Skip to main content

How to Use the INTRABEAM System

  • Chapter
  • First Online:
Targeted Intraoperative Radiotherapy in Oncology

Abstract

Mobile radiotherapy systems offer a versatility desirable for certain cancer treatments where the patient requires some form of surgical intervention. These systems can be taken into operating rooms and used to irradiate the tumour or tumour bed as part of a surgical procedure. Mobile techniques include brachytherapy treatments using sealed sources (i.e. HDR), electron units (Mobetron, Novac-7) and photon units (INTRABEAM®).

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 84.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 139.00
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 109.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

References

  • Carl Zeiss Surgical (2007) INTRABEAM® system PRS 500 with XRS 4. Carl Zeiss Surgical, Oberkochen

    Google Scholar 

  • Biggs DS, Thomson ES (1996) Radiation properties of a miniature X-ray device for radiosurgery. Br J Radiol 69:544–547

    Article  CAS  PubMed  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Regina Gonzalez .

Editor information

Editors and Affiliations

Appendices

Appendices

3.1.1 Appendix A: Treatment Calculation Time

3.1.1.1 Depth Dose Curve in Water

During production or recalibration, Zeiss determines the depth dose curve of a given XRS in a specially designed water phantom that allows the mounting and positioning of the XRS without the stand, as well as the insertion of the ion chamber (IC) inside a purpose-made holder within the phantom. The current obtained from the IC measured at different depths (z) will allow calculation of the depth dose curve from the following equation:

$$ \begin{array}{c}{D}_{w,z}\;\left[ Gy/ min\right]=I{C}_{TP,z}\;\Big[ nC/s\Big]\times {N}_s\;\Big[R/C\Big]\\ {}\kern0.48em \times {k}_q\times f\;\left[ Gy/R\right]\times 60\;\Big[s/ min\Big]\end{array} $$

where D w,z = absorbed dose to water at depth z; ICTP,z = ion chamber current reading in water phantom at depth z, temperature and pressure corrected; N s = calibration factor for the ion chamber used during the water phantom measurements taken from the PTW calibration certificate; f = conversion factor from roentgens to grays with a value of 8.81 mGy/R, as extracted from ICRU Report 17; and k q = beam quality correction factor – this takes the value of 1 for beam qualities in the (PTW) T30 to T50 range (accelerating voltage of 30 to 50 kV with effective energies of approx. 17–20 kV).

A fit function of the depth dose curve is generated mathematically to account for the impossibility of measuring directly on the surface of the XRS tip.

Similarly, depth dose curves are obtained with applicator, for each of the clinical applicators. The ratio between the depth curves with and without applicator provides the transfer function (Y z) for each applicator. Again, a fit function of these depth dose curves will be generated to account for the impossibility of directly measuring from the surface of the applicator.

Both calibration files, bare probe depth dose curve and applicator transfer functions, will be loaded onto the user terminal. The information is securely linked via the serial numbers of XRS and each individual applicator.

3.1.1.2 Original PAICH Output and IRM

Baseline values for dose rates and IRM rates are also loaded onto the system via calibration files obtained from measurements taken with the Zeiss factory PAICH and IC.

Thus, the original PAICH output at factory will be given as:

$$ \begin{array}{c}{D}_{original}\;\left[ Gy/ min\right]=I{C}_{TP}\;\left( PAIC{H}_{factory}\right)\kern0.22em \Big[ nC/s\Big]\\ {}\kern0.48em \times {N}_{k, factory}\;\left[ Gy/C\right]\times {k}_q\\ {}\kern0.58em \times 60\kern0.22em \left[s/ min\right]\end{array} $$

where ICTP = ion chamber current reading inside the PAICH, temperature and pressure corrected; N k,factory = calibration factor for the ion chamber used during the PAICHfactory measurements and taken from its PTW Air Kerma calibration certificate; and k q = beam quality correction factor as above.

