• DocumentCode
    983331
  • Title

    On the stored energy of planar apertures

  • Author

    Rhodes, Donald R.

  • Author_Institution
    North Carolina State Univ., Raleigh, NC, USA
  • Volume
    14
  • Issue
    6
  • fYear
    1966
  • fDate
    11/1/1966 12:00:00 AM
  • Firstpage
    676
  • Lastpage
    683
  • Abstract
    The volume integrals in the complex Poynting theorem are usually assumed to represent stored magnetic and electric energy. But for a planar aperture radiating into a lossless homogeneous medium it is shown that the only physically observable part of the volume integrals is twice that produced in the invisible region of the pattern space factor by those field components that vanish in the plane outside of the aperture. The inductive and capacitive reactive powers corresponding to the observable parts \\langle W_{m} \\rangle and \\langle W_{e} \\rangle , respectively, of the volume integrals are found to be given by the following integrals over the invisible region k_{y}^{2} + k_{z}^{2} > k^{2} , 2\\omega \\langle W_{m} \\rangle = frac{(2\\pi)^{2}}{2kZ_{0}} \\int \\int_{k_{y}^{2}+k_{z}^{2} > k^{2}} frac{|k_{z}F_{y}-k_{y}F_{z}|^{2}} {\\sqrt {k_{y}^{2}+k_{z}^{2}-k^{2}} dk_{y}dk_{z} , 2\\omega \\langle W_{e} \\rangle = frac{(2\\pi)^{2}}{2kZ_{0}} \\int \\int_{k_{y}^{2}+k_{z}^{2} > k^{2}} frac{k^{2}}(|F_{y}|^{2}+|F_{z}|^{2})} {\\sqrt {k_{y}^{2}+k_{z}^{2}-k^{2}} dk_{y}dk_{z} , for an arbitrary aperture consisting of holes in a conducting plane. They are expressed in terms of the rectangular components F_{y} and F_{z} of the pattern space factor obtained from the tangential components E_{y} and E_{z} of electric field over the holes S , F_{y}(k_{y},k_{z},k) = frac{1}{(2\\pi)^{2}} \\int \\int_{s} E_{y}(0,y,z,k)e^{i (k_{y}y+k_{z}z)}dydz F_{z}(k_{y},k_{z},k) = frac{1}{(2\\pi)^{2}} \\int \\int_{s} E_{z}(0,y,z,k)e^{i (k_{y}y+k_{z}z)}dydz where Z_{0} = \\sqrt {\\mu/\\epsilon} , and k_{y} and k_{z} are two components of the vector propagation constant of magnitude k=\\omega \\sqrt {\\mu\\epsilon} . For the complementary aperture whose space factor is obtained from Z_{0} times the tangential components of magnetic field in the aperture, the formulas for inductive and capacitive reactive power simply interchange. The new formulas are used to make the first known test of the widely held assumption that the reciprocal relationship between Q and bandwidth of nonradiating systems applies also to radiating systems. B- y direct computation of Q and of bandwidth independently it is shown that the reciprocal relationship does hold for the test case treated (the planar dipole).
  • Keywords
    Aperture antennas; Planar arrays; Aerospace testing; Apertures; Bandwidth; Conductors; Helium; Magnetic fields; Magnetic separation; Propagation constant; Reactive power; System testing;
  • fLanguage
    English
  • Journal_Title
    Antennas and Propagation, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-926X
  • Type

    jour

  • DOI
    10.1109/TAP.1966.1138801
  • Filename
    1138801