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Rad Physics Review 2 Rad Physics Prof. Stelmark Transformers Rad Physics Prof. Stelmark A transformer changes the intensity of alternating voltage and current. Rad Physics Prof. Stelmark Mutual Induction Rad Physics Prof. Stelmark Transformers A device in which two coils are placed near one another without electrical connection. The number of turns in the coils differs, causing a change in currnet in the secondary coil; this serves to either increase or decrease the voltage. Rad Physics Prof. Stelmark http://harphys.com/wp-content/uploads/2010/10/transformermovie-clip.swf Rad Physics Prof. Stelmark Types of transformers • • • • Air core Open core Closed core Shell type Rad Physics Prof. Stelmark Air core transformer Rad Physics Prof. Stelmark Open core transformer Rad Physics Prof. Stelmark Closed core transformer Rad Physics Prof. Stelmark Shell type transformer Rad Physics Prof. Stelmark Step up vs Step-down Rad Physics Prof. Stelmark If you increase the number of turns on the right, the voltage coming off the transformer will increase in proportion. Using the numbers in the example above, you can see that the right side has four times more turns. As a result, the voltage on the right has increased four times (from 100 V to 400 V). The voltage has been stepped up by a factor of four. Because current is inversely proportional to voltage, you can see that stepping up the voltage pays a price ... the current on the right is only a quarter of what it was on the left. Step-up transformers increase the voltage, but decrease the current. In our example above, the current went from 10 A to 2.5 A, a reduction of by a factor of four Rad Physics Prof. Stelmark If you decrease the number of turns on the right, the voltage coming off the transformer will decrease in proportion. Using the numbers in the example above, you can see that the right side has one fifth the number of turns. As a result, the voltage on the right is only one-fifth as large. The voltage has been stepped down by a factor of five (1000 V down to 200 V). Because current is inversely proportional to voltage, you can see that stepping down the voltage gives a bonus ... the current on the right is five times what it was on the left. Step-down transformers decrease the voltage, but increase the current. In our example above, the current went from 2 A to 10 A, an increase by Rad Physics Prof. Stelmark a factor of five. Transformer law Rad Physics Prof. Stelmark Ns Np If the turns ratio is greater than 1 the transformer is a step-up transformer. If the turns ratio is less than 1 the transformer is a step-down transformer Rad Physics Prof. Stelmark Autotransformer (kVp selector) self-induction Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark RECTIFICATION Rad Physics Prof. Stelmark X-RAY CIRCUIT Rad Physics Prof. Stelmark RECTIFICATION PROCESS BY WHICH ALTERNATING CURRENT IS CHANGED TO PULSATING DIRECT CURRENT Rad Physics Prof. Stelmark ALTERNATING CURRENT 1 PHASE A/C ( UNRECTIFIED)FREQUENCY 60 Hz Rad Physics Prof. Stelmark 60 POSITIVE PULSES/SEC Physics Prof. Stelmark 60 NEGATIVERadPULSES/SEC 60 POSITIVE PULSES 60 NEGATIVE PULSES 120 PULSES 60 FULL CYCLES Rad Physics Prof. Stelmark BATTERY – CURRENT OUTPUT STEADY D/C Rad Physics Prof. Stelmark D/C HALF WAVE RECTIFIED D/C HALF-WAVE – 60 POSITIVE PULSES/SEC NEGATIVE PULSES ARE SUPPRESSED 1 Physics PULSE/CYCLE Rad Prof. Stelmark D/C FULL WAVE RECTIFIED D/C HALF-WAVE – 120 POSITIVE PULSES/SEC Rad Physics Prof. Stelmark 2 PULSES/CYCLE D/C -3 PHASE 6 PULSE CURRENT D/C 3 PHASE 6 PULSE – 6 PULSES/CYCLE Rad Physics Prof. Stelmark D/C - 3 PHASE 12 PULSE D/C 3 PHASE 12 PULSE – 12 PULSES/CYCLE Rad Physics Prof. Stelmark DIODES OR VALVE TUBES HELP RECTIFY A/C CURRENT ELECTRONS DIODE VALVE TUBE Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark