On call Flashcards

1
Q

at the unit, patient contour doesn’t jive with body contour

A

-if body too big, dosimetry is ok (just air), but make sure body-generated structures like PTVeval are appropriate
-if body too small, dose distribution will be different

-investigate if setup issue, bowel prep issue etc., immobilization issue

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2
Q

3 P’s

A

check these for each patient
-pregnancy, pacemaker, previous tx

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3
Q

options with pacemakers/defibrillators

A

TG203
Consider:
-assess patient dependency (class 1 is most dependent, class 3 least dependent) and also risk category
-beam energy </= 10MV
-optimize beam geometry
-assess device functional before and after tx, monitor device if required per dependency protocol
-in vivo dosimetry (bolus on top of detector for buildup)
-Be aware of dose limits (use manufacturer limit or use 2 Gy)

-can consider moving pacemaker to other side if cannot get it out of beam path…
-protons and heavy ions also produce neuttrons; electrons produce very few

-MRI effects depend on field strength and imaging conditions

-stereo- higher dose/fraction but potentially less to device given high conformity

-what we measure is the dose to water (not to the actual device, which is typically SiO2)

-lower dose rates are preferred

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4
Q

on exam, don’t ever say yes to treating if machine is out of tolerance
-some people will only tune beam by < 1% with solid water, do full TG51 after hours

A
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5
Q

ways to assess energy

A

-profiler
-PDD10 in solid water

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6
Q

why would machine beam energy drift

A

-problem with target, FF, bend magnet issues (scrubbers that only allow elexctrons at a given energy to pass could be malfunctioning)

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7
Q

hip prosthesis

A

-consider MV image
-contour artifacts (streaks, or starvation)- assign HU value
-even if no obvious streaking in prostat,e likely HU value is wrong
-extent of error depends on how different the HU value is from what it should be
-don’t enter through prosthesis with beam

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8
Q

can we use TPS to assess dose to pacemaker?

A

-only if device is within 3 cm of tx field; or else calc is inccurate
-use specific models like Peridose or Tg36 to calculate dose to device > 3 cm out of field
-for dosed of 50-60 Gy photons, dose should be < 2 GY to device if it is > 5 cm from beam edge, 7 cm for IMRT- use 10 cm for rule of thumb- determine dose with in vivo dosimetry if device 3-10 cm from beam edge
-if non-coplanar beams, use in vivo dosimetry even if d>10 cm

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9
Q

what can be used to measure dose to pacemaker

A

-TLD, OSLD, film, diode, MOSFET, ion chamber

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10
Q

risk levels for pacemaker

A

-dose > 5 Gy or neutron producting therapy = high risk
-dose< 2 Gy and patient is pacing independent- low risk
-otherwise, medium

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11
Q

devices other than pacemakerss that should be considered

A

-chochlear
-epidural pumps
-nerve stimulators

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12
Q
  • Explain how you would go about commissioning IMRT
A

See TG-119: IMRT commissioning with multi-institution comparison. Use phantom studies to verify that treatments can be planned, prepared for treatment, and delivered with sufficient accuracy. Gamma criteria of 3%/3 mm are used. It is common to only analyze pixels with doses > 10% of maximum dose. Alternatively, rectangular ROI may be set to jaw settings. Typically require 95% pass rate (2 sigma confidence interval). Commissioning studies should mimic the types of target and structure geometries and target doses and dose constraints that are likely to be encountered in the clinic.
* -QA MLC leaf positioning and speed
* -E2E
* -anthropomorphic phantom
* IROC
o –use test plans in TG reports for comparison

