EE 499 · Week 7 · Engineering view

Watch a Waveguide Mode Move

One mode, one rectangular guide, and the electric and magnetic fields drawn as vectors that you can watch evolve in space and in time. It draws the dominant TE10 mode of a rectangular guide, and lists the other modes the guide can carry at the chosen frequency.

Part of Week 7 · Fields Inside the Waveguide. New to waveguides? Start with the simplified 3D Waveguide Field Explorer →

Rectangular waveguide · TE10

Above cutoff — propagating
Guide
Operating frequency
Show
Time and position
0.20 cycles/s
0°
0.0 mm
Cutoff fc
GHz
f / fc
β
rad/m
α (decay)
Np/m
Free-space λ
mm
Guided λg
mm
Phase velocity
Group velocity

Travelling wave. The pattern in the cross-section keeps its shape, and the whole field pattern advances along +z: watch the crests in the lower plot move to the right. The phase velocity vp = ω/β is faster than c; that is a speed of pattern, not of energy. Energy and information move at the group velocity vg, which is slower than c. Ey and Hx rise and fall at the same instant (with opposite signs, because E × H must point along +z), so power flows.

Cross-section (x–y) at z = 0.0 mm. Looking along +z, the direction of propagation, toward the viewer.
Top view (x–z plane, y = b/2). Arrows: magnetic field H. Dot/cross: electric field Ey, pointing out of or into the screen.

Side view (y–z plane, x = a/2). Arrows: electric field E. Dot/cross: magnetic field Hx, pointing out of or into the screen.

Field along the guide at one point (x = a/4, y = b/2), for every component that is nonzero there: . Solid curves are the strongest component of each field, dotted curves the weaker one, and dashed curves the envelope the solid curve must stay inside. Dots mark the moving crests.
Electric field E Magnetic field H longitudinal component toward +z toward −z ⊙ field toward viewer   ⊗ field away from viewer

Modes of this guide, by cutoff

    Dominant mode
    Single-mode interval
    Next mode after the dominant
    Axial window shown
    mm
    Attenuation below cutoff
    dB/m
    What this model assumes.
    • Perfectly conducting walls and an air-filled, lossless guide, so there is no attenuation above cutoff.
    • Arrow length is proportional to field magnitude, and E and H are each scaled to their own peak over the cross-section at z = 0, so each longest arrow is 1. E and H sizes cannot be compared with each other.
    • Each arrow shows the instantaneous field at one point and one moment. Arrows in an axial view show only the components lying in that plane; the third component is the dot or cross.
    • The animation shows the phase ωt in slow motion. A real X-band field completes 1010 cycles each second.
    • One field pattern at one amplitude is drawn. Nothing here shows how the guide is excited.