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INTRODUCTION OF
CO -60 UNIT
NILESH KUMAR
PG RADIATION PHYSICS
DEPARTMENT OF RADIATION PHYSICS
• Overview
Radionuclide's such as radium-226, cesium-137, and cobalt-60 have been
used as sources of gamma rays for teletherapy.
These gamma rays are emitted from the radionuclide's as they undergo
radioactive disintegration.
Of all the radionuclide's, Co-60 has proved to be the most suitable for
external beam radiotherapy.
The reasons for its choice over radium and cesium are higher
possible specific activity (curies per gram), greater radiation
output per curie, and higher average photon energy .
 A typical source activities are in the order of 5000-10,000 ci and provide
typical dose rate at 80 cm from the teletherapy source of the order of 100-
200 cGy/min.
 often the output of teletherapy machine is started in Rmm ( roentgen per
minute at 1 m ) as a rough guide for source strength .
 Treatment head has the capacity to take a source with an activity of
10,000 roentgens per hour at a meter ( RHm ) .
 COBALT-60 UNIT
Source
 The 60Co source, usually in the form of a solid cylinder, disks, or pallets, is
contained inside a stainless-steel capsule and sealed by welding.
 This capsule is placed into another steel capsule which is again sealed by
welding.
 The double-welded seal is necessary to prevent any leakage of the
radioactive material.
 The Co-60 source decays to Ni-60 with the emission of β particles (Emax = 0.32
MeV) and two photons per disintegration of energies 1.17 and 1.33 MeV.
 These gamma rays constitute the useful treatment beam.
 The β particles are absorbed in the cobalt metal and the stainless-steel capsules
resulting in the emission of bremsstrahlung x-rays and a small amount of
characteristic x-rays.
 A typical teletherapy 60Co source is a cylinder of diameter ranging from 1.0 to 2.0
cm and is positioned in the cobalt unit with its circular end facing the patient
 Source Housing / source head
 It consists of a steel shell filled with lead for shielding purposes and a device
for bringing the source in front of an opening in the head from which the
useful beam emerges.
 a heavy metal alloy sleeve is provided to form an additional primary shield
when the source is in the off position.
 A number of methods have been developed for moving the source from the
off position to the on position.
 These methods are -:
I. Rotating wheel
II. Sliding drawer
III. mercury shutter
IV. moving jaw
 Rotating wheel
 The source mounted on a
rotating wheel inside the
sourcehead to carry the source
from the off position to the on
position.
 Sliding drawer
A pneumatically driven source
drawer is used for moving the
source between shielded
position and treatment position.
The pneumatic cylinder will
return the sourceautomatically
to radiation-off position in case
of any failure.
 Mercury shutter
 mercury is allowed to flow into
the space immediately below
the source to shut off the beam.
 Moving jaw
 The source is fixed in front of the
aperture and the beam can be
turned on and off by a shutter
consisting of heavy metal jaws.
 Beam Collimation
 The size and orientation of the radiation beam is controlled by the collimator
assembly.
 Two pairs of motorized jaws generate rectangular and square field of desired
size.
 The collimator can also be rotated around the radiation beam axis.
 The radiation field can be visualized by a high intensity light during patient
positioning
 The centre of the radiation field
is indicated by the collimator
cross hairs.
 Two sets of trimmers are
provided to decrease the
penumbra of the beam.
 The lower pad of the collimator
is prepared to receive wedge
filters and shadow tray for the
beam shaping lead blocks.
 Penumbra
 Penumbra refers the region at the edge of beam where dose rate changes
rapidly as function of distance from beam axis.
Types of penumbra :
Geometric
Transmission
 Transmission penumbra
• It is the region irradiated by photons which are transmitted through the
edge of the collimator blocks
 Geometrical penumbra :
 formula =
• it is formed due to dimension of source.
• It is formed due to finite source size and must be concern in teletherapy
machines where the sources is between 1 – 2 cm in size.
 Conclusions :
 penumbra increases with increase in source diameter , SSD , and depth.
Penumbra width decreases with a increase in SDD
penumbra trimmers - :
 it consists of extensible , heavy metal bars to attenuate the beam in the
penumbra region.
 increase the source to diaphragm distance , reducing the geometric
penumbra.
 Gantry
 The gantry can rotate by 360°. The rotational movement of the gantry is
motorized and controlled in two directions continuously; its rotation speed
can be adjusted.
 Teletherapy machines are most often mounted isocentrically, allowing the
beam to rotate about the patient at a fixed SAD. They can be used either as
fixed field machines or rotation units.
 Most cobalt-60 unit machines have SAD of 80 cm.