X-RAY TUBE FORWARD BIAS Rad Physics Prof. Stelmark REVERSE BIAS - + NO X-RAY Rad Physics Prof. Stelmark FORWARD vs REVERSE Rad Physics Prof. Stelmark RECTIFICATION TYPES ►HALF-WAVE ►FULL WAVE ►THREE PHASE SIX PULSE ►THREE PHASE TWELVE PULSE ►HIGH FREQUENCY SINGLE PHASE Rad Physics Prof. Stelmark RECTIFICATION NO RECTIFICATION HALF-WAVE FULL-WAVE Rad Physics Prof. Stelmark 3 PHASE RECTIFICATION Rad Physics Prof. Stelmark 3 PHASE RECTIFICATION Rad Physics Prof. Stelmark HIGH FREQUENCY RECTIFICATION Rad Physics Prof. Stelmark HALF-WAVE RECTIFICATION Rad Physics Prof. Stelmark HALF-WAVE RECTIFICATION Rad Physics Prof. Stelmark FULL-WAVE RECTIFICATION Rad Physics Prof. Stelmark FULL-WAVE RECTIFICATION Rad Physics Prof. Stelmark FULL-WAVE RECTIFICATION Rad Physics Prof. Stelmark 3 PHASE 6 PULSE Rad Physics Prof. Stelmark 3 PHASE 12 PULSE Rad Physics Prof. Stelmark HIGH FREQUENCY Rad Physics Prof. Stelmark VOLTAGE RIPPLE ►HALF WAVE------------------- 100% ►FULL WAVE ------------------ 100% ►3 PHASE 6 PULSE ----------- 13% ►3 PHASE 12 PULSE ---------- 4% ►HIGH FREQUENCY ---------- <1% Rad Physics Prof. Stelmark RIPPLE 100% 100% 100% Rad Physics Prof. Stelmark RIPPLE-3 PHASE 13% Rad Physics Prof. Stelmark RIPPLE-HIGH FREQUENCY <1% Rad Physics Prof. Stelmark Home-made x-ray apparatus Rad Physics Prof. Stelmark CHECKING FAILURE OF RECTIFICATION SYSTEM ►SPINNING TOP TEST – 1 PHASE EQUIPMENT ►SYNCHRONOUS SPINNING TOP TEST3 PHASE WITH LONGER EXPOSURE TIMES ►OSCILLOSCOPE- 3 PHASE EQUIPMENT WITH SHORT EXPOSURE TIMES Rad Physics Prof. Stelmark SPINNING TOP TEST Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark RESULT OF SPINNING TOP TEST- 1 PHASE - DASHES Rad Physics Prof. Stelmark HALF- WAVE RECTIFICATION # OF DASHES = TIME (SEC) x 60 PULSES Rad Physics Prof. Stelmark FULL- WAVE RECTIFICATION # OF DASHES = TIME (SEC) x 120 PULSES Rad Physics Prof. Stelmark RESULT OF SYNCHRONOUS SPINNING TOP TEST-3PHASE ARC Rad Physics Prof. Stelmark 3 PHASE RECTIFICATIONLONGER EXPOSURE TIME DEG. OF ARC = 360°/ sec x TIME (sec) Rad Physics Prof. Stelmark UTILIZING OSCILLOSCOPE Rad Physics Prof. Stelmark UTILIZING OSCILLOSCOPE RECTIFIED SYSTEM Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark 1. Main breaker - this is where the alternating current comes from to power the circuit. 2. Exposure switch - when you push the button to start an exposure this switch closes to start the exposure. 3. Autotransformer - this is where you adjust the kVp for the exposure. 4. Timer circuit - this part of the circuit stops the exposure. 5. High-voltage step-up transformer - this transformer bumps the voltage up so that the x-ray tube has very high voltage to make the electrons have enough energy to form x-rays. 6. Four-diode rectification circuit - this makes the current only go in one direction through the x-ray tube. 7. Filament circuit variable resistor - this variable resistor adjusts the current going to the filament. 8. Filament step-down transformer - this transformer steps the voltage down and therefore the current up. 9. X-ray tube - this is where the x-rays are created. Rad Physics Prof. Stelmark 10. Rotor stator - this rotates the anode. Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark Control Factor Electrical Device and Location in Circuit kVp Selection kVp Level Autotransformer (between incoming line and exposure switch) mA Selection Filament Current Variable resistor (in filament circuit between incoming line and step-down transformer) Time Selection Length of exposure Timer circuit (between exposure switch and step-up transformer) Rotor Switch Speed of rotating anode Stator (separate circuit from stator of anode motor) Exposure Switch Moment of exposure Switch (between autotransformer and timer circuit) Rad Physics Prof. Stelmark Rad Physics Prof. Stelmark