
Hierarchical Methods
Undulative Electrodynamical Systems, Volume 2
By:Â V. Kulish
Hardcover | 31 October 2002
At a Glance
404 Pages
24.13 x 16.51 x 2.54
Hardcover
$169.75
or 4 interest-free payments of $42.44 with
 orÂShips in 7 to 10 business days
| Preface | p. xv |
| Hierarchical Theory of Undulative Induction Accelerators (EH-Accelerators) | p. 1 |
| EH-Accelerators: General Ideas and Properties | p. 2 |
| Principles of Operation of EH-Accelerators | p. 2 |
| Comparison of Charged Particle Motions in Longitudinal Electric and Transverse EH-Undulated Fields | p. 5 |
| Example of the EH-Field Presentation | p. 7 |
| EH-Accelerator as a Hierarchical Oscillative System | p. 11 |
| Oscillations and Quasi-Resonances | p. 11 |
| Hierarchy of Oscillations | p. 17 |
| Motion of Charged Particles in the Non-Stationary Linearly Polarized EH-Accelerator | p. 21 |
| Analytical Solutions of the Problem of Particle Motion | p. 21 |
| Effect of Electron Reflection from the System Input | p. 24 |
| Effect of a Particle's Capture | p. 27 |
| Picosecond Electron Bunch Formers | p. 32 |
| Motion of an Electron Bunch in a Non-Stationary EH-System | p. 32 |
| Example of the EH-Former for Picosecond Electron Bunches | p. 37 |
| Stationary EH-Accelerators | p. 39 |
| Elementary Theory of the Stationary Linearly Polarized EH-Accelerators | p. 39 |
| Inhomogeneous One-Particle Models | p. 45 |
| Example: Project of an Especially Compact Stationary EH-Accelerator | p. 52 |
| One of Possible Applications: the E-Beam Sterilizers | p. 52 |
| Example: the EH-accelerator for Waste and Natural Water Purification Systems | p. 53 |
| The Effect of 'Cooling' of Charged Particle Beams in EH-Accelerators | p. 59 |
| The Cooling Effect and the Fundamental Principles of Physics | p. 59 |
| Essence of the Cooling Effect | p. 60 |
| Homogeneous Non-Stationary Model | p. 61 |
| Inhomogeneous Non-Stationary Models | p. 67 |
| Stationary EH-Coolers | p. 70 |
| Undulative Electric and Magnetic Fields in Stationary EH-Coolers | p. 70 |
| Single Particle Theory of the Linearly Polarized Stationary EH-Cooler | p. 73 |
| Optimization of the Stationary EH-Cooler | p. 79 |
| Inhomogeneous Model of the Stationary EH-Cooler | p. 82 |
| Free Electron Lasers as a Classical Electron Device with a Long-Time Interaction | p. 89 |
| Free Electron Lasers: General Information | p. 89 |
| Place of the Free Electron Lasers in Modern Electronics | p. 89 |
| Priority Problem | p. 91 |
| Basic Physical Mechanisms and the First Theoretical Design | p. 92 |
| The First Realized Designs of Free Electron Lasers | p. 104 |
| Grouping (Bunching) Mechanisms in Free Electron Lasers | p. 107 |
| Longitudinal Grouping Mechanism | p. 107 |
| Transverse Grouping (Bunching) Mechanism | p. 114 |
| Energy Transfer in the System 'Beam+Pumping+Signal' | p. 115 |
| Hierarchical Single-Particle Theory of Free Electron Lasers | p. 123 |
| General Approach to the Single-Particle Theory of Free Electron Lasers | p. 124 |
| Method of Simulated Magneto-Dielectric | p. 124 |
| Types of Modeling Pumping Fields | p. 130 |
| Electron Motion in the Field of Electromagnetic Waves. Integrals of Motion | p. 132 |
| Reducing Initial Equations to the Standard Form | p. 136 |
| Classification of Models | p. 138 |
| Case of a Weak Magnetic Field | p. 139 |
| Single-Particle Theory of the Free Electron Lasers of Dopplertron Type | p. 142 |
| Obtaining the Equations of the First Hierarchical Level | p. 142 |
| Passing to the H-Ubitron Model | p. 144 |
| 'Efficiency-Phase' Variables | p. 145 |
| Model with the Optimal Electrostatic Support | p. 146 |
| Model with the Optimal Variation of the Retardation Factor | p. 148 |
