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2) Analyze these data to determine the accuracy with which the beam range can be monitored and the actually delivered dose can be estimated.
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Radio waves with wavelengths in the centimetre range can be beamed by a reflector, like light in an automobile headlamp, to make up a radar system.
Some additional range can be accomplished by decreasing beam divergence angle θ, although this imposes more rigorous pointing and tracking requirements on the link.
The value of H is dependent on beam dimensions, relative rigidity of the beam with the soil and load pattern acting on the beam and can be taken in the range of 2 4 times beam width [28, 30].
By rotating lever L the lower end of beam z can be positioned along the range r to adjust for different external loads (F_z).
The total proton beam power will be in the range of 10 MW or more, while the beam quality can be relaxed compared to accelerators designed for H− beams and injection capability.
While higher on axis beam density can be achieved (better beam collimation), the beam temperatures are usually higher too (~10°K).
However, in accelerators which produce mono-energetic beams, such as fixed energy cyclotrons, a beam degrader can be used to change the energy of the proton beam.
Stretching of the GUV along the beam axis can be clearly observed.
Furthermore, a transmit subaperturing is designed in [20] with convex optimization, so that the range and angle responses are decoupled and the equivalent transmit beam can be focused in a certain range-angle sector to localize the targets.
From the Doppler shift of the backscattered sound, the component of water velocity parallel to the beam can be determined to a range of 1,400 metres from the transmitter with a precision of one centimetre per 0.1 second (one centimetre = 0.394 inch).
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