 The axis of rotation of the three structures:
Gantry
Collimator
Couch
coincide at a point known as the Isocenter.
Isocentric Mounting
 Enhances accuracy.
 Allows faster setup and is more accurate than older non isocentrically
mounted machines.
 Makes setup transfer easy from the simulator to the treatment machine
 Patient Support Assembly / Couch
 Treatment Bed has motorized movements
 Horizontal
 Vertical
 . Lateral.
 Table Top - 90°rotation to each side
 Base - 90° rotation to each side
 Control Console
 Control Console is situated outside the bunker
 Interlocks present on the console for- :
Air Pressure
 Door
Head Lock -Treatment Head has a swivel movement of +/- 180°.
 OFF Shield
 Treatment Mode.
 Wedge Filter.
Tray Interlock.
 Timer
 Timer
 The prescribed target dose is delivered with the help of two treatment
timers -:
 primary timer - the primary timer actually controls the treatment time.
 secondary timer - accounts for the source movement from OFF to ON
position and agin to OFF position ( shutter time )
 Formula of shutter time =
 where , R1 - meter reading for given time ( say 2 min )
R2 - Meter reading for two consecutive times ( 1+1 min )
eg - :
Meter reading
+ 300 v
Time 1 min
MR 1 MR 2 Mean
36.15 nc 36.14 nc 36.145 nc
 Warning lights
• Red light: Radiation present- do not enter room
• Green Light: time elapsed
• Malfunction: both red and green lights still on- means that machine is still
in on position after prescribed dose has been delivered. Remove patient.
 Beam shaping and modifying devices
 The system has accessories like -:
wedge filters
Breast cone
Sheilding blocks, to modify the beam shape or beam attenuation.
 They are placed on the machine between the collimator and the patient.
 wedge filters
 special filters or absorbing blocks are placed in the path of a beam to
modify its isodose distribution.
 The most commonly used beam-modifying device is the wedge filter.
 This is a wedge-shaped absorber that causes a progressive decrease in the
intensity across the beam, resulting in a tilt of the isodose curves from their
normal positions.
 the isodose curves are tilted
toward the thin end, and the
degree of tilt depends on the slope
of the wedge filter.
 In actual wedge filter design, the
sloping surface is made either
straight or sigmoid in shape .
 The wedge is usually made of a dense material, such as lead or steel, and is
mounted on a transparent plastic tray,
 which can be inserted in the beam at a specified distance from the source .
 This distance is arranged such that the wedge tray is always at a distance of at
least 15 cm from the skin surface,
so as to avoid destroying the skin-sparing effect of the megavoltage beam.
 Wedge Systems
 Wedge filters are of two main types -:
I. individualized wedge system,
 which requires a separate wedge for each beam width, optimally designed
to minimize the loss of beam output.
 A mechanism is provided to align the thin end of the wedge with the border
of the light field
2 . The second system uses a universal wedge -:
 a single wedge serves for all beam widths.
 Such a filter is fixed centrally in the beam, while the field can be opened to
any size.
 only a small part of this wedge is effective in producing the given wedge
angle.
 The rest, being unwedged, does not contribute to the isodose tilt but
reduces the beam intensity .
 the individualized system reducing the beam output, it is preferred for use
in cobalt teletherapy.
 The universal wedge, is useful for linear accelerator beams where the
output is more.
 From the setup and treatment planning points of view, the universal wedge
is simpler to use than the individualized filter.
 Effect on Beam Quality
 The wedge filter alters the beam quality by preferentially attenuating the lower-
energy photons (beam hardening)
 to a lesser extent, by Compton scattering, which results in energy degradation (beam
softening).
 For the 60Co beam, because the primary beam is essentially monoenergetic, the
presence of the wedge filter does not alter the central axis percent depth dose
distribution.
 For x-rays, on the other hand, there can be some beam hardening , and as a result
the depth dose distribution can be somewhat altered, especially at large depths
 Breast Cone
 A beam modifying and directing device used for a tangential fields therapy
 Advantages: –
 Directs beam to the central axis of the area of interest, where a tangential beam is
applied to a curved surface
 Helps position, the patient with an accurate SSD
 Endplate provides compensation,
 which enhances surface dose and presses down the tissue.
 Effective shielding of lungs
 SHIELDING BLOCKS
 Aims of shielding-
 protect critical structures ( organ )
 avoid unnecessary radiation to normal tissues
 matching adjacent fields
 An ideal shielding material should have the following characteristics :
 high atomic no
 high density
 easily available
 inexpensive
 easily modifiable
 The most commonly used shielding material for photons is Lead ( Pb )
The thickness of shielding block used depends upon the energy of the
radiation
The shielding material which reduces beam transmission to 5% of its original is
considered acceptable .