| Some Approximate Analytical Solutions | p. 149 |
| Model with the Two-Frequency Pumping | p. 150 |
| The Single-Particle Theory of the Free Electron Laser with EH-Pumping | p. 154 |
| Fields and Problem Formulation | p. 154 |
| Resonant Conditions | p. 155 |
| Truncated Equations in the Case of a Weak Magnetic Field | p. 156 |
| Truncated Equations in the Case of a Coupled Parametric-Cyclotron Resonance | p. 158 |
| Isochronous Models. The Case of a Super-Weak Magnetic Field | p. 159 |
| Simplified Multi-Particle Theory of the EH Free Electron Laser | p. 161 |
| Hierarchical Self-Consistent Theory of Free Electron Lasers | p. 169 |
| General Formulation of the Problem | p. 170 |
| General Arrangement | p. 170 |
| Fields and Resonances | p. 170 |
| Electric Support | p. 172 |
| Parametric Free Electron Laser as a Hierarchical Oscillative System | p. 172 |
| Motion Problem | p. 173 |
| Self-Consistent Problem | p. 174 |
| Self-Consistent Truncated Equations. Simplified Version of the Method of Slowly Varying Amplitudes | p. 175 |
| Statement of the Problem | p. 176 |
| Initial Equations | p. 176 |
| Truncated Equations in the Complex Form | p. 177 |
| Truncated Equations in the Real Form | p. 180 |
| Integrals of Motion | p. 181 |
| Raman and Compton Modes | p. 182 |
| Self-Consistent Truncated Equations. Method of the Averaged Kinetic Equation. The Cubic Dopplertron Model | p. 183 |
| Statement of the Problem | p. 183 |
| Transforming the Kinetic Equation into the Form with Total Derivatives | p. 184 |
| Scalar Part of the Fields | p. 184 |
| Current Density and Space Charge | p. 185 |
| The Problem of Large Parameters | p. 186 |
| Averaged Kinetic Equation | p. 187 |
| Wave and Single-Particle Resonant Conditions | p. 187 |
| Representation of the Distribution Function in the Form of a Fourier Series | p. 188 |
| Truncated Equations for the Slowly Varying Amplitudes of Distribution Function | p. 188 |
| Solving the Truncated Equation by Successive Approximations | p. 190 |
| Back Transformation | p. 192 |
| Maxwell's Equations | p. 193 |
| Truncated Equations for the Wave Amplitudes | p. 194 |
| Raman and Compton Interaction Modes | p. 196 |
| Self-Consistent Truncated Equations. The Method of the Averaged Kinetic Equation. The Cubic Nonlinear H-Ubitron Model | p. 197 |
| Formulation of the Problem | p. 197 |
| Three-Level Hierarchical Calculational Scheme | p. 198 |
| Double-Averaged Kinetic Equation | p. 200 |
| Solutions of the Double-Averaged Kinetic Equation | p. 200 |
| Back Transformation on the First Hierarchical Level | p. 201 |
| Truncated Equations for the Complex Wave Amplitudes | p. 203 |
| Simplified Version of the Truncated Equations | p. 204 |
| Self-Consistent Truncated Equations. The Method of Slowly Varying Amplitudes. The Quadratic Kinetic Dopplertron Model with Arbitrarily Polarizations of the Electromagnetic Waves | p. 205 |
| Formulation of the Problem | p. 206 |
| Truncated Equations for the Wave Amplitudes | p. 207 |
| Solving the Kinetic Equation by Successive Approximations | p. 208 |
| Again the Truncated Equations for Wave Amplitudes | p. 210 |
| Stationary Version of the Truncated Equations for Wave Amplitudes | p. 212 |
| Integrals of Motion | p. 213 |
| Self-Consistent Quadratic FEL Theory of the Simplest Linearly Polarized Quasi-Hydrodynamic Model | p. 214 |
| Truncated Equations for the Simplest Model | p. 214 |
| Case of the Given Pumping Field | p. 214 |
| Case of Self-Consistent Changing of All Slowly Varying Amplitudes. Integration Algorithm | p. 216 |
| The Case of Self-Consistent Changing of All Slowly Varying Amplitudes. The Boundary Conditions Problem | p. 219 |
