Test 3 - NCRP 49 Terms Flashcards
(37 cards)
Weekly design exposure rate (limit on exposure on person)
P, unit is in Roentgen
Weekly workload X-ray
W, unit is in mA*min
Weekly workload MV and gamma ray
W, unit is in R, measured at 1 meter from source
Use factor
U. 1 for floor, 1/4 for walls, since most x-rays tubes point downward.
Occupancy factor
T. 1 for commonly occupied spaces, 1/4 for medium, 1/16 for sparsely occupied.
Normalized output
X_n. Exposure per current output. Unit given as R/mA at 1 meter from source.
Exposure rate at 1 m from source of 1. useful beam, 2. leakage radiation, 3. scattered radiation
X’_u, X’_L, X’_s. (primes represent time derivative) Unit given as R/min at 1 meter from source.
Quotient of exposure at 1 m and workload
K_UX. Unit given as R/mA-min at 1 meter from source. Also known as exposure per workload.
Transmission factor for useful beam for 1. x-rays 2. gamma rays 3. leakage x-rays 4. leakage gamma 5. scattered x-ray 6. scattered gamma ray.
B_UX, B_UG, B_LX, B_LG, B_SX, B_SG. Transmission factor
Barrier Thickness 1. primary wall 2. secondary wall
S_p, S_s. Primary wall is the actual irradiated wall for useful beams. Secondary wall is the wall irradiated by leakage and scattered radiations.
Exposure in terms of X’_u and distance d in meters
X = X’_u*t/(d)^2. Since X’_u is defined as exposure rate at 1 meter, d in meter is suffice to obtain true exposure at point of interest.
Solving for B using P, X’_u, t and d.
Since P is what we want to achieve, we can solve for B given the exposure limit, P. P = B * X, and we know X = X’_u * t / d^2. So, P = B * X’_u * t / d^2. Note P = 10 mR/week, as of NCRP 147.
X’_u in terms of X_n, t, and workload W.
X’_u is exposure rate at 1 m. X_n is exposure at 1 m per workload W. Thus X_n * W / t = X’_u.
Solving for B using P, X_n, and workload W.
Since P = B * exposure / d^2, and exposure = X’_n * W (since X’_n is R at 1 meter per workload 1 mA*min), P = B * X_n * W / d^2.
Solving for K_UX given exposure limit P
Since K_UX is exposure / mAmin at 1 meter, K_UX = P * d^2 / W. Why? P is desired exposure at point of interest d meters away. P / W gives exposure per workload. Multiplying by d^2 will give R / mAmin AT 1 METER, or K_UX.
Solving for K_UX with U and T, use factor and occupancy factor.
U and T will give leniency to allowed K_UX (specifically will raise K_UX). This means more workload is needed to reach P, so more leniency. Specifically, K_UX = P * d^2 / WUT.
General equation relating B (transmission factor), X’_n (exposure per workload) to P (exposure limit), d, and WUT in the presence of shielding
K_UX = B*X’_n = P * d^2 / WUT
Note that B is missing if no shielding exists. Note that when one calculates P * d^2 / WUT, the value can be used on a table to search for right lead thickness for acceptable value.
What was NCRP 49? Replaced by what NCRP? What was updated?
Structural shielding design for medical use of x-rays and gamma rays. NCRP 147. Dose limits for medical shielding designs were defined.
NCRP 116 vs ICRP 60 on dose limits
To workers. Annual effective dose limit: 20mSv for both. Cumulative eff. dose: 10mSv x age VS 20mSv in 5 years. Equivalent dose: 150mSv/500mSv lens/rest for both.Dose to public. Eff. dose limit: 1mSv if continuous, 5mSv if infrequent VS 1mSv, higher if needed provided 5yr avg <1mSv/yr. Equivalent dose: 15mSv/50mSv lens/rest for both.
NCRP 49 dose limit (old and defunct)
Derived from ICRP 26 limits by assuming 50 week = 1 working year. So, eff. dose limit for radiation worker is 100mR/wk ~ 1mSv/wk, for public is 10mR/wk ~ 0.1mSv/wk.
NCRP 49 VS 147 x-ray machines occupational/public dose limit?
Occupational: 100mR/wk to 10mR/wk! (1mSv/wk to 0.1)Public: 10mR/wk to 2mR/wk! (0.1mSv/wk to 0.02)
Rotating anode disk ~1930s
Molybdenum disk used. ~3000rpm, ~10000rpm for cineangiography. 6mm x 1.5mm = 9 mm^2 region bombarded with e-, with 1900mm^2 total area bombarded per rotation. Coolant oil in the covering of the tube absorbs infrared light.
Aluminum filter restrictions
Under 50kVp: 0.5mm, 50~70kVp: 1.5mm, above 70: 2.5mm Aluminum.
Beam hardening and effective/equivalent energy
Hardening = higher equivalent energy. Equivalent energy is monoenergetic beam that would go through same attenuation as the spectrum.