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Wireless Channel

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Wireless Channel

From a technical point of view, the greatest distinction between wireless and wireline communications lies in the physical properties of wireless channels. These physical properties can be described in terms of several distinct phenomena, including ambient noise, propagation losses, multipath, interference, and properties arising from the use of multiple antennas. Here we review these phenomena only briefly. Further discussion and details can be found, for example, in [38, 46, 148, 216, 405, 450, 458, 465].

Like all practical communications channels, wireless channels are corrupted by ambient noise. This noise comes from thermal motion of electrons on the antenna and in the receiver electronics and from background radiation sources. This noise is well modeled as having a very wide bandwidth (much wider than the bandwidth of any useful signals in the channel) and no particular deterministic structure (structured noise can be treated separately as interference). A very common and useful model for such noise is additive white Gaussian noise (AWGN), which as the name implies, means that it is additive to the other signals in the receiver, has a flat power spectral density, and induces a Gaussian probability distribution at the output of any linear filter to which it is input. Impulsive noise also occurs in some wireless channels. Such noise is similarly wideband but induces a non-Gaussian amplitude distribution at the output of linear filters. Specific models for such impulsive noise are discussed in Chapter 4.

Propagation losses are also an issue in wireless channels. These are of two basic types: diffusive losses and shadow fading. Diffusive losses arise because of the open nature of wireless channels. For example, the energy radiated by a simple point source in free space will spread over an ever-expanding spherical surface as the energy propagates away from the source. This means that an antenna with a given aperture size will collect an amount of energy that decreases with the square of the distance between the antenna and the source. In most terrestrial wireless channels, the diffusion losses are actually greater than this, due to the effects of ground-wave propagation, foliage, and so on. For example, in cellular telephony, the diffusion loss is inverse square with distance within line of sight of the cell tower, and it falls off with a higher power (typically, 3 or 4) at greater distances. As its name implies, shadow fading results from the presence of objects (buildings, walls, etc.) between the transmitter and receiver. Shadow fading is typically modeled by an attenuation (i.e., a multiplicative factor) in signal amplitude that follows a log-normal distribution. The variation in this fading is specified by the standard deviation of the logarithm of this attenuation.

Multipath refers to the phenomenon by which multiple copies of a transmitted signal are received at the receiver, due to the presence of multiple radio paths between the transmitter and receiver. These multiple paths arise due to reflections from objects in the radio channel. Multipath is manifested in several ways in communications receivers, depending on the degree of path difference relative to the wavelength of propagation, the degree of path difference relative to the signaling rate, and the relative motion between the transmitter and receiver. Multipath from scatterers that are spaced very close together will cause a random change in the amplitude of the received signal. Due to central-limit effects, the resulting received amplitude is often modeled as being a complex Gaussian random variable. This results in a random amplitude whose envelope has a Rayleigh distribution, and this phenomenon is thus termed Rayleigh fading. Other fading distributions also arise, depending on the physical configuration (see, e.g., [396]). When the scatterers are spaced so that the differences in their corresponding path lengths are significant relative to a wavelength of the carrier, the signals arriving at the receiver along different paths can add constructively or destructively. This gives rise to fading that depends on the wavelength (or, equivalently, the frequency) of radiation, which is thus called frequency-selective fading. When there is relative motion between the transmitter and receiver, this type of fading also depends on time, since the path length is a function of the radio geometry. This results in time-selective fading. (Such motion also causes signal distortion due to Doppler effects.) A related phenomenon arises when the difference in path lengths is such that the time delay of arrival along different paths is significant relative to a symbol interval. This results in dispersion of the transmitted signal, and causes intersymbol interference (ISI); that is, contributions from multiple symbols arrive at the receiver at the same time.

Many of the advanced signal transmission and processing methods that have been developed for wireless systems are designed to contravene the effects of multipath. For example, wideband signaling techniques such as spread spectrum are often used as a countermeasure to frequency-selective fading. This both minimizes the effects of deep frequency-localized fades and facilitates the resolvability and subsequent coherent combining of multiple copies of the same signal. Similarly, by dividing a high-rate signal into many parallel lower-rate signals, OFDM mitigates the effects of channel dispersion on high-rate signals. Alternatively, high-data-rate single-carrier systems make use of channel equalization at the receiver to counteract this dispersion. Some of these issues are discussed further in Section 1.3.

Interference, also a significant issue in many wireless channels, is typically one of two types: multiple-access interference and co-channel interference. Multiple-access interference (MAI) refers to interference arising from other signals in the same network as the signal of interest. For example, in cellular telephony systems, MAI can arise at the base station when the signals from multiple mobile transmitters are not orthogonal to one another. This happens by design in CDMA systems, and it happens in FDMA or TDMA systems due to channel properties such as multipath or to nonideal system characteristics such as imperfect channelization filters. Co-channel interference (CCI) refers to interference from signals from different networks, but operating in the same frequency band as the signal of interest. An example is the interference from adjacent cells in a cellular telephony system. This problem is a chief limitation of using FDMA in cellular systems and was a major factor in moving away from FDMA in second-generation systems. Another example is the interference from other devices operating in the same part of the unregulated spectrum as the signal of interest, such as interference from Bluetooth devices operating in the same 2.4-GHz ISM band as IEEE 802.11 wireless LANs. Interference mitigation is also a major factor in the design of transmission techniques (e.g., the above-noted movement away from FDMA in cellular systems) as well as in the design of advanced signal processing systems for wireless, as we shall see in the sequel.

