A look inside the (large) Reverberation Chamber at the Otto-von-Guericke-University Magdeburg, Germany. On the left side is the vertical Mode Stirrer (or Tuner), that changes the electromagnetic boundaries to ensure a (statistically) homogeneous field distribution.
An electromagnetic reverberation chamber (also known as a reverb chamber (RVC) or mode-stirred chamber (MSC)) is an environment for electromagnetic compatibility (EMC) testing and other electromagnetic investigations. Electromagnetic reverberation chambers have been introduced first by H.A. Mendes in 1968. A reverberation chamber is screened room with a minimum of absorption of electromagneticenergy. Due to the low absorption very high field strength can be achieved with moderate input power. A reverberation chamber is a cavity resonator with a high Q factor. Thus, the spatial distribution of the electrical and magnetic field strengths is strongly inhomogeneous (standing waves). To reduce this inhomogeneity, one or more tuners (stirrers) are used. A tuner is a construction with large metallic reflectors that can be moved to different orientations in order to achieve different boundary conditions. The Lowest Usable Frequency (LUF) of a reverberation chamber depends on the size of the chamber and the design of the tuner. Small chambers have a higher LUF than large chambers.
The concept of a reverberation chambers is comparable to a microwave oven.
The notation is mainly the same as in the IEC standard 61000-4-21. For statistic quantities like mean and maximal values, a more explicit notation is used in order to emphasize the used domain. Here, spatial domain (subscript ) means that quantities are taken for different chamber positions, and ensemble domain (subscript ) refers to different boundary or excitation conditions (e.g. tuner positions).
where is the speed of light, , and are the cavity's length, width and height, and , , are non-negative integers (at most one of those can be zero).
With that equation, the number of modes with an eigenfrequency less than a given limit , , can be counted. This results in a stepwise function. In principle, two modes—a transversal electric mode and a transversal magnetic mode —exist for each eigenfrequency.
The Quality Factor (or Q Factor) is an important quantity for all resonant systems. Generally, the Q factor is defined by
where the maximum and the average are taken over one cycle, and is the angular frequency.
The factor Q of the TE and TM modes can be calculated from the fields. The stored energy is given by
Using the Q values of the individual modes, an averaged Composite Quality Factor can be derived:
includes only losses due to the finite conductivity of the chamber walls and is therefore an upper limit. Other losses are dielectric losses e.g. in antenna support structures, losses due to wall coatings, and leakage losses. For the lower frequency range the dominant loss is due to the antenna used to couple energy to the room (transmitting antenna, Tx) and to monitor the fields in the chamber (receiving antenna, Rx). This antenna loss is given by
where is the number of antenna in the chamber.
The quality factor including all losses is the harmonic sum of the factors for all single loss processes:
Resulting from the finite quality factor the eigenmodes are broaden in frequency, i.e. a mode can be excited even if the operating frequency does not exactly match the eigenfrequency. Therefore, more eigenmodes are exited for a given frequency at the same time.
The Q-bandwidth is a measure of the frequency bandwidth over which the modes in a reverberation chamber are
correlated. The of a reverberation chamber can be calculated using the following:
Using the formula the number of modes excited within results to
Related to the chamber quality factor is the chamber time constant by
That is the time constant of the free energy relaxation of the chamber's field (exponential decay) if the input power is switched off.
Crawford, M.L.; Koepke, G.H.: Design, Evaluation, and Use of a Reverberation Chamber for Performing Electromagnetic Susceptibility/Vulnerability Measurements, NBS Technical Note 1092, National Bureau od Standards, Boulder, CO, April, 1986.
Ladbury, J.M.; Koepke, G.H.: Reverberation chamber relationships: corrections and improvements or three wrongs can (almost) make a right, Electromagnetic Compatibility, 1999 IEEE International Symposium on, Volume 1, 1-6, 2–6 August 1999.