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Microstrip Antennas Questions and Answers

Answer: C

The direct radiation and the contribution diffracted from the board edge arrive with a path difference that varies with angle, so they alternately add and cancel and the pattern ripples, most noticeably towards the horizon and behind. A larger or absorber lined ground plane smooths it. Connector reflection, mode excitation and range length can all degrade a measurement but produce different signatures. Recognising a ripple as an interference effect points straight at a second path.

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Answer: D

Absorber at the board edge attenuates the surface and creeping waves before they can diffract, so the measured pattern is closer to that of an infinite ground plane. It costs a little gain rather than adding any. Chamber wall reflections are dealt with by absorber on the walls, and thermal management is not a pattern measurement concern. Treating the antenna's own structure as a source of unwanted radiation, and absorbing it, is a standard measurement technique.

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Answer: A

An impedance measurement cannot distinguish power that has been radiated from power that has been dissipated, since both leave the input port and neither returns. Efficiency is therefore obtained by comparing measured gain with computed directivity, or by a reverberation chamber or Wheeler cap measurement. Signal level is ample, efficiency is a scalar property rather than a directional one, and connector loss is calibrated in the usual way. A quantity that cannot be measured at one port needs a method that looks at both.

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Answer: B

Enclosing the antenna in a conducting cap suppresses radiation while leaving the ohmic losses unchanged, so comparing the input resistance with and without the cap separates the two. It is the classical way of measuring the efficiency of an electrically small antenna. Patterns cannot be measured inside a cap, resonance is found from the impedance sweep, and polarisation needs a far field measurement. Suppressing one loss mechanism to measure the other by difference is an elegant and widely applicable idea.

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Answer: C

For a small antenna the two resistances are of the same order, so the difference the cap reveals is a large and well measured fraction of the total. For an efficient antenna the difference would be a small residue between two nearly equal numbers and the method would be imprecise. Physical size, bandwidth and pattern breadth are practical conveniences rather than the reason. A differential method works best when the difference being measured is not a small remainder.

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Answer: D

A stirred reflective chamber creates a statistically uniform field, so the received or radiated power can be integrated over all directions and polarisations without measuring the pattern at all. That gives total radiated power and, with the input power, the efficiency. Pattern and impedance are measured by other means, and polarisation information is deliberately averaged away, which is exactly what makes the measurement fast and pattern independent.

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Answer: A

Since a phone is held at arbitrary angles against a head and hand, no single direction of the pattern characterises it usefully, and the power summed over all directions is what predicts performance. Network operators specify it for that reason. Regulators specify emissions and exposure rather than patterns, handset patterns are routinely measured, and a closed case presents no obstacle to a pattern measurement. Choosing a figure of merit that matches how the device is actually used is the point.

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Answer: B

Specific absorption rate measures how much radiofrequency power is deposited per kilogram of tissue, and exposure limits are written in those terms. Handset antennas are designed and placed to keep it within the limit, which sometimes conflicts with radiation efficiency. Moisture uptake, conductor loss and receiving aperture are quite different quantities. A regulatory limit expressed in terms of an effect on the user, rather than on the equipment, constrains design in ways that purely electrical specifications do not.

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Answer: C

Distance from the head reduces the specific absorption rate and the detuning that tissue proximity causes, at the cost of the hand gripping that end. It is a compromise between two absorbers rather than an escape from either. Board width, battery placement and available volume all influence the layout but none is the governing reason. Where an antenna is placed inside a product is usually decided by the human body rather than by electromagnetics alone.

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Answer: D

Tissue is a lossy dielectric close to the radiating structure, so it shifts the resonance and absorbs a substantial fraction of the power, and losses of several decibels are common. Designs are evaluated with standardised hand and head phantoms for this reason. A hand is a poor ground plane and a good absorber, the plastic case provides no shielding at all, and polarisation is set by the current direction. Anything within a fraction of a wavelength becomes part of the antenna, and a hand is no exception.

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