The term half value layer is an expression for the attenuation produced by any
material.
half-value layer (HVL) is defined as the thickness of an absorber of specified
composition required to attenuate the intensity of the beam to half its original
value.
Practically thickness of lead between 4.5 – 5 half value layers which results in
5% or less of primary beam transmission.
 Custom blocks
• The conformal blocks are made with low melting point alloy called Cerrobend.
• The Cerrobend material consists of 50.0% bismuth, 26.7% lead, 13.3% tin, and 10.0%
cadmium .
• The main advantage of Cerrobend over lead is that it melts at about 70 °C (compared with
327 °C for lead) and therefore, can be easily cast into any shape.
• At room temperature, it is harder than lead.
• The minimum thickness of Cerrobend blocks required for blocking may be calculated from
Table 13.1 using its density ratio relative to lead (e.g., multiply lead thickness by 1.21).
 Placing of shielding material
 In kilovoltage radiation shielding is readily achieved by placing sheets of lead on
the surface directly
 It is because of the lower penetrating power of beam
 In megavoltage radiation,
Thicker blocks used.
Placed higher up in shadows trays (15-20cm )
 T - ROD mechanism in cobalt-60 unit
 The external T-ROD shall be fitted with this indicator rod incase of failure of
Automatic source retracting system to push the source to the OFF condition.
 Source stuck during treatment – Emergency situation when the Cobalt-60
source gets stuck in between the “off” and “on” position .
 Rotate gantry to side opposite to maze wall – Insert “T-rod” and push it till the
source reaches “safe” position
 The beamstopper
 The beamstopper is a lead-filled steel assembly, which acts as a beam
absorber. The beamstopper attenuates 99.9% of the primary beam.
 A beam stopper is used to intercept the beam for additional shielding of the
exit beam. The beam stop also acts as a counterweight for the head of the
machine.
 References -:
I. KHAN’S The Physics of Radiation Therapy
II. Radiation Oncology Physics: E.B. Podgorsak
III. Article - BARC DEVELOPS COBALT-60 TELETHERAPY MACHINE FOR CANCER TREATMENT
Intro of co 60 unit

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Intro of co 60 unit

  • 1. INTRODUCTION OF CO -60 UNIT NILESH KUMAR PG RADIATION PHYSICS DEPARTMENT OF RADIATION PHYSICS
  • 2. • Overview Radionuclide's such as radium-226, cesium-137, and cobalt-60 have been used as sources of gamma rays for teletherapy. These gamma rays are emitted from the radionuclide's as they undergo radioactive disintegration. Of all the radionuclide's, Co-60 has proved to be the most suitable for external beam radiotherapy.
  • 3. The reasons for its choice over radium and cesium are higher possible specific activity (curies per gram), greater radiation output per curie, and higher average photon energy .
  • 4.
  • 5.  A typical source activities are in the order of 5000-10,000 ci and provide typical dose rate at 80 cm from the teletherapy source of the order of 100- 200 cGy/min.  often the output of teletherapy machine is started in Rmm ( roentgen per minute at 1 m ) as a rough guide for source strength .  Treatment head has the capacity to take a source with an activity of 10,000 roentgens per hour at a meter ( RHm ) .
  • 6.
  • 7.  COBALT-60 UNIT Source  The 60Co source, usually in the form of a solid cylinder, disks, or pallets, is contained inside a stainless-steel capsule and sealed by welding.  This capsule is placed into another steel capsule which is again sealed by welding.  The double-welded seal is necessary to prevent any leakage of the radioactive material.
  • 8.
  • 9.  The Co-60 source decays to Ni-60 with the emission of β particles (Emax = 0.32 MeV) and two photons per disintegration of energies 1.17 and 1.33 MeV.  These gamma rays constitute the useful treatment beam.  The β particles are absorbed in the cobalt metal and the stainless-steel capsules resulting in the emission of bremsstrahlung x-rays and a small amount of characteristic x-rays.  A typical teletherapy 60Co source is a cylinder of diameter ranging from 1.0 to 2.0 cm and is positioned in the cobalt unit with its circular end facing the patient
  • 10.
  • 11.  Source Housing / source head  It consists of a steel shell filled with lead for shielding purposes and a device for bringing the source in front of an opening in the head from which the useful beam emerges.  a heavy metal alloy sleeve is provided to form an additional primary shield when the source is in the off position.