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13
Q
  • Explain how you would commission VMAT: Because VMAT involves simultaneous use of DMLC and gantry arcing, need to ensure that system is able to properly perform these motions in synchrony, along with dose rate modulation
A
  • -additional QA: output as function of dose rate, gantry angle, profiles for other gantry angles, MLC leaf speed and positioning
  • -E2E, verification plans, anthropomnorchic phantom
  • IROC again
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14
Q
  • Explain process for commissioning and clinical implementation of SRS/SBRT on conventional C-arm linac. What equipment/measurements are required?
A

o Beam measurements with small fields are challenging due to charged particle non-equilibrium, non-negligible detector perturbation effects, enhanced influence of finite source size. Challenges in defining field size.
 Typically stereo commissioning data must go to field sizes smaller than for conventional RT. Extrapolation of commissioning data potentially leads to errors in dose calculation.
 Requires special small field dosimeters
o Some TG-142 QA test tolerances are more stringent (e.g., coincidence of mechanical and radiation isocentres, measured using Winston-Lutz test)
o The commissioning of MLC commonly includes mechanical stability checks [e.g., Winston-Lutz test with MLC defined field, spoke shot], leaf position verification [accuracy/reproducibility using picket fence test, log file analysis], beam data acquisition, leaf transmission, leaf leakage, verification of beam penumbra, and the dynamic leaf gap test [I.e., dynamic picket fence test]
o IGRT system: image quality, isocentricity
o End to end test with anthropomorphic phantom with embedded target to test full workflow including e.g., target localization ability
o TPS may be finer grid- have to commission this as well
o Any additional imaging, motion or immobilization have to be commissioned

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15
Q
  • Explain how to commission a new dose calculation algorithm (e.g., Acuros if you already have AAA)
A

o Can use same commissioning data that was used for original algorithm beam commissioning (there is no reason to remeasure the data).
o Comparison of results from the two algorithms: if new agrees with old and old agrees with measurements that were done originally, then new agrees with measurements (there is no reason to redo measurements)
o Use measurements (e.g., with film in anthropomorphic phantom) or Monte Carlo to investigate cases where they disagree

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16
Q
  • Give example situations where you would and would not include skin in the evaluation structure.
A

o Want to include skin in evaluation structure if the intent is to treat the skin, and in these cases you would want to use e.g., MV photons with bolus, kV photons or MV electrons.
o Example where bolus is typically used: post-mastectomy chest wall radiotherapy

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17
Q
  • You are called to a treatment unit where you determine that the kV imaging system is not functioning properly and your service personnel inform you that they can’t fix it until parts arrive tomorrow. Should you take the machine out of service in such a scenario? Discuss the reasons for you choice.
A

o Yes, kV system needed for IGRT. No substitute for this exists. Even if MV imaging system is available (EPID), there is much less soft tissue contrast so this is not a reliable substitute.

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18
Q
  • Compare and contrast the plan QA methodology when checking a cranial, single fraction, stereotactic plan and a cranial 3D conformal plan.
A

o Rx to 100% for conventional. Typically prescribe to lower value isodose for stereotactic (so that dose fall off outside of target it faster).
o Dose calculation grid and CT sim voxel sizes smaller for stereotactic.
o Stereotactic typically requires multiple non-coplanar arcs or beams.
o OAR tolerance doses are much lower for stereotactic due to hypofractionation.
o Patient immobilization equipment more stringent for stereo. Need thermoplastic mask plus IGRT or head frame for SRS.
o FFF beam likely appropriate for SRS.
o Arc type needs to be “SRS” to allow for more MU per arc.

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19
Q
  • A patient has lost weight during the course of their head and neck treatment and their mask no longer fits. The oncologist has ordered a new mask and CT scan for the patient and would like to continue treating with the current plan until a new plan is ready. He has contacted you to determine the dosimetric implications of this. Describe what you would do in this scenario to help the oncologist make his decision.
A

o Discuss potential for intra-fraction motion given that mask is now too loose.
o Can deform planning CT to match daily treatment CBCT (use extended range CBCT ideally). Then recalc current plan on deformed CT to assess dosimetric implications. Discuss with RO, noting that deformed contours may not be accurate (don’t just blindly look at DVHs). Tell RO that they must assess accuracy of deformed contours, image registration and dose distribution.

