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Magnetic shielding is a mechanical solution, most of the time issued from a sheet metal process, done to solve a problem of low frequency  electromagnetic interference. Shielding channels the magnetic lines of the electromagnetic wave at frequencies from 0.1 to 10,000 Hz.
In the case of alternating fields (type 50 Hz), we must consider two factors: the concentration and the eddy currents that oppose the external fields. Unlike the electrical shield, magnetic shielding deflects the field lines ; so a single disc is therefore a shield.
Why are apertures and seams so important in some applications and completely irrelevant in others? It is convenient to divide shielding requirements into three categories: electric field shielding, magnetic field shielding and shielded enclosures. A conductive enclosure that completely surrounds a given volume prevents anything within that volume from electrically coupling to anything outside that volume.
Without the shield – Figure 1(b) – field lines may terminate on other conductors, resulting in potential differences between these conductors.
Key concepts for practical electric field shielding are choosing a location that will intercept the stronger field lines and choosing a suitably conductive shield material. For static electric fields, almost any material will look like a conductor, since the free charge can slowly reposition itself. Figure 3(a) illustrates a guard trace being used to reduce the coupling between two parallel traces on a printed circuit board. Because there are no free magnetic charges, it is not possible to terminate lines of magnetic flux on a shield. Currents induced in a conducting material by a time-varying magnetic field in this manner are called eddy currents.
In order to divert a magnetic field with a conductive plate, it is important to be able to develop sustained eddy currents. At kHz frequencies or lower, it is generally necessary to use permeable magnetic materials to divert magnetic fields. Note that it is important for the magnetic material shield to divert the magnetic flux all the way around the object being shielded. At high frequencies it is possible for the currents induced on the shield to radiate as well as (or possibly much better than) the original source of the fields.
An ideal shielded enclosure with infinite conductivity and no breaks would perfectly isolate (electromagnetically) whatever was inside the enclosure from whatever was outside.
Unfortunately, such an enclosure would not be very practical for electronic devices since it would be impossible to interact electrically with whatever was inside. Apertures are holes in a shielded enclosure such as those required for ventilation, optical displays, plastic components or mechanical supports.
Generally, the amount of energy escaping an enclosure through small apertures is insignificant compared to the energy escaping through seams, larger openings and wire penetrations.
A seam that optically appears to be well sealed can often disrupt the flow of surface currents significantly, causing a major breach in the shielding enclosure. In order for the shield on a shielded wire to be effective, it must make a low-inductance connection to the shielded enclosure.
Sometimes it is necessary to have a large number of apertures in a shield for the purposes of ventilation. For a rectangular waveguide with height b, width a and length d, the mode of propagation with the lowest cut-off frequency is the TE10 mode.
At frequencies where the term under the radical is negative, the propagation constant is imaginary and fields do not propagate.
For a circular waveguide with diameter a and length d, as illustrated in Figure 12, the mode of propagation with the lowest cut-off frequency is the TE11 mode. Note that derivations based on both rectangular and circular waveguides have a constant in front that is within 3 dB of 30. This model does not account for how the field was set up at one end of the opening or how efficiently it is radiated from the other end. Note that if a wire or second conductor of any kind penetrates the opening, the lowest-order mode of propagation is the TEM mode.
Some textbooks state that the attenuation in Equation 2 should be reduced by a factor of 10*log10(# of apertures) if there are multiple apertures.
These shields may be penetrated by unfiltered wires and sometimes consist of a single plate of metal that may or may not be connected to ground.

The answer relates to the fact that there are different kinds of shielding for different applications. However, a partial shield – Figure 2(a) – or even a simple metal plate – Figure 2(b) – can substantially reduce these potentials by altering the path of the electric field lines and preventing stronger fields from reaching the ‘victim’ circuit.Figure 2.
However, for high-frequency electric fields, the conductivity of the shield material must be high enough to allow the charge to move quickly back and forth. Figure 3(b) shows how grounding a heatsink attenuates the electric field between the heatsink and a printed circuit board ground plane. However, it is still possible to redirect magnetic flux lines to prevent unwanted coupling.
A vertical magnetic field from an electric motor couples to a small circuit board, resulting in interference.
Both the incident field and the magnetic field created by the eddy currents are shown in Figure 4(b). Since the eddy currents are driven by time-varying fields, a conductive plate cannot divert a static magnetic field. Since these materials have a reluctance much less than air, magnetic field lines can effectively be rerouted by providing an alternative path through a permeable material such as steel or mu-metal. A plate of magnetic material above or below the circuit board would provide no shielding at all.
This is possible whenever the maximum dimension of the shield is a significant fraction of a wavelength or larger. Even an enclosure with finite, but high, conductivity (eg, copper, aluminium or steel), would provide essentially perfect isolation in most practical applications if there were no seams, apertures or cable penetrations.
So the best that can be done is to start with a perfect enclosure and carefully evaluate every seam, every aperture and every cable penetration to ensure that no significant interfering signals are allowed to pass from one side to the other. In order for the enclosure to provide shielding, currents must be able to flow on the surface unimpeded.
Note how the grid in Figure 6(a) interrupts the flow of current much more significantly than the grid in Figure 6(b).