| The Case of Self-Consistent Changing of All Slowly Varying Amplitudes. The Solutions | p. 219 |
| The Case of Self-Consistent Changing of All Slowly Varying Amplitudes. The Passage to the Approximation of a Given Pumping Field | p. 220 |
| Analysis of the Wave Resonant Conditions | p. 221 |
| The Model of a Cold Electron Beam | p. 221 |
| ADE Interaction Modes in the Dopplertron FEL | p. 222 |
| Passing to the Case of the H-ubitron Model | p. 224 |
| Dopplertron Models with Retarded Pumping | p. 224 |
| Role of the Thermal Electron Beam Spread | p. 226 |
| Self-Consistent Quadratic FEL Theory of the Arbitrary Polarized Kinetic Model. The Approximation of a Given Pumping Field in the Case of the Raman Mode | p. 227 |
| Types of Instabilities which Are Possible in the Dopplertron FELs | p. 227 |
| Boundary Conditions | p. 228 |
| Solutions | p. 228 |
| Threshold of Interaction | p. 229 |
| Passage to the H-Ubitron Model | p. 230 |
| Phase Effects | p. 230 |
| Polarization Effects | p. 231 |
| The Effects of Phase and Polarization Discrimination | p. 233 |
| The Role of the Pumping Wave Retardation in the Amplification Process | p. 237 |
| Self-Consistent Quadratic FEL Theory of the Arbitrarily Polarized Kinetic Model. The Approximation of the Given Pumping Field in the Case of Compton Mode | p. 238 |
| Truncated Equations | p. 238 |
| Boundary Conditions | p. 239 |
| Solutions | p. 239 |
| Phase and Polarization Effects | p. 241 |
| Self-Consistent Quadratic FEL Theory. The Explosive Instability in the Linearly Polarized Raman Model | p. 242 |
| Classification of the Self-Consistent Modes of Interaction | p. 243 |
| Truncated Equations. The Cold Linearly Polarized Dopplertron Model | p. 244 |
| Classification of Models with Explosive Instability | p. 245 |
| Analysis of the Synchronous Conditions (Kinematic Analysis) | p. 245 |
| Amplitude Analysis | p. 246 |
| Case of Degeneration of the Wave Frequencies | p. 248 |
| The Influence of Dissipation for the SCW | p. 250 |
| Self-Consistent Quadratic Fel Theory. The Explosive Instability in the Arbitrarily Polarized Self-Consistent Raman Model | p. 251 |
| Truncated Equations in the Real Form | p. 251 |
| Motion Integrals | p. 252 |
| Functions u(z) and R(z) | p. 252 |
| Nonlinear Potential | p. 253 |
| Analytical Solutions | p. 253 |
| Explosive Length | p. 256 |
| Polarization Effects | p. 256 |
| Explosive Instability in the Linearly Polarized Self-Consistent Compton Model | p. 259 |
| The Self-Consistent Quadratic Fel Theory. The Explosive Instability in Linearly Polarized Self-Consistent Compton Model | p. 260 |
| The Compton Truncated Equations | p. 261 |
| Motion Integrals | p. 262 |
| Energy | p. 262 |
| Solutions | p. 262 |
| Compton Critical Length | p. 263 |
| Self-Consistent Quadratic Fel Theory of the Effect of the Generation of the Transverse H-Ubitron Field | p. 263 |
| Two Modes of the Effect of the Generation of Additional Magnetic Field | p. 264 |
| Wave Nonlinear Mechanism | p. 265 |
| Diamagnetic Mechanism | p. 266 |
| The Dopplertron Cubic Nonlinear Model. The Effect of Nonlinear Generation of the Longitudinal Electric Field | p. 268 |
| Physical Nature of the Generated Longitudinal Electric Field | p. 269 |
| Wave Efficiency | p. 269 |
| Gain Factor | p. 271 |
| Numerical Analysis | p. 271 |
| Dopplertron Cubic Nonlinear Model. The Isochronous Model of a Dopplertron Amplifier | p. 274 |
| H-Ubitron Cubic Nonlinear Model. The Effect of Nonlinear Generation of the Transverse Periodic Magnetic Field | p. 279 |
| Adapted System of Truncated Equations and Its Accuracy | p. 280 |
| Generation of the Additional Improper H-Ubitron Fields | p. 281 |