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20
Q
  • Patient abdomen body contour consistently smaller than it was at CT sim. RO asks for help deciding how to proceed. What do you do?
A

o Follow same procedure as point #2 above.
o Assess whether it is weight loss or gas.
 Can argue that gas won’t be a problem since amount of tissue traversed by beam is unchanged. This is valid as long as the gas is not directly adjacent to target.
o Assess patient setup (have they been setup wrong, with a rotation)
o Assess beam entry points. Contour change that does not occur at beam entry point is generally less of an issue.

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21
Q
  • You are called to the treatment unit because a patient being treated with a 6MV POP, 10x10cm field (has lost weight – separation has changed from 30cm to 25cm). What do you advise? Would your advice change if this were an ENT IMRT patient (determined from CBCT that external has shrunk by 1cm near tumour)?
A

1 cm change vs 5 cm is significant

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22
Q
  • The dosimetrist calls you with a patient who has bilateral hip replacement as seen on a CT scan. The physician wants to treat the pelvis with a standard 4-field beam arrangement. What advice would you give the dosimetrist in the case?
A

o Consider acquiring planning CT with higher energy beam, if available (e.g., MV CBCT using EPID, tomotherapy)
o Regions of artefact (e.g., dark streaks) that are outside of prostheses resulting in non-representative HU values should be contoured and set to HU=0 (assuming water equivalent region is more appropriate than streaky artefacts).
o Instead of ant/post/right/left beams, should use oblique beams that avoid entering or exiting through prostheses since this may result in strong attenuation and may not be properly modelled in TPS.

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23
Q
  • Create a plan QA checklist for standard 2 field tangent-breast technique.
A

 Check that there is 2 cm flash.
 Isocentre should be near chest wall-lung interface to minimize divergence into lung.
 Check documentation to see if it is a breath hold patient (for left sided treatments). If so, this should be indicated appropriately (for example in the plan name, consistent across all documents, etc.)
 Arms should be above head using breast board immobilization equipment (unless particular reason why patient can’t do this)
 In evaluating treatment plan, look for intensity modulation using FiF technique or wedges.
-location of norm point
-hot spots acceptable
-coverage
-dose to OARs, don’t enter through contra breast
-lung < 2 cm in field
-no heart in field

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24
Q
  • A large patient, being simulated for a right breast treatment, undergoes a CT scan and her anatomy does not fit within the standard 50 cm field-of-view. The patient has missing anatomy on both the right and left sides. The therapists call you for advice; describe what options you have at the CT simulator in this case.
A

o Breast typically treated using partial arcs or tangents so beam enter/exit on one side. So it is more desirable to have more missing anatomy on the not treated side than a smaller amount of missing anatomy on both sides (which will have a larger clinical impact in terms of calculating dose accurately). Therefore, shift patient so that right breast (being treated) is closer to centre of CT bore [this means user origin closer to right breast I think].
o Otherwise could manually add in extrapolated contours set to HU=0 where there is missing tissue. However, this is an approximation since don’t actually know where body contour is and won’t be able to account for heterogeneities.

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25
Q
  • List pros and cons of MR sim (see III.73)
A

o Pros: potentially more accurate target contouring due to improved soft tissue contrast, treatment planning for MV photons not strongly affected by small changes in HU (so requirements for synthetic CT are not particularly onerous), only one sim appointment instead of two in cases where MRI would be requested by the RO anyway.
o Cons: synthetic CT generation may run into issues with tissues that have similar MR signals but different HU values and therefore different x-ray attenuation properties. Unlike x-ray CT, MRI is prone to geometric distortion due to e.g., susceptibility artefacts

26
Q
  • What is the most common PET radiotracer? What is its half life? Why do you use PET in radiation oncology?
A

o Fluorodeoxyglucose (FDG); half-life = 110 minutes
o FDG is a glucose analog, which has more uptake in metabolically active cells such as cancer cells. This is helpful for localizing the target, for identifying lymph node involvement and for finding distant metastases.

