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Bush__The_Essential_Physics_for_Medical_Imaging - Biomedical ...

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greater overall input power). Next, an inverter circuit creates the high-frequency ACwave<strong>for</strong>m. This AC current supplies the high-voltage trans<strong>for</strong>mer and creates awave<strong>for</strong>m of fixed high voltage and corresponding low cutrent. Mter rectificationand smoothing, two high-voltage capacitors on the secondary circuit (shaded in Fig.5-32) accumulate the electron charges. <strong>The</strong>se capacitors produce a voltage acrossthe x-ray tube that depends on the accumulated charge, described by the relationshipV = QlC, where V is the voltage (volts), Q is the charge (coulombs), and C isthe capacitance (farads). During the x-ray exposure, feedback circuits monitor thetube voltage and tube current and correct <strong>for</strong> fluctuations.For kVp adjustment, a voltage comparator/oscillator measures the differencebetween the reference voltage (a calibrated value proportional to the requested kVp)and the actual kVp measured across the tube by a voltage divider (the kV sense circuit).Trigger pulses generated by the comparator circuit produce a frequency thatis proportional to the voltage difference between the reference signal and the measuredsignal. A large discrepancy in the compared signals results in a high triggerpulsefrequency, whereas no difference produces few or no triggc;r pulses. For eachtrigger pulse, the DC/AC inverter circuit produces a corresponding output pulse,which is subsequently converted to a high-voltage output pulse by the trans<strong>for</strong>mer.<strong>The</strong> high-voltage capacitors store the charge and increase the potential differenceacross the x-ray tube. When the x-ray tube potential reaches the desired value, theoutput pulse rate of the comparator circuit settles down to an approximately constantvalue, only recharging the high-voltage capacitors when the actual tube voltagedrops below a predetermined limit. <strong>The</strong> feedback pulse rate (generator frequency)strongly depends on the tube current (mA), since the high-voltagecapacitors discharge more rapidly with higher mA, thus actuating the kVp comparatorcircuit. Because of the closed-loop voltage regulation, autotrans<strong>for</strong>mers <strong>for</strong>kVp selection and input line voltage compensation are not necessary, unlike othergenerator designs.<strong>The</strong> mA is regulated in an analogous manner to the kVp, with a resistor circuitsensing the actual mA (the voltage across a resistor is proportional to the current)and comparing it with a reference voltage. If the mA is too low, the voltage comparator/oscillatorincreases the trigger frequency, which boosts the power to the filamentto raise its temperature and increase the thermionic emission of electrons.<strong>The</strong> closed-loop feedback circuit eliminates the need <strong>for</strong> space charge compensationcircuits and automatically corrects <strong>for</strong> filament aging effects.<strong>The</strong> high-frequency inverter generator is the preferred system <strong>for</strong> all but a fewapplications (e.g., those requiring extremely high power, extremely fast kVp switching,or submillisecond exposure times). In only rare instances is the constant-potentialgenerator a better choice.Voltage Ripple<strong>The</strong> voltage ripple of a DC wave<strong>for</strong>m is defined as the difference between the peakvoltage and the minimum voltage, divided by the peak voltage and multiplied by 100:01. I . I70 vo tage npp e = V max -V; V min X 100 [5-6]maxA comparison of the voltage ripple <strong>for</strong> various x-ray generators is shown in Fig.5-33. In theory, a single-phase generator, whether one-pulse or two-pulse output,

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