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Page 318
... waveguide equation ' , and it is found to hold for any shape of waveguide , although it has here been deduced only for a simple special case . The cut - off wavelength λ , depends on the shape and dimensions of the waveguide , and on ...
... waveguide equation ' , and it is found to hold for any shape of waveguide , although it has here been deduced only for a simple special case . The cut - off wavelength λ , depends on the shape and dimensions of the waveguide , and on ...
Page 322
... waveguide with TE01 mode . ( a ) Lines of electric field ( b ) Lines of magnetic field and current flow approaches a purely transverse wave travelling along the x - axis . As → 0 since λ 。。→ 0 , giving in the limit a transverse wave ...
... waveguide with TE01 mode . ( a ) Lines of electric field ( b ) Lines of magnetic field and current flow approaches a purely transverse wave travelling along the x - axis . As → 0 since λ 。。→ 0 , giving in the limit a transverse wave ...
Page 705
... waveguide to a loosely coupled resonant cavity containing the paramagnetic sample and immersed in a refrigerant between the poles of an electromagnet . A small fraction of the cavity signal is fed through a second waveguide to a silicon ...
... waveguide to a loosely coupled resonant cavity containing the paramagnetic sample and immersed in a refrigerant between the poles of an electromagnet . A small fraction of the cavity signal is fed through a second waveguide to a silicon ...
Contents
ELECTROSTATICS I | 1 |
ELECTROSTATICS II | 33 |
STEADY CURRENTS | 62 |
Copyright | |
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Ampère's law amplifier amplitude angle angular anode anode current anode voltage applied approximately assumed atom band boundary C₁ C₂ capacitance capacitor cathode cavity coaxial coil components conducting conductor curl current flow curve deflexion detector dielectric constant difference diode dipole direction distance effect electric field electromagnetic electrons electrostatic emission energy equal equivalent filter flux force frequency galvanometer gives grid Hence impedance incident input ions known load magnetic field magnetic moment Mc/s mean square measured medium metal modulation molecule negative noise normal obtained ohms oscillator output parallel particle pentode phase plane polarization potential R₁ R₂ radiation radius ratio refractive index resistance resonance secondary shown in Fig shows signal solution space charge substance surface temperature tion triode tube tuned circuit unit V₁ V₂ vacuum tube vector velocity voltage volume wave waveguide wavelength wire Z₁ zero