27
Q
  • Refer to image: 3-field rectum plan and the 95% isodose is not covering the PTV. What would you do to get coverage?
A

increase weighing of PA beam and use wedges

28
Q
  • Common field arrangements:
A

o Wedged pair: Two beams with wedges are used to achieve a trapezoid shaped high dose region. Useful for relatively low lying lesions e.g., thyroid
 The optimum relationship between the wedge angle theta and the hinge angle phi which provides the most uniform dose distribution in the overlap region: theta = 90 – phi/2.
 See wedged fields examples in treatment planning notes
o Four-field box: four beams (two opposing pairs at right angles) producing a relatively high dose box shaped region. Useful for central lesions in the pelvis (e.g., prostate, bladder, uterus).
 Having opposing pairs at angles other than 90 degrees results in rhombic (not square) shape high dose region.
o Three field box: similar to four field box but for lesions that are closer to the surface (e.g., rectum). Wedges are used in the two opposed beams to compensate for the dose gradient in the third beam.

29
Q
  • In the context of electron therapy, define the obliquity factor:
A

o Obliquity factor OBF = dose (measured at depth d along CAX in oblique case) / dose (beam perpendicular to surface, same depth along CAX)…. i.e., depth is measured along CAX for each beam
 OBF always > 1
 OBF increases with increasing angle of obliquity, increasing more drastically for lower energies initially (due to more scatter, and larger scattering angles)
 OBF reaches a higher maximum for higher energy beams.
 OBF reaches a max around 75 degrees (this is the angle between incident beam and a line perpendicular to the surface), then starts decreasing again [I think because some of the lateral scatter starts exiting the patient at a certain point, leading to a decreased surface dose].

30
Q
  • Your physics department has decided to decommission physical wedges. What are the alternatives for clinic? What are the advantages and disadvantages of this decision?
A

o Uses of wedges:
 Compensate for missing tissue/sloping surface
 To treat lesion near surface using two beams incident obliquely.
* Optimal wedge angle = 90˚ - ½ (hinge angle). However, if surface is curved then wedge angle may need to be even higher to compensate for this.
o Alternative: use field-in-field technique (forward planned) or IMRT (step and shoot SMLC or sliding window DMLC; inverse planned)

31
Q
  • ***What is the rationale for per-patient dose verification for IMRT and VMAT? What are the options with regard to measurement or calculation methods? What are acceptable tolerances? What would your action be if a measurement was out of tolerance compared to the treatment plan?
A

o WHY: Patient-specific dose verification is needed to ensure (1) that the plan has properly transferred from the treatment planning system to the treatment delivery system (less important in the paperless era where manual data input from TPS to TCS is not required), (2) to ensure that the plan is deliverable and (3) to ensure that the TPS is calculating the dose properly (especially important for small fields or highly modulated plans). Can catch errors such as field symmetry/flatness, MLC errors, monitor chamber end effect.
o HOW: This can be done (1) using portal dosimetry (EPID), (2) using 2D OR 3D detector array (e.g., Octavius, Matrixx – both of these are 2D arrays; ArcCHECK is a 4D array which “measures and correlates gantry angle, leaf-end position, absolute dose and time to identify any potential source of error throughout the patient volume”), (3) with film and ion chamber in solid water phantom.
 EPID will not detect gantry sag – however, EPID doesn’t require phantom setup and is typically fully integrated with ROIS
 When choosing commercial detector arrays, must pay attention to resolution, especially for stereotactic plans

32
Q
  • A physician wishes to use in 18 MeV electron beam and an electron cut out of 4 x 4 cm2 to treat a 3 cm diameter area extending from the surface to a depth of 6 cm. The dose is prescribed to the 80% isodose line. Are there any issues with this treatment?
A