  • 12.  A number of methods have been developed for moving the source from the off position to the on position.  These methods are -: I. Rotating wheel II. Sliding drawer III. mercury shutter IV. moving jaw
  • 13.  Rotating wheel  The source mounted on a rotating wheel inside the sourcehead to carry the source from the off position to the on position.
  • 14.  Sliding drawer A pneumatically driven source drawer is used for moving the source between shielded position and treatment position. The pneumatic cylinder will return the sourceautomatically to radiation-off position in case of any failure.
  • 15.  Mercury shutter  mercury is allowed to flow into the space immediately below the source to shut off the beam.
  • 16.  Moving jaw  The source is fixed in front of the aperture and the beam can be turned on and off by a shutter consisting of heavy metal jaws.
  • 17.  Beam Collimation  The size and orientation of the radiation beam is controlled by the collimator assembly.  Two pairs of motorized jaws generate rectangular and square field of desired size.  The collimator can also be rotated around the radiation beam axis.  The radiation field can be visualized by a high intensity light during patient positioning
  • 18.  The centre of the radiation field is indicated by the collimator cross hairs.  Two sets of trimmers are provided to decrease the penumbra of the beam.  The lower pad of the collimator is prepared to receive wedge filters and shadow tray for the beam shaping lead blocks.
  • 19.  Penumbra  Penumbra refers the region at the edge of beam where dose rate changes rapidly as function of distance from beam axis. Types of penumbra : Geometric Transmission
  • 20.  Transmission penumbra • It is the region irradiated by photons which are transmitted through the edge of the collimator blocks  Geometrical penumbra :  formula = • it is formed due to dimension of source. • It is formed due to finite source size and must be concern in teletherapy machines where the sources is between 1 – 2 cm in size.
  • 21.
  • 22.  Conclusions :  penumbra increases with increase in source diameter , SSD , and depth. Penumbra width decreases with a increase in SDD penumbra trimmers - :  it consists of extensible , heavy metal bars to attenuate the beam in the penumbra region.  increase the source to diaphragm distance , reducing the geometric penumbra.
  • 23.  Gantry  The gantry can rotate by 360°. The rotational movement of the gantry is motorized and controlled in two directions continuously; its rotation speed can be adjusted.  Teletherapy machines are most often mounted isocentrically, allowing the beam to rotate about the patient at a fixed SAD. They can be used either as fixed field machines or rotation units.  Most cobalt-60 unit machines have SAD of 80 cm.
  • 24.  The axis of rotation of the three structures: Gantry Collimator Couch coincide at a point known as the Isocenter. Isocentric Mounting  Enhances accuracy.  Allows faster setup and is more accurate than older non isocentrically mounted machines.  Makes setup transfer easy from the simulator to the treatment machine
  • 25.
  • 26.  Patient Support Assembly / Couch  Treatment Bed has motorized movements  Horizontal  Vertical  . Lateral.  Table Top - 90°rotation to each side  Base - 90° rotation to each side
  • 27.  Control Console  Control Console is situated outside the bunker  Interlocks present on the console for- : Air Pressure  Door Head Lock -Treatment Head has a swivel movement of +/- 180°.  OFF Shield  Treatment Mode.  Wedge Filter. Tray Interlock.  Timer
  • 28.  Timer  The prescribed target dose is delivered with the help of two treatment timers -:  primary timer - the primary timer actually controls the treatment time.  secondary timer - accounts for the source movement from OFF to ON position and agin to OFF position ( shutter time )  Formula of shutter time =
  • 29.  where , R1 - meter reading for given time ( say 2 min ) R2 - Meter reading for two consecutive times ( 1+1 min ) eg - : Meter reading + 300 v Time 1 min MR 1 MR 2 Mean 36.15 nc 36.14 nc 36.145 nc
  • 30.  Warning lights • Red light: Radiation present- do not enter room • Green Light: time elapsed • Malfunction: both red and green lights still on- means that machine is still in on position after prescribed dose has been delivered. Remove patient.
  • 31.  Beam shaping and modifying devices  The system has accessories like -: wedge filters Breast cone Sheilding blocks, to modify the beam shape or beam attenuation.  They are placed on the machine between the collimator and the patient.
  • 32.  wedge filters  special filters or absorbing blocks are placed in the path of a beam to modify its isodose distribution.  The most commonly used beam-modifying device is the wedge filter.  This is a wedge-shaped absorber that causes a progressive decrease in the intensity across the beam, resulting in a tilt of the isodose curves from their normal positions.
  • 33.  the isodose curves are tilted toward the thin end, and the degree of tilt depends on the slope of the wedge filter.  In actual wedge filter design, the sloping surface is made either straight or sigmoid in shape .