| Nonlinear Generation of the Proper H-Ubitron Fields | p. 285 |
| Hierarchical Theory of Two-Stream Superheterodyne Free Electron Lasers | p. 291 |
| Two-Stream Superheterodyne Free Electron Lasers As a New Class of Relativistic Electron Devices | p. 292 |
| History of the Problem and the Main Ideas | p. 292 |
| Two-Stream Superheterodyne Free Electron Laser (TSFEL): Design Schemas and Their Principles of Operation | p. 295 |
| Analyzed Models | p. 298 |
| Theory of the Two-Stream Instability | p. 302 |
| Initial Model. Statement of the Problem | p. 303 |
| The Linear Approximation | p. 304 |
| Nonlinear Approximation | p. 308 |
| Analysis | p. 311 |
| The Essence of the Effect of Two Superheterodyne Amplification | p. 314 |
| Qualitative Comparison of the Parametric and Superheterodyne Mechanisms of Amplification | p. 314 |
| Main Idea of the Effect of Superheterodyne Amplification | p. 315 |
| Formulation of the Cubic Nonlinear Two-Stream Superheterodyne Problem | p. 317 |
| Model and Fields | p. 317 |
| Two-Stream Superheterodyne Free Electron Laser as a Hierarchical Wave-Oscillative System | p. 319 |
| Quasi-Compton and Raman Interaction Modes | p. 321 |
| Electric Support and the Effect of Nonlinear Generation of the Longitudinal Electric Field | p. 323 |
| Motion Problem | p. 324 |
| Concept of the Space Charge Waves in the Cases of Raman and Compton Modes | p. 325 |
| Cubic Nonlinear Truncated Equations and Analysis | p. 329 |
| Cubic Nonlinear Truncated Equations | p. 329 |
| Amplification Dynamics | p. 332 |
| Efficiency Dynamics | p. 334 |
| Influence of the Effect of Nonlinear Generation of the Longitudinal Electric Field | p. 335 |
| Influence of the Generated Magnetic Field | p. 338 |
| Influence of Highest Harmonics and Longitudinal Focusing Magnetic Field | p. 341 |
| Klystron TSFEL Amplifiers | p. 344 |
| Epilogue | p. 353 |
| Appendices | p. 354 |
| Appendix A | p. 355 |
| Appendix B | p. 359 |
| Appendix C | p. 361 |
| Appendix D | p. 363 |
| Appendix E | p. 365 |
| Appendix F | p. 367 |
| Index | p. 375 |
| Table of Contents provided by Ingram. All Rights Reserved. |
ISBN: 9781402009686
ISBN-10: 1402009682
Series: FUNDAMENTAL THEORIES OF PHYSICS : Book 2
Published: 31st October 2002
Format: Hardcover
Language: English
Number of Pages: 404
Audience: Professional and Scholarly
Publisher: Springer Nature B.V.
Country of Publication: US
Dimensions (cm): 24.13 x 16.51 x 2.54
Weight (kg): 0.84
Shipping
| Standard Shipping | Express Shipping | |
|---|---|---|
| Metro postcodes: | $9.99 | $14.95 |
| Regional postcodes: | $9.99 | $14.95 |
| Rural postcodes: | $9.99 | $14.95 |
Orders over $79.00 qualify for free shipping.
How to return your order
At Booktopia, we offer hassle-free returns in accordance with our returns policy. If you wish to return an item, please get in touch with Booktopia Customer Care.
Additional postage charges may be applicable.
Defective items
If there is a problem with any of the items received for your order then the Booktopia Customer Care team is ready to assist you.
For more info please visit our Help Centre.
You Can Find This Book In
This product is categorised by
- Non-FictionSciencePhysicsClassical MathematicsDynamics & Statics
- Non-FictionEngineering & TechnologyMechanical Engineering & MaterialsMaterials ScienceMechanics of SolidsDynamics & Vibration
- Non-FictionMathematicsCalculus & Mathematical AnalysisNumerical Analysis
- Non-FictionEngineering & TechnologyEnergy Technology & EngineeringElectrical Engineering
- Non-FictionMedicineMedicine in General
- Non-FictionSciencePhysicsElectricity
- Non-FictionSciencePhysicsMathematical Physics


























