-rays are therefore emitted with discrete energies characteristic of atoms in the target and the energies between the shells where the transitions take place

18
Q

what is an example of a characteristic x-ray?

A

to hit electron out, it must have energy at least equal to the binding energy

19
Q

how much of diagnostic x-ray beam is composed of characteristic x-rays?

A

-a typical diagnostic beam is composed of less than 20% characteristic x-rays
-the remainder of the x-rays (over 80%) are bremsstrahlung x-rays

20
Q

what is the graph of interactions of electrons with the target of a bremsstrahlung x-ray?

A
21
Q

when are bremsstrahlung x-rays produced?

A

-produced when an incoming electron (-) interacts with a nucleus (+) through electrostatic (Coulomb) force
-the incoming electron is the accelerated electron directed at the target
-the nucleus is from an atom in the anode material

22
Q

what is the definition of bremsstrahlung x-rays?

A

-defined as the radiation produced when an electron gives up part or all of its energy during a ‘collision’ with a nucleus (the electron is slowed, or braked, by the nucleus)
-the electron loses kinetic energy which is converted into a photon (x-ray) to satisfy the law of conservation of energy (energy cant be created nor destroyed)

23
Q

what are bremsstrahlung x-rays referred to as?

A

-white radiation or braking radiation
-the x-ray is emitted with a spectrum of energies up to the initial electron energy

24
Q

what does the energy of bremsstrahlung x-rays depend on?

A

-depends on how much the electron is slowed, which depends on how close it passes to the positively charged nucleus
-if the electron directly impacts the nucleus, and stops, then the energy of the outgoing x-ray is equal to that of the incoming electron`

25
Q

what is the possibility of x-rays?

A
26
Q

what is the description of x-ray spectrum?

A

-a graph representing an x-ray beam generated by an x-ray tube
-the x-axis is x-ray energy
-the y-axis is the number of x-rays of each particular energy
-an x-ray spectrum includes both characteristic and brem x-rays

27
Q

what is the x-ray spectra?

A
28
Q

why is brem a continuous spectrum of x-ray energies?

A

brem x-rays energy depends on incoming electron energy and how close the electron passes to the nucleus
-the energy of the electrons accelerate in an x-ray tube is variable (a continuous spectrum of electron energies)
-distance of the electrons from the nucleus varies, and this determines the energy of x-ray produced

29
Q

what is the continuous spectrum?

A
30
Q

what does the x-ray spectra look like with brem x-rays?

A
31
Q

why are filters added to brem x-rays?

A

-filters (usually a metal) are inserted into the path of the beam, before it reaches the patient and preferentially remove low energy x-rays (resulting in curve b)
-there is also inherent filtration of low energy x-rays (ex: the wall of the tube)
-curve b represents the x-rays used to image the patient

32
Q

what is the maximum energy and average energy of x-rays?

A