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System noise

Fig. 13. Expected signal and noise levels for RE-TM alloys and Pt/Co multilayers (schematic). The total noise entering the SNR is the sum of the system noise, disk noise, and write noise. The system noise is electronic noise and photon shot noise and is comparable for disks with the same reflectivity. Fig. 13. Expected signal and noise levels for RE-TM alloys and Pt/Co multilayers (schematic). The total noise entering the SNR is the sum of the system noise, disk noise, and write noise. The system noise is electronic noise and photon shot noise and is comparable for disks with the same reflectivity.
As femtomolar detection of analytes become more routine, the goal is to achieve attomolar (10 molar) analyte detection, corresponding to the detection of thousands of molecules. Detection sensitivity is enhanced if the noise ia the analytical system can be reduced. System noise consists of two types, extrinsic and intrinsic. Intrinsic aoise, which represents a fundamental limitation linked to the probabiHty of finding the analyte species within the excitation and observation regions of the iastmment, cannot be eliminated. However, extrinsic aoise, which stems from light scatteriag and/or transient electronic sources, can be alleviated. [Pg.395]

Criteria for Acceptable Air-Handling Units and HVAC System Noise Levels... [Pg.800]

Noise generation and erosion/corrosion considerations limit the maximum water velocity in pipework systems. Noise is caused by the free air present in the water, sudden pressure drops (which, in turn, cause cavitation or the flashing of water into steam), turbulence or a combination of these. [Pg.408]

In this section we derive a system equation which describes a drifting calibration line. Let us suppose that the intercept jC (/ + 1) at a time y + 1 is equal to xfj) at a time j augmented by a value a(j), which is the drift. By adding a non-zero system noise to the drift, we express the fact that the drift itself is also time dependent. This leads to the following equations [5,6] ... [Pg.593]

Equations (41.15) and (41.19) for the extrapolation and update of system states form the so-called state-space model. The solution of the state-space model has been derived by Kalman and is known as the Kalman filter. Assumptions are that the measurement noise v(j) and the system noise w(/) are random and independent, normally distributed, white and uncorrelated. This leads to the general formulation of a Kalman filter given in Table 41.10. Equations (41.15) and (41.19) account for the time dependence of the system. Eq. (41.15) is the system equation which tells us how the system behaves in time (here in j units). Equation (41.16) expresses how the uncertainty in the system state grows as a function of time (here in j units) if no observations would be made. Q(j - 1) is the variance-covariance matrix of the system noise which contains the variance of w. [Pg.595]

L0 noise suppression Alixer noise temperature 900 K (DS8) -System noise temperature 1360 K (DSB) -Alixer conversion loss 6 dB (DSB) -20mWat 80 GHz required inW at 160 GHz generated by D162 >TF bandwidth to > 20 GHz... [Pg.251]

Figure 9. A 183 GHz receiver and its system noise temperature as a function of frequency [15]. Figure 9. A 183 GHz receiver and its system noise temperature as a function of frequency [15].
Its special properties offer the possibility of reducing the so-called correlation noise, caused by a limited correlation time. CC is essentially statistical by nature. The system noise (detector noise) is not correlated with the input PRBS the noise in the correlogram, resulting from the detector noise, is converging to zero with increasing correlation time. [Pg.106]

The viscometer assembly is placed in the constant temperature column compartment of the chromatograph between the column outlet and the refractometer. A combination of two Waters Associates M-45 hydraulic filters in series with a capillary tubing coil (length 10 ft., I.D. 0.01 in.) is used to dampen the line pressure fluctuations caused by the pump. With the above pressure damping modifications the overall system noise was reduced to less than 1 millibar at 1.0 ml/min flow rate in tetrahydrofuran (THF) for a set of six p-Styragel columns 10 ,... [Pg.282]

For practical reasons, silicon detectors are usually cooled from room temperature down to approximately — 20°C cooling below — 60°C is not useful because the system noise becomes dominated by the external electronic circuit. Temperatures below — 20°C are not used also because the internal physical stresses from differences... [Pg.556]

There is a substantial amount of material developed for the LQP and its extensions the December, 1971, issue of IEEE Transactions on Automatic Control and a review article by Edgar et al. (47) provide a fairly complete exposition on the effects of non-linearities in the state equations, parameter variations, constraints, disturbances, incomplete measurement, and system noise. There are several general purpose computer programs for solving the LQP, as discussed by Edgar et al (47). [Pg.105]

Noise measurements are extensively used in the studies of metastable pits. Pistorius37 discussed several factors that can influence the proper interpretation of electrochemical noise measurements (ENM). These factors can be probe size, sampling rate, and system noise. The current measurements seem to give clearer information on the corroding system than that of the potential28 46... [Pg.369]

Flicker-noise spectroscopy — The spectral density of - flicker noise (also known as 1// noise, excess noise, semiconductor noise, low-frequency noise, contact noise, and pink noise) increases with frequency. Flicker noise spectroscopy (FNS) is a relatively new method based on the representation of a nonstationary chaotic signal as a sequence of irregularities (such as spikes, jumps, and discontinuities of derivatives of various orders) that conveys information about the time dynamics of the signal [i—iii]. This is accomplished by analysis of the power spectra and the moments of different orders of the signal. The FNS approach is based on the ideas of deterministic chaos and maybe used to identify any chaotic nonstationary signal. Thus, FNS has application to electrochemical systems (-> noise analysis). [Pg.274]

Like sensitivity, LOD depends on the inherent sensitivity of the device itself, as well as the kinetics and thermodynamics of the coating-analyte interaction and the quantity (thickness and/or surface area) of coating available. Unlike sensitivity, however, LOD also depends on the system noise level. The LOD is expressed in terms of the ratio [response when analyte is present]/[noise level when there is no analyte present]. Commonly, LODs are denned as signal-to-noise (S/N) ratios of two or three, corresponding roughly to situations where the signal exceeds the noise at statistical confidence levels of 95% and 99%, respectively [91]. Thus, in the latter case, the LOD can be defined as 3N/sensitivity. The LOD is expressed in units of concentration (e.g., M, fig/L, or iqnn). [Pg.244]

Within the context of this article, the LOD is defined to be the smallest concentration of a sample that can be reliably detected, producing a signal that is three times as large as the standard deviation of the system noise. The ability to improve the LOD can greatly expand the utility of a technique. For example, an improved LOD may allow for the identification of a low abundance sample that would normally be missed in the background of other samples, regardless of the total amount of sample tested. [Pg.131]


See other pages where System noise is mentioned: [Pg.147]    [Pg.147]    [Pg.422]    [Pg.154]    [Pg.246]    [Pg.87]    [Pg.125]    [Pg.125]    [Pg.591]    [Pg.220]    [Pg.250]    [Pg.255]    [Pg.236]    [Pg.642]    [Pg.366]    [Pg.22]    [Pg.154]    [Pg.216]    [Pg.229]    [Pg.147]    [Pg.147]    [Pg.249]    [Pg.253]    [Pg.171]    [Pg.136]    [Pg.194]    [Pg.122]    [Pg.87]   
See also in sourсe #XX -- [ Pg.591 ]




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