3.1.1.3 Customer’s PAICH Output and IRM

The PAICH output measurement performed during the pre-treatment quality control determines the output of the XRS before the actual treatment session:

$$ \begin{array}{c}{D}_{customer}\;\left[ Gy/ min\right]=I{C}_{TP}\;\left( PAIC{H}_{customer}\right)\Big[ nC/s\Big]\\ {}\kern0.75em \times {N}_{k, customer}\;\left[ Gy/C\right]\\ {}\kern0.58em \times {k}_q\times 60\kern0.24em \left[s/ min\right]\end{array} $$

where N k,customer = calibration factor for the ion chamber used during the PAICHcustomer measurements taken from its PTW Air Kerma calibration certificate.

The software will compare the PAICH output value calculated during pre-treatment QA with that given in the stored calibration file. The software will not permit delivery of treatment when the deviation revealed by the comparison exceeds 10 %. If the deviation is between 5 and 10 %, the software will require the customer to acknowledge a warning message.

The actual absolute dose output in water (depth dose curve to be used for treatment) is calculated from the fitted depth dose curve in water and the factory and customer’s PAICH outputs:

$$ \begin{array}{c}{D}_{w,z\left( treat, bareXRS\right)}\kern0.24em \left[ Gy/ min\right]={D}_{w,z}\kern0.24em \Big[ Gy/ min\Big]\\ {}\kern0.6em \times \frac{D_{customer}}{D_{factory}}\end{array} $$

Finally, the total depth dose curve for the XRS plus applicator chosen will be:

$$ \begin{array}{l}{D}_{w,z(treat)}\kern0.17em [Gy/min]\\ {}\text{}={D}_{w,z(treat,bareXRS)}\kern0.17em [Gy/min]\kern0.17em \times \kern0.17em {Y}_z\end{array} $$

The calculated treatment time given by the INTRABEAM for a prescribed dose D w,z (Gy) will be:

$$ \begin{array}{l} Calculated\kern0.24em Treatment\; Time\kern0.24em \left[ \min \right]\\ {}=\frac{D_{w,z}\kern0.24em \left[ Gy\right]}{D_{w,z(treat)}\;\left[ Gy/ min\right]}\kern1.12em or,\end{array} $$
$$ \begin{array}{l} Calculated\kern0.24em Treatment\kern0.24em Time\kern0.24em \left[s\right]\\ {}=\frac{D_{w,z}\;\left[ Gy\right]}{D_{w,z(treat)}\;\left[ Gy/ min\right]}\times 60\kern0.24em \left[s/ min\right]\end{array} $$

This time and the actual IRM rate [count/s] measured during the pre-treatment QA procedure are used to calculate the total number of IRM counts that correspond to the treatment dose prescribed, D w,z [Gy].

$$ \begin{array}{c} Total\kern0.24em Counts\kern0.24em \left[ counts\right]={I}_{actual}\kern0.24em \Big[ counts/s\Big]\;\\ {}\kern0.36em \times Treatment\kern0.24em Time\kern0.24em \left[s\right]\end{array} $$

where I actual = IRM rate during pre-treatment QA procedure.

The actual treatment time, i.e. time during which radiation is being emitted, may increase or decrease depending on whether the dose rate of the XRS changes during treatment. The radiation will stop once the total IRM counts have been reached. However, if the calculated counts are not reached during 110 % of the calculated treatment time, then the system will stop the treatment. The delivered dose, up until the system stops the radiation, is recorded at all times.

3.1.2 Appendix B: Troubleshooting

The following flowcharts aim to provide a quick guide to the essential steps to follow when a problem or interlock with the INTRABEAM system is encountered. Any problem beyond the common faults/interlocks given here will require consultation with the manufacturer before an attempt is made to resolve it.

figure i
figure j

Rights and permissions

Reprints and permissions

Copyright information

© 2014 Springer-Verlag Berlin Heidelberg

About this chapter

Cite this chapter

Gonzalez, R., Reynolds, C. (2014). How to Use the INTRABEAM System. In: Keshtgar, M., Pigott, K., Wenz, F. (eds) Targeted Intraoperative Radiotherapy in Oncology. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-39821-6_3

Download citation

  • DOI: https://doi.org/10.1007/978-3-642-39821-6_3

  • Published:

  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-642-39820-9

  • Online ISBN: 978-3-642-39821-6

  • eBook Packages: MedicineMedicine (R0)

Publish with us

Policies and ethics