XrayFund
5/12/99
Beam angle vs FFD
| |
40" |
60" |
72" |
|
Size |
|
|
|
|
8x10 |
14 |
9 |
8 |
|
10x12 |
18 |
11 |
10 |
|
14x17 |
24 |
16 |
13 |
|
14x36 |
|
|
28 |
- Need to get the correct bevel on the anode to have the correct focal position and beam coverage
- Could do most shots at 72" for everyone
X-ray production
- Characteristic radiation
- The radiation produced is characteristic for the anode material
- Depended on electron binding energies for the target material
- Projectile electron ionizes a K shell electron
- Electrons from higher orbits fill the "hole"
- The change in electron binding energies results in photons w/the keV value—69.5keV
- The K shell binding of electrons is different for different materials depending upon the nucleus
- The projectile energy of the electron from the cathode must have more energy than the energy binding the electron in the K shell
- When an electron from the K shell leaves, it pulls an electron from a higher orbit to fill the space, changing the electrical configuration of the molecule—X-ray
- at 70keV, 15% is characteristic radiation (actual x-ray)
- Bremsstrahlung radiation
- Below 70keV, all Bremsstrahlung radiation—not enough energy to create an x-ray
- at 70keV, 85% is Bremsstrahlung radiation
- Above 70keV, Bremsstrahlung radiation
- Braking (slowing, decelerating) radiation
- Projectile electron (negative charge) comes under influence of the nucleus (electric Coulomb force)
- Projectile electron changes direction, variably
- Change in direction causes bremsstrahlung x-ray photon production (conservation of momentum)
- Electrons always travel at the speed of light or not at all
- Change of direction = scatter radiation
- Three electrons enter at different distances form the nucleus
- Three photons exit at different directions, different wavelengths
Alternating Electrical Current
- Electricity from the wall is alternating current
- Sine wave (reproducing)
- Start electricity is 0, move up to 110V, moves to 0, moves down to –110V
- Need to boost energy to 1000's of V
- Negative portion of the wave is not useful as it is
- 1/60s is one cycle of the wave
Single Phase, Full Wave Rectified Waveform
- bring negative part of the cycle to the positive part make it useful
- this is done by the rectified waveform
- cut the exposure time in half
- would run it through a transformer to boost it up to 60,000V
- only in the top 30% of the curve is useful
- there is waiting time b/w reaching the top of the curve
- ripple factor—going form max to min—100%
Three phase electrical waveform
- add two more circuits
- as the first phase starting to decline, the next phase would kick in and so forth
- so the ripple factor is b/w 6% and 12%
- similar to what most hospitals have had in the recent past
- have to have a transformer hung on the electric pole outside
- do not want to buy a three phase machine
- came in during the 1950's
6 kHz Medium Frequency Electrical Waveform
- 1985 came about
- no extra transformers on electrical pole
- ripple phase at about 10%
- use single phase electricity
100 kHz High Frequency Electrical Waveform
- 1989
- a switch that turns on and off 100,000 times/sec
- ripple factor about 1%
- claimed dose reduction to pt's
- 20-40% less exposure to pt's that the 6kHz system
Ripple Factor
- single phase—100%
- three phase—10%
- medium frequency—10% (below 40keV)
- high frequency—1% (above 40keV)
X-ray Production
- x-ray emission spectrum, filtered beam kVp (keV) >70
- aluminum filter that is required by law—regulated by FDA
- line begins at 0
- very few Bremsstrahlung released upon people
- the peak largest number of x-rays
- the far right has the peak x-rays
- every thing under the curve is Bremsstrahlung
- the peak to penetrate the pt is Bremsstrahlung
- change in milliamperage, kVp >70
- the average energy of the two peaks is the same
- the only difference is the 400mA has twice as many photons as 200mA
- mA is directly proportional to x-ray photon production
- time is directly proportional to x-ray photon production
- tend to talk about mAs which is directly proportional to x-ray photon production
- change in tube potential
- characteristic is at the same point
- 90kVp is taller—more photons produced—more electrical force
