Scanners in Real Life Flashcards
Why is MRI not routinely used in Radiotherapy?
Resolution is not always as good as CT
Geometric accuracy not as good and depends on more factors than CT
Intensity is not calibrated to HU or tissue density
It is not as widely available as CT
It may not be supported by all TPS options
What is the MRI localisation decribed by?
wG = gamma.(B0+G.x)
What type of magnet is most common in MRI? Why?
Closed bore superconducting
It has a high B0 field and stability - therefore high SNR and good resolution
What is the equation for finding the magnetic field of an infinite solenoid?
B0 = u0 . n . I
What is the compromise in bore length?
Short bore is better for patient compliance but has worse homogeneity, long bores are the opposite
How is the homogeneity of a scanner described?
ppm over a diameter spherical volume (DSV)
How does the localisation of an MRI signal change if B0 is inhomogeneous?
wG = gamma(B0(r)+G.x)
The frequency is no longer linearly related to the location so get geometric distortion
What options are there for imaging patients in the Radiotherapy treatment positions?
Use a shorter bore, wider bore - worse overall B0 homogeneity
Use an open bore - better patient access, permanent magnet with cryogenic systems - lower B0 field and stability therefore lower SNR and worse resolution - longer scan times
Why is high gradient uniformity needed?
It will result in G being replaced by Gr) in the localisation equation
How are gradient coils manufactured to make the uniformity as high as possible?
Resistive coils are laminated to the coil structure The winding (plate) geometry is used to generate the required gradient field The accuracy of the windings determines the linearity
How is linearity checked for gradients?
Check with a uniform structure to measure the distortion - it typically gets worse the further off axis you are - end effects
What are the switching effects for the gradient coils?
The gradients are switched on and off to encode te signal location - they have resistance R and inductance L
The minimum TE is determined by the gradient rise and fall times - if they are slow get T2 loss so reduced SNR
What are the equations for the applied voltage across a coil and the current?
V = iR + Ldi/dt i = V/R(1-e^(-tL/R))
How is the inductance overcome to minimise the gradient rise/fall times?
Design the coils with minimal L
Use high voltage to drive the current rapidly
Drive the gradient with a trapezoidal waveform: has a rise rate which is deliverable in a linear fashion - within the capacity of gradient amplifiers
What is the side effect when high current and voltage are used to overcome the inductance?
There is significant heating - gives thermal expansion of gradient coils resulting in geometric changes
Heating of the local environment (shims) results in a frequency change and therefore geometric effects