o Using {2,3,4,5} rule, {R100, R90, R50, Rp} = {3.6, 5.4, 7.2, 9} cm
 Also R80 [cm] ~ E [MeV] / 3 = 6 cm so choice of energy is appropriate at first glance
o ISSUES WITH SMALL ELECTRON FIELDS: Rule of thumb states that if FS < Rp, the lateral scatter equilibrium does not exist on CAX – dmax, R90 (therapeutic range) and R80 decrease from values expected with larger FS according to {2,3,4,5} rule, dose fall off is less steep (Rp unaffected because is determined by max beam energy), surface dose increases relative to dmax, flatness of the beam profile compromised
 So target may not actually be covered by desired dose level.
 Flatness compromised: lateral constriction of high value isodose curves especially with deeper depths, small FS and higher energies means that lateral edges of target may not be well covered.
o Should measure actual output factor for this cutout due to issues described above.
o At dmax, Generally the 20%–80% width is expected to be 10 mm to 12 mm for electron beams below 10 MeV, and 8 mm to 10 mm for electron beams between 10 MeV and 20 MeV (smaller penumbra for higher energy because higher energy electrons more forward directed). So the choice of field size is appropriate, given size of penumbra.
o What would be the approximate depth of the practical range for this beam? Rp unaffected by FS, is determined by nominal energy of beam so is 9 cm
o What is the approximate dose of the skin? Rule of thumb: Dsurface ~ 76% + E [MeV] = 94% and may be even higher due to small FS
o What are other options? Orthovoltage photons, surface brachytherapy (although 6 cm depth may be challenging to treat while maintaining acceptable skin dose with these techniques).

33
Q
  • How are wedge angles defined?
A

o The angle between the isodose line and a line perpendicular to the CAX. ICRU recommends specifying this at a depth of 10 cm. So, without a wedge, this angle is ZERO.
o Due to beam hardening and the presence of scattered radiation at shallower depths, the angle of isodose tilt will decrease with increasing depth in the phantom (wedge becomes less effective at tilting isodose lines due to beam hardening).

34
Q
  • List the relevant commissioning data that must be collected for a physical wedge?
A

o PDDs, beam profiles (verify wedge angle; need to measure both crossline and inline), wedge factors
 Various field sizes, depths
o Also check interlocks are functional
o Typically determine wedge factors for one FS and depth. However, may be a function of FS and depth and should do more extensive measurements (e.g., for the purpose of empirical, correction-based MU calculations)

35
Q
  • How is the commissioning process different for a soft/dynamic wedge compared to a hard/physical wedge?
A

 Each data point must consist of measurement integrated over the entire jaw sequence, 2D detector array or film is recommended for measuring transverse beam profiles.
* Consider using detector array that can be mounted on the scanning arm or use detector array with solid water slabs or can use film sandwiched between solid water slabs.
 For dynamic wedges, you must check a variety of different wedge angles. The same is also true for a universal wedge that is combined with open fields to yield different effective wedge factors.
 For dynamic wedge, verify that jaws move at the correct speed throughout their entire motion, which should be smooth and reproducible [use log files for this?]
 For hard wedge, must also ensure functionality of interlocks to ensure hard wedge is in place for treatment.

36
Q
  • How do you check if wedges are centered properly?
A
  • First, ensure that chamber is on CAX (on collimator rotation axis): take measurements at two collimator angles 180 degrees apart – adjust chamber position until readings are equal within 1%. X and Y jaws are at different heights so expect different readings at different collimator angles if chamber not centred.
  • Once chamber is centred, repeat measurement with wedge (not collimator) rotated through 180 degrees. Reading should differ by <5% for 60˚ wedge and <2 % for a 30 degree wedge. Larger discrepancies may indicate that the side rails are not symmetric about the CAX. Take average of the 2.
37
Q
  • How do you determine the position of water surface when setting up ion chamber in water tank?
A

o The reflection method: chamber and its reflection in water should form circle for cylindrical chamber with long axis parallel to water surface.
 Pros: easy to understand, requires no specialized equipment
 Cons: inherently qualitative, susceptible to inconsistencies between users and measurement setup. TG-51 addendum estimates that this method results in 0.33-0.5 mm uncertainty

38
Q
  • What if the DVHs for a critical structure from two competing plans cross? Which would you select and why?.
A

depends on if parrallel vs serial organ

39
Q
  • How to decrease skin dose to patient treated with blocks using high energy photon beam?
A

o First of all, what is a block? Shielding blocks are used to protect normal critical structures within the irradiated area. For MV beams, these blocks are supported on a plastic tray and have a particular position within the radiation field. They can be custom made for particular patient using lead or cerrobend. For ortho/superficial, they can be made much thinner (few mm Pb) and can be placed directly on patient skin. For electrons, mm Pb ~ energy [MeV] / 2.
o They add additional scatter & electron contamination so want to position far enough away (a few cm at least?) to allow this contamination to escape laterally
o For ortho/superficial, it is common to cover lead shields for e.g., nostril in low Z material such as wax to absorb low energy backscatter toward skin.