- 90 hits the x-axis further out
- increase in the average energy of 90—a more penetrating beam
- has a darkening effect on the film
- effect of filtration, kVp >70
- reduces low energy radiation, creating less exposure to the pt
- cooper or aluminum as filters
- 2mm Al—thickness of filter
- 4mm Al—less photons, peak shifted to the right, made the beam stronger
mR per mAs
|
KV |
Single phase |
High Freq |
|
50 |
1.13 |
2.50 |
|
60 |
2.00 |
4.40 |
|
70 |
3.09 |
6.00 |
|
80 |
4.05 |
7.90 |
|
90 |
5.33 |
10.00 |
|
100 |
6.88 |
12.50 |
|
110 |
8.5 |
14.7 |
|
120 |
10.1 |
17.50 |
- use the same amount of ??? and
X-ray Properties
- Wilhelm Conrad Roentgen—discovered x-rays by accidents
- Essentially no mass
- No electrical charge—makes them hard to focus
- Travel at the speed of light or not at all
- Can penetrate most matter
- Travel in a straight line until they interact w/matter
- Capable of making certain chemical compounds fluoresce
- Capable of exposing photographic film—but normal photographic film is save to go through x-ray scanners like at airports
- Can change biologic matter by ionization
- Radiation is either electromagnetic or particulate—lots come from the sun
- Alpha and beta are particulate
- X and gamma are electromagnetic
- Part of the electromagnetic spectrum
- Average wavelength of 10-9cm
- Average frequency of 1019hertz
- Average energy of 60,000 electrons volts
Interactions
- classical scattering
- Compton effect
- photoelectric effect
- pair production—will not be tested on
- photodisintegration—will not be tested on
Classical Scatter
- aka coherent or Thompson scattering
- b/w low energy x-ray photon and an atom
- photon changes direction w/o loss of energy
- no ionization
- most scatter forward—towards the film
- may contribute to film fogging—layer of gray on top of anatomy—destroys detail
- do not worry about
Compton Effect
- x-rays are capable of scatter
- noble prize winner
- 1945, St. Louis, chancellor of Wash U
- b/w moderate energy x-ray photons and an outer shell electron—the one's we use
- photon changes direction , loses energy, ionizes atom creating a Compton electron—leaves at reduced energy and at a different directions, the loss of energy is what was needed to remove the electron
- scattered photon may ionize another atom—multiple ionizations
- may cause back-scatter (180°
)—turn back towards the tube
- adds to film fog—measures more than 12cm, need a grid to help capture the scatter (80-90%)
- increases w/increasing kVp
Photoelectric Effect
- b/w moderate energy x-ray photons and an inner shell electron—like a K shell
- photon loses all of its energy (it can no longer go anywhere), ionizes the atom creating a photoelectron—produces the white areas of the film
- produces characteristic x-rays (secondary radiation) in the object being x-rayed—not very strong and can not exit the tissues
- affects smaller atoms like C, O, N, etc
- secondary x-rays behave like scattered x-rays
Differential Absorption
- Compton scattered x-rays contribute no useful information
- adds radiographic density, results in film fog
- structures that absorb a great amount of x-ray are radiopaque—cortex of bone, teeth fillings, etc
- structures that allow x-rays to pass through are radiolucent—calcium, metals
- the bigger the atom, the better the target for the x-ray—oxygen, carbon
- generally less than 5% of x-rays that hit the patient reach the film
- less than half of those interact w/the film to form an image
- therefore approx. 1% of the x-rays emitted from the tube make the image
- maximal differential absorption results from lower kVp values
- but as kVp is lowered pt dose increases
- at lower energies (kVp) the % of photoelectric interactions increases (relative to Compton)
- around 40keV have equal number of interactions
- above 40 have more Compton scatter 85%—15% photoelectric
- to image small differences in soft tissue (renal stone) use low kVp technique (for maximal differential absorption)—make white whiter and background darker—use less kVp
- you can "see" four things radiographically:
- air—blackest
- fat—lighter than air; dark gray; around muscle and such
- water –lighter than fat; lighter gray; muscle, nerve, CSF
- metal—bone; whitest