However, if the enclosure is well sealed and it is necessary to further reduce the energy escaping through the apertures, then apertures with sufficient depth can be provided to further attenuate the radiated emissions. Seams are often a more significant source of leakage than apertures because of their greater length.
For example, two metal surfaces simply pressed against each other as illustrated in Figure 7(a) or Figure 7(b) rarely provide sufficiently reliable contact at high frequencies. A single unshielded, unfiltered wire penetrating a shielded enclosure can completely eliminate any shielding benefit that the enclosure otherwise provided. This is generally accomplished by using a shielded connector that makes a 360° metal-to-metal contact with both the cable shield and the enclosure as illustrated in Figure 9(a).Figure 9.
As a result, any current flowing in the shield will produce a voltage drop across the pigtail that drives the cable shield relative to the enclosure, causing radiated emissions. Filtering will minimise voltage between the wire and enclosure at radiation frequencies, while allowing low-frequency signals or power to pass unattenuated.
In large enclosures with very stringent shielding and thermal requirements, it may be necessary to further reduce the amount of energy that can escape through any given aperture. The cut-off frequency is approximately the frequency at which the maximum height or width, a, is equal to a half-wavelength. Other modes of propagation yield different constants, but the lower-order modes dominate so it is reasonable to use a value of 30. However, even thin apertures will provide some attenuation if their cross sections are small relative to a wavelength. Therefore, by itself, it cannot be used to determine the shielding effectiveness of any particular shield. However, the attenuation in Equation 2 is in addition to any attenuation provided by a thin aperture or an array of thin apertures. Ott, Noise Reduction Techniques in Electronic Systems, John Wiley & Sons, New York, 1988.
On the other hand, it is not uncommon to find shields that do not surround the entire product. In terms of crosstalk, whether a cable shield needs to be grounded on one or both ends depends on the type of crosstalk the designer is trying to prevent. Electric fields generated within the volume either terminate on objects within the enclosure or on the inner surface of the enclosure walls, as illustrated in Figure 1.

Intercepting electric field lines with a conductive shield is primarily a matter of visualising the field lines that are potentially responsible for the unwanted coupling and positioning the shield so that it blocks these fields. Figure 3(c) demonstrates how the orientation of a daughter card affects the coupling of power bus noise to components on a mother board.
This can be accomplished by electric currents induced in an electrically conductive shield or by altering the path of magnetic flux lines using permeable materials.
Even if the field is slowly varying, losses in the conducting plate will cause the eddy currents to dissipate, allowing the magnetic flux to penetrate the plate.
Figure 5 illustrates how a shield made from a permeable material can be used to protect the circuit in the previous example.Figure 5.
At these frequencies, it is generally necessary to enclose the source completely while paying close attention to any apertures, seams or cable penetrations that could allow electromagnetic energy to escape. Fortunately, apertures with maximum dimensions that are much smaller than a wavelength provide very little impedance to the flow of currents on a conducting surface. In terms of electromagnetic shielding, the grid in Figure 6(b) is far superior, even though the total open area of both patterns is similar. A seam that is on the order of a half-wavelength long can be a very efficient radiation source, much like a resonant half-wave dipole.
Surface oxidation, corrosion and warping on the metal plates reduce the quality of the electrical contact. It is usually necessary to locate the filter as close to the connector location as possible in order to minimise the inductance of the connections and to prevent the possibility of noise coupling to the filtered wire before it exits the enclosure. This can be accomplished by increasing the depth of the aperture so that it resembles a small waveguide. The shielding effectiveness of an opening with a wire penetrating the opening is 0 dB regardless of its depth. Free charge on the enclosure relocates itself as needed to exactly cancel the fields within or external to the enclosure.Figure 1.
As long as charges are able to move freely enough to reorient themselves as fast as the field changes, cancellation of the external fields will be achieved.
Note that field lines terminating on a conductor imply there is a negative charge induced at that point. Note that the eddy currents cause the magnetic flux to be diverted around the plate and significantly reduce the coupling to the circuit.
For this reason, conductive materials are generally poor magnetic shields at low frequencies (below a few hundred kHz). For this reason, if it becomes necessary to provide a certain amount of open area (eg, for air flow), it is much better to accomplish this with many small apertures than with a few large apertures. Note that a shielding enclosure can be very effective even when it has a significant amount of open area, as long as each individual aperture is much smaller than a wavelength.
For apertures with a small cross-section, the frequencies of the sources within the enclosure are likely to be well below the cut-off frequency of the waveguide. It is possible to make inefficient antennas (such as an electrically small wire or loop antenna) radiate much more efficiently by enclosing them in a metal enclosure with a resonant slot or seam. Screws or rivets – Figure 7(c) – can provide a good electrical contact at points, but they do not necessarily improve the connection at locations between fasteners. At frequencies where the cross-sectional dimensions of the aperture are small relative to a half-wavelength, energy propagating through the aperture will be attenuated in the same manner that energy propagating through a waveguide below the cut-off frequency is attenuated. Conductive magnetic shields are also ineffective if they have slots or gaps that interrupt the flow of the eddy currents. One technique for reducing the impedance of seams is to overlap both sides of the plates as illustrated in Figure 7(d).
If the field is time varying, there will be a current on the surface of the conductor as these charges move back and forth. Another common solution is to employ finger stock or gaskets as shown in Figure 7(e) and (f).Figure 7.