40
Q

what to do for each risk case for pacemaker

A
  • What to do in each risk case:
    o LOW RISK
     Resuscitation protocol and associate equipment available
     Close audio-visual monitoring of patient
     Communicate with cardiology/electrophysiology: for ICD, can tachycardia function be temporarily turned off for Tx delivery (this will inhibit defibrillator ability)? - must turn back on after Tx delivered. Placing a magnet over an ICD will cause it to turn off [fully; no defib ability or pacing]. Placing a magnet over an ICP will cause it to pace at a constant rate so that it cannot be affected by the radiation. (note that only pacing independent with dose < 2 Gy are low risk)
     CIED interrogation before fraction #1 and after last fraction.
    o MEDIUM RISK
     Same as above, plus:
     Formal consult with cardiology/electrophysiology. If pacing dependent, consult on use of magnet, pulse oximetry
     Need cardiac support available in case of malfunction.
     CIED technician to interrogate device mid-Tx
     Evaluate at 1 and 6 months after treatment
    o HIGH RISK
     Same as above, plus:
     ECG weekly, examined by trained staff
     Interrogate device weekly
     Appropriate technologist available if needed.
    o Emergency response equipment available
     Crash cart including CPR devices
     ECG
     Pacemaker magnet, pulse oximetry, AED
     Temporary transcutaneous pacing and staff trained in its use
41
Q
  • How to take into account delay in treatment? (e.g., BED equation with proliferation term) What are the assumptions/limitations of this approach?
A

o Use the linear quadratic concept to calculate effective doses in radiotherapy (page 404 of Hall & Giaccia)
o Biological effect E = -ln(S)
o Biologically effective dose (BED) = E/alpha
o Can add in term to account for tumour proliferation, assuming exponential growth with potential doubling time Tpot: (ln(2) = 0.693)
 Where t is the time available for proliferation. Rapid proliferation in tumours appears not to start up until about 21 to 28 days after treatment begins in H&N tumour. Therefore, t = T – 21 or 28 where T is the overall time. I.e., t = T – Tk where Tk is the kick-off time.
o Assumptions/limitations:
 Tumour profileration is assumed to follow simple exponential growth model when in reality, tumour cell proliferation is a complex process affected by many factors.
 There is uncertainty associated with all parameters. These parameters vary from tissue to tissue and from person to person.
 This model does not take into account redistribution of cells throughout the cell cycle as time progresses, nor does it account for reoxygenation.

42
Q

kV vs MV image for reference

A
43
Q

dose from MV and kV image

A

1-2 cGy for MV
0.1 cGy for kV

44
Q

o Do image doses need to be included in your plan? Assuming conventional fractionation, typical dose per fraction is 2 Gy = 200 cGy so imaging dose account for ~1% of delivered dose which is < 5% threshold given in TG-180. KV imaging doses are ~ an order of magnitude lower and are also typically ignored.

A

 TG-180: It is recommended that imaging dose be considered part of the total dose at the treatment planning stage if the dose from repeated imaging procedures is expected to exceed 5% of the prescribed target dose.
* For 2 Gy per fraction, 5% corresponds to 10 cGy = 100 mGy, so MV CBCT organ doses should be taken into account in planning

45
Q

wrong couch in plan

A

thick or thin vs med is < 0.5% difference for PA beam
thick vs thin is > 1 % difference for PA beam

46
Q

treating bone in rad calc

A

-can set target density to ~ 1.2- accounts for higher density of the bone

47
Q

tricks for scenario questions

A

-go over consequences and potential causes
-don’t assume a certain scenario=- ask questions-
-check for trends
-refer to institutional guidelines (ex. CBCT match structure fails triggers a physics warning that triggers velocity assessment versus just using a hunch)
-refer to AAPM/CPRQ tresholds if relevant

48
Q

plan was calculated on MIP insted of ave

A

lung volume would be smaller and higher density
likely need to replan
MIP is max CT value of all phases at that slice position

49
Q

4DCT has phase errors can you use it?

