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| Content Provider | IEEE Xplore Digital Library |
|---|---|
| Author | Parmar, N. Deshpande, P. Choyal, Y. Maheshwari, K.P. Bhat, K.S. |
| Copyright Year | 2011 |
| Description | Author affiliation: Microwave Tube Research and Development Centre, BEL Complex, Jalahalli, Bangalore, India (Bhat, K.S.) || School of Physics, D.A. University, Khandwa Road Campus, Indore, India (Parmar, N.; Deshpande, P.; Choyal, Y.) || Vardhman Mahaveer Open University, Kota, India (Maheshwari, K.P.) |
| Abstract | A strong axial magnetic field is required to guide a relativistic pulsed electron beam. The magnetic field can be supplied either by a permanent magnet or an electromagnet. In a backward wave oscillator (BWO) experiment, as the required field is 0–1.2 T in a cylindrical volume having radius of a couple of centimeters and length of about 10–12 cm, an electromagnet is preferred. A large pulsed current is passed into a solenoid to generate a pulsed magnetic field. This current is provided by a capacitor bank. In the paper, development of a pulsed magnetic field system is described. The generated magnetic field is of strength 1.25T with the pulse duration of 2 ms. Inner diameter of solenoid is 5 cm and length is 12 cm. The magnetic field guides a relativistic electron beam that excites a slow wave structure to generate high power microwaves. To generate a unidirectional magnetic field, we must have a unidirectional current pulse. This is obtained by discharging a charged capacitor into an inductor with a resistor in between them. For critical damping, we get a unidirectional pulse. Assuming inductance L and resistance R, a maximum occurs att = 2L/R where the maximum current is t = 0.74V /R. The pulse duration is The experimental set up is as follows: Secondary of a step-up transformer gives a peak voltage of 2.5 kV. After half wave rectification, a capacitor bank having capacity of 450µF is charged through a 800 ohm hand woven resistor. Charging time of the capacitor bank is 3 sec. Charged capacitor bank is discharged into a solenoid, inductance L, through pulse forming non-inductive resistance R=1.3 Ω. A small resistance R=0.125Ω is in series for measurements. A spherical spark gap having 2 cm sphere diameter acts as a self breaking switch. As soon as the instantaneous value of current overshoots a predefined strength, the corresponding voltage that drops across the resistor R exceeds the comparing voltage on a comparator. This causes a timer circuit to give a turn on a relay that controls switching of a Marx capacitor bank for relativistic electron beam $generation^{1}.$ The voltage across R, therefore give us the information of current pulse as well as controls the triggering of electron beam system. Peak current is controlled by the pulse forming resistor R. Table 1 given below shows various values of R and corresponding value of voltage on R. Measured current, pulse duration and magnetic field are given in last three columns. |
| Starting Page | 467 |
| Ending Page | 468 |
| File Size | 70868 |
| Page Count | 2 |
| File Format | |
| ISBN | 9781424486625 |
| e-ISBN | 9781424486618 |
| DOI | 10.1109/IVEC.2011.5747078 |
| Language | English |
| Publisher | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Publisher Date | 2011-02-21 |
| Publisher Place | India |
| Access Restriction | Subscribed |
| Rights Holder | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Subject Keyword | Magnetic fields Electron beams Capacitors Microwave oscillators Resistors Voltage measurement Solenoids slow wave structures Relativistic electron beam capacitor bank HPM generation |
| Content Type | Text |
| Resource Type | Article |
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