The phenomena we have discussed above can be incorporated into a general analytical model for a wireless multiple-access channel. In particular, the signal model in a wireless system is illustrated in Fig. 1.2. We can write the signal received at a given receiver in the following form:

Equation 1.9

graphics/01equ009.gif


where gk(t,u) denotes the impulse response of a linear filter representing the channel between the kth transmitter and the receiver, i(·) represents co-channel interference, and n(·) represents ambient noise. The modeling of the wireless channel as a linear system seems to agree well with the observed behavior of such channels. All of the quantities gk(·, ·), i(·), and n(·) are, in general, random processes. As noted above, the ambient noise is typically represented as a white process with very little additional structure. However, the co-channel interference and channel impulse responses are typically structured processes that can be parameterized.

Figure 1.2. Signal model in a wireless system.

graphics/01fig02.gif

An important special case is that of a pure multipath channel, in which the channel impulse responses can be represented in the form

Equation 1.10

graphics/01equ010.gif


where Lk is the number of paths between user k and the receiver, a,k and t,k are the gain and delay, respectively, associated with the th path of the kth user, and d(·) denotes the Dirac delta function. Note that this is the situation illustrated in Fig. 1.2, in which we have written the time-invariant impulse response as gk(t) gk(t, 0). This model is an idealization of the actual behavior of a multipath channel, which would not have such a sharply defined impulse response. However, it serves as a useful model for signal processor design and analysis. Note that this model gives rise to frequency-selective fading, since the relative delays will cause constructive and destructive interference at the receiver, depending on the wavelength of propagation. Often, the delays {t, k} are assumed to be known to the receiver or are spaced uniformly at the inverse of the bulk bandwidth of the signaling waveforms. A typical model for the path gains {a, k} is that they are independent complex Gaussian random variables, giving rise to Rayleigh fading.

Note that, in general, the receiver will see the following composite modulation waveform associated with the symbol bk[i]:

Equation 1.11

graphics/01equ011.gif


If these waveforms are not orthogonal for different values of i, ISI will result. Consider, for example, the pure multipath channel of (1.10) with signaling waveforms of the form

Equation 1.12

graphics/01equ012.gif


where sk(·) is a normalized signaling waveform [ |sk(t)|2 dt = 1], Ak is a complex amplitude, and T is the inverse of the single-user symbol rate. In this case, the composite modulation waveforms are given by

Equation 1.13

graphics/01equ013.gif


with

Equation 1.14

graphics/01equ014.gif


If the delay spread (i.e., the maximum of the differences of the delays {t, k} for different values of ) is significant relative to T, ISI may be a factor. Note that for a fixed channel, the delay spread is a function of the physical geometry of the channel, whereas the symbol rate depends on the data rate of the transmitted source. Thus, higher-rate transmissions are more likely to encounter ISI than are lower-rate transmissions. Similarly, if the composite waveforms for different values of k are not orthogonal, MAI will result. This can happen, for example, in CDMA channels when the pseudorandom code sequences used by different users are not orthogonal. It can also happen in CDMA and TDMA channels, due to the effects of multipath or asynchronous transmission. These issues are discussed further in the sequel as the need arises.

This model can be further generalized to account for multiple antennas at the receiver. In particular, we can modify (1.9) as follows:

Equation 1.15

graphics/01equ015.gif


where the boldface quantities denote (column) vectors with dimensions equal to the number of antennas at the received array. For example, the pth component of gk(t, u) is the impulse response of the channel between user k and the pth element of the receiving array. A useful such model is to combine the pure multipath model of (1.10) with a model in which the spatial aspects of the array can be separated from its temporal properties. This yields channel impulse responses of the form

Equation 1.16

graphics/01equ016.gif


where the complex vector a, k describes the response of the array to the th path of user k. The simplest such situation is the case of a uniform linear array (ULA), in which the array elements are uniformly spaced along a line, receiving a single-carrier signal arriving along a planar wavefront and satisfying the narrowband array assumption. The essence of this assumption is that the signaling waveforms are sinusoidal carriers carrying narrowband modulation and that all of the variation in the received signal across the array at any given instant in time is due to the carrier (i.e., the modulating waveform is changing slowly enough to be assumed constant across the array). In this case, the array response depends only on the angle f, k at which the corresponding path's signal is incident on the array. In particular, the response of a P-element array is given in this case by

Equation 1.17

graphics/01equ017.gif


where j denotes the imaginary unit and where graphics/012fig01.gif, with l the carrier wavelength and d the interelement spacing (see [126, 266, 269, 404, 445, 450, 510] for further discussion of systems involving multiple receiver antennas).

It is also of interest to model systems in which there are multiple antennas at both the transmitter and receiver, called multiple-input/multiple-output (MIMO) systems. In this case the channel transfer functions are matrices, with the number of rows equal to the number of receiving antennas and the number of columns equal to the number of transmitting antennas at each source. There are several ways of handling the signaling in such configurations, depending on the desired effects and the channel conditions. For example, transmitter beamforming can be implemented by transmitting the same symbol simultaneously from multiple antenna elements on appropriately phased versions of the same signaling waveform. Space-time coding can be implemented by transmitting frames of related symbols over multiple antennas. Other configurations are of interest as well. Issues concerning multiple-antenna systems are discussed further in the sequel as they arise.


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