A

assess where artifacts are
if it is upper lobe and artifacts are lower, could potentially use it
same with laterality

50
Q

physician/planner realize that CTSim wasn’t inf enough

A

how close is the target volume to the edge of the FOV? Potentially can extrapolate the final slice to provide more scatter volume. Can set HU to -1000 vs bone vs water to see what effect the HU has on the target dose distrubituon and if a re-sim is necessary. Typically a few cm of buildup is sufficient. penumbra 80/20 at 6 MV for depth is about 7 mm.

51
Q

what kind of gamma error would you expect if dark field calibration is off?

A

failing at low dose, at edges of target

52
Q

for gamma test portal verification, what plan is the baseline?

A

the calculated plan

53
Q

issue with not cropping PTV from skin

A

no build-up or scatter
-TPS may compensate by introdcing more fluence
-high dose gradient at skin
-with weight loss, could also get high dose gradient inside tissue

54
Q

CONSIDERATIONS FOR A BARIATRIC LUNG PATIENT

A
  1. assess RT vs chemo
  2. consider weight limit for couch and QA to do afterwards (400-500 lb)
  3. see if patient can lose weight (maybe chemo done earlier to help lose weight)
  4. mobility
  5. if patient is touching CT bore, that tissues will be spilling out at tx
  6. issueds with noisy image and photon starvation- higher mAs, higher kV
  7. -higher mAs might mean time needed for tube to cool- scan may take longer
  8. worse artifacts especially since cupping artifact correction etrc is done for standard size patient
  9. using another kV- HU/RED curve may not be accurate- consider range of HU accuracy for curve and also getting 2 scans- one for contours and one for calcs
  10. consider beam entry points at TP. May have to contour outser patient anatomy based on physical measurement (may not have choice)- can test a different range of outer contours and assess sensitivity of plan. Avoiding entering through missing tissue, avoid artifacts, contour artifacts
  11. consider high E - but more inhomogeneity and interface effects (but higher E is hotter hot spot)
  12. couch deflection at CT may be diffeernt than that at tx (saf and deflection)- 6 DOF could help
  13. IGRT image may be extremely poor quality- spotlight image (high mAs and small FOV) could help
  14. clearance, trouble positioning patient
55
Q

what could be the cause of an bump on the prostate PTV?

A

ditzel!

56
Q

activated breathing control

A

The patient breathes through a mouth-piece connected to the ABC apparatus. The respiratory signal is processed continuously, using a personal computer that displays the changing lung volume in real-time. After the patient’s breathing pattern becomes stable, the operator activates ABC at a preselected phase in the breathing cycle. Both valves are then closed to immobilize breathing motion

57
Q

collimator star shot fails- why?

A

jaws are miscalibrated
try using asymmetric jaws so crosshair is at center of field and see if it passes

58
Q

what could happen if light in iX is offset?

A

could get a light field that reverses with collimator rotation

59
Q

colli rotation is perfect but collimator has walkout- what is the cause?

A

mylar in the wrong place

60
Q

how to tell gantry star shot from collimator starshot

A

gantry starshot will see beam divergence and attenuation through the film

61
Q

how to tell gantry star shot from collimator starshot

A

gantry starshot will see beam divergence and attenuation through the film

62
Q

you see a 72% normalization factor for VMAT- course pf action

A

-where did 72% come from (i.e. glasgow incident)- likely doc changed Rx
-ensure plan is deliverable on machine

used to be an issue with sliding window IMRT because sliding window was designed so that at last leaf is moving at max speed. Therefore with scaling, other leaves couldn’t keep up