  • 34.  The wedge is usually made of a dense material, such as lead or steel, and is mounted on a transparent plastic tray,  which can be inserted in the beam at a specified distance from the source .  This distance is arranged such that the wedge tray is always at a distance of at least 15 cm from the skin surface, so as to avoid destroying the skin-sparing effect of the megavoltage beam.
  • 35.  Wedge Systems  Wedge filters are of two main types -: I. individualized wedge system,  which requires a separate wedge for each beam width, optimally designed to minimize the loss of beam output.  A mechanism is provided to align the thin end of the wedge with the border of the light field
  • 36.
  • 37. 2 . The second system uses a universal wedge -:  a single wedge serves for all beam widths.  Such a filter is fixed centrally in the beam, while the field can be opened to any size.  only a small part of this wedge is effective in producing the given wedge angle.  The rest, being unwedged, does not contribute to the isodose tilt but reduces the beam intensity .
  • 38.
  • 39.  the individualized system reducing the beam output, it is preferred for use in cobalt teletherapy.  The universal wedge, is useful for linear accelerator beams where the output is more.  From the setup and treatment planning points of view, the universal wedge is simpler to use than the individualized filter.
  • 40.
  • 41.  Effect on Beam Quality  The wedge filter alters the beam quality by preferentially attenuating the lower- energy photons (beam hardening)  to a lesser extent, by Compton scattering, which results in energy degradation (beam softening).  For the 60Co beam, because the primary beam is essentially monoenergetic, the presence of the wedge filter does not alter the central axis percent depth dose distribution.  For x-rays, on the other hand, there can be some beam hardening , and as a result the depth dose distribution can be somewhat altered, especially at large depths
  • 42.  Breast Cone  A beam modifying and directing device used for a tangential fields therapy  Advantages: –  Directs beam to the central axis of the area of interest, where a tangential beam is applied to a curved surface  Helps position, the patient with an accurate SSD  Endplate provides compensation,  which enhances surface dose and presses down the tissue.  Effective shielding of lungs
  • 43.  SHIELDING BLOCKS  Aims of shielding-  protect critical structures ( organ )  avoid unnecessary radiation to normal tissues  matching adjacent fields
  • 44.  An ideal shielding material should have the following characteristics :  high atomic no  high density  easily available  inexpensive  easily modifiable  The most commonly used shielding material for photons is Lead ( Pb ) The thickness of shielding block used depends upon the energy of the radiation
  • 45. The shielding material which reduces beam transmission to 5% of its original is considered acceptable . The term half value layer is an expression for the attenuation produced by any material. half-value layer (HVL) is defined as the thickness of an absorber of specified composition required to attenuate the intensity of the beam to half its original value. Practically thickness of lead between 4.5 – 5 half value layers which results in 5% or less of primary beam transmission.
  • 46.  Custom blocks • The conformal blocks are made with low melting point alloy called Cerrobend. • The Cerrobend material consists of 50.0% bismuth, 26.7% lead, 13.3% tin, and 10.0% cadmium . • The main advantage of Cerrobend over lead is that it melts at about 70 °C (compared with 327 °C for lead) and therefore, can be easily cast into any shape. • At room temperature, it is harder than lead. • The minimum thickness of Cerrobend blocks required for blocking may be calculated from Table 13.1 using its density ratio relative to lead (e.g., multiply lead thickness by 1.21).
  • 47.
  • 48.  Placing of shielding material  In kilovoltage radiation shielding is readily achieved by placing sheets of lead on the surface directly  It is because of the lower penetrating power of beam  In megavoltage radiation, Thicker blocks used. Placed higher up in shadows trays (15-20cm )
  • 49.  T - ROD mechanism in cobalt-60 unit  The external T-ROD shall be fitted with this indicator rod incase of failure of Automatic source retracting system to push the source to the OFF condition.  Source stuck during treatment – Emergency situation when the Cobalt-60 source gets stuck in between the “off” and “on” position .  Rotate gantry to side opposite to maze wall – Insert “T-rod” and push it till the source reaches “safe” position
  • 50.
  • 51.  The beamstopper  The beamstopper is a lead-filled steel assembly, which acts as a beam absorber. The beamstopper attenuates 99.9% of the primary beam.  A beam stopper is used to intercept the beam for additional shielding of the exit beam. The beam stop also acts as a counterweight for the head of the machine.
  • 52.
  • 53.  References -: I. KHAN’S The Physics of Radiation Therapy II. Radiation Oncology Physics: E.B. Podgorsak III. Article - BARC DEVELOPS COBALT-60 TELETHERAPY MACHINE FOR CANCER TREATMENT