Grad class notes II Flashcards

1
Q

pulsed dose rate

A

low dose rate, but radiation is delivered for only short part of the hour
-nurse can attend to patient during breaks

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2
Q

BED

A

BED = nd(1+g*d/(alpha/beta))
-g is repair function
-depends on 1/2 time for cell repair and fractionation

-if HDR or EBRT, g = 1

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3
Q

BED for LDR

A

-includes g factor
-BED = Rt[1+(2R/(mu *alpha/beta)) * (1- ((1-e^-mut)/mut))]
t= implant time for each LDR fraction
R= dose rate
mu = ln2/T1/2 (T1/2 is repair time of tissue)

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4
Q

BED for PDR

A

-repair between successive fractions and during the whole fraction

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5
Q

why do we prefer pure gamma emitters in brachy?

A

absence of alpha (don’t penetrate) and beta emissions simplifies geometry and reduces encapsulation thickness required

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6
Q

why do we care about specific activity in brachy?

A

the higher the specific activity, the smaller the source can be
-determines max possible dose rate. Higher dose rates may be desirable to reduce patient treatment times

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7
Q

why do we care about energy of emitted radiation in brachy?

A

-affects tissue penetration
-determines dose distribution
-important for radiation protection

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8
Q

effect of photon energy on absolute dose rate

A

E > 200 keV - all sources have same dose rate constant regardless of medium
E < 100 keV - photoelectric effect results in up to 2-fold heterogeneity corrections (Z dependent)

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9
Q

apparent activity

A

Sk/ (tau * (W/e))

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10
Q

air kerma strength

A

Sk = K * d^2

K is air kerma rate in vaccuo due to photons with energy greater than 5 keV
-cutoff designed to exclude low energy photon-emitting radiation (would not contribute to dose in tissue beyond 0.1 cm but would increase K)

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11
Q

NIST calibration standard for brachy source > 2 mCi

A

-series of graphite cavity ion chambers
-source of unknown strenght is calibrated by intercomparison with the working standard using 2.5 L spherical aluminum ion chamber in air positioned at 1 m

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12
Q

NIST calibration standard for weaker source

A

-WAFAC- directly determine strength of unknown strength source
-Ti characteristic xrays are filtered out

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13
Q

Sk for well-type ion chamber and electrometer

A

Sk = ImassPionpolPtpPelecNsk

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14
Q

difference between TG43 and previous models

A

TG43 uses dose rate constants and other dosimetric parameters that depend on the specific source design, and are directly measured or calculated for each source design

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15
Q

issue with Sv integral

A

only looked at IS law and some attenuation
-did not consider the media

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16
Q

how is dose rate constant determined?

A

-measured or Monte Carlo

17
Q

what does dose rate constant depend on?

A

-internal design of source
-experimental methodology used by primary standard to realize Sk

18
Q

3 things that can cause anisotropy

A

-self filtration
-oblique filtration of primary photons through encapsulating materials
-scattering of photons in the medium

19
Q

dependency of anisotropy factor

A

F decreases as:
-r decreases
-theta goes to 0 or 180 degrees
-encapsulation increases
-photo energy decreases

20
Q

total dose delivered

A

1.44 * T1/2 * initial dose rate

21
Q

other dose limiting structures in manchester technique

A

< 40% of total dose to A can be delivered to ovoids
-rectum and bladder must get less < 80% of dose to pt A

22
Q

where is rectal pt

A

5 mm from most posterior aspect of system/packing

23
Q

where is bladder pt?

A

most inf pt of foley balloon surface

24
Q

why use MR vs CT for brachy planning?

A

MR can differentiate between uterus, periuterine tissues, and tumor whereas CT cannot
-both require special applicators