PREEMPTIVE CONTROL OF MULTIPLY ACTUATED PROCESSES: APPLICATION TO MOISTURE CONTENT CONTROL IN PAPER MANUFACTURING USING SURROGATE MEASUREMENTS
|
|
- Jasmine Thornton
- 5 years ago
- Views:
Transcription
1 PREEMPTIVE CONTROL OF MULTIPLY ACTUATED PROCESSES: APPLICATION TO MOISTURE CONTENT CONTROL IN PAPER MANUFACTURING USING SURROGATE MEASUREMENTS Perry Y. Li Dept. of Mechanical Engineering Uniersity of Minnesota Minneapolis, Minnesota Petar J. Bjegoic Dept. of Mechanical Engineering Uniersity of Minnesota Minneapolis, Minnesota Shri Ramaswamy Dept. of Wood and Paper Science Uniersity of Minnesota St. Paul, Minnesota ABSTRACT Many manufacturing processes inole the successie processing of the substrate at multiple station on a transport medium, with the hope that at the end of the process, the product has the desired property. Paper manufacturing is an example in which oer 90% of the water from pulp is sequentially remoed through graity, acuum dewatering, pressing, and thermal drying. The consistency and uniformity of the moisture content at the end of process is important for paper quality. Current strategy for the control of moisture content uses a feedback sensor at the end of the process to adjust the dryers. This introduces a long deadtime and causes excessie use of the dryers, which translate to limitations in performance, robustness and inefficient energy usage. In this paper, we inestigate a new control approach in which in-process moisture contents are estimated using air-flow as surrogate measurements, and the pressure settings in the multiple acuum dewatering boxes are adjusted according to the surrogate measurements. A preemptie control algorithm is deeloped which has the ability to decouple and eliminate the effects of the disturbances that occur upstream in the process from downstream. Robustness analysis and simulation studies suggest that as long as the surrogate measurements are accurate, the proposed control scheme will be robust and accurate. 1 Introduction The paper industry in the U.S. alone consumes approximately 2.7 quadrillion Joules ( J) of energy eery year [1]. To be competitie, it is necessary to improe quality and to reduce cost. The two key quality measures are 1) moisture content; and 2) basis weight (weight of paper fiber / m 2 of paper). THIS RESEARCH IS SUPPORTED BY THE TAPPI FOUNDATION AND THE NATIONAL SCIENCE FOUNDATION. headbox graity drainage Figure 1. incoming slurry Circulating wire mesh... acuum dewatering Wet press Dryer section Dryer cans steam pressure Controller Moisture sensor Schematic of a water remoal processes in a paper machine and the current process control strategy These measures must be regulated at desired alues and must be uniform throughout the length and width of the paper produced. Paper manufacturing (Fig. 1) inoles the sequential remoal of water from pulp with 99.5% moisture by means of graity, acuum dewatering, mechanical press, and thermal drying in a paper machine, to form end product with moisture content of 4 8%. Of these, the dryer section is the most energy inefficient but is also currently utilized as the main moisture control actuator. Therefore, an effectie moisture control strategy with proper means can hae significant impact on energy utilization. Currently, acuum dewatering is not actiely inoled in closed loop process control. Rather, pressure settings are determined by operator based on isual inspection. The most important disturbances and uncertainties in the paper making process relate to the composition and the initial water content of the slurry entering the process at the headbox (Fig. 1). Composition in terms of basis weight, types of fibers and their treatments, and chemical addities affect the drainage property of the sheet, and hence the moisture content of the end product. The uncertainties of the composition become een more pronounced when recycled stock is used. Current process control strategy for moisture content makes
2 use of a single online moisture measurement at the end of a paper machine (typically 100m long) to monitor the moisture content of the end product. Based on this measurement, steam pressures in the thermal dryer cans are adjusted ia a ariety of possible control algorithms (e.g. P-I, adaptie [2], stochastic control [3], self-tuning LQ method [9], neuro-fuzzy control [15], self-tuning control [18], model algorithmic control [17], and arious robust control and model predictie control [13]) to remoe more or less water from the paper. This control topology itself presents the following fundamental limitations: 1. It would be too late to take any correctie action for any endproduct that already deiates from specifications. 2. Limited robustness and control performance due to the long deadtime (a few seconds) associated with the 30-60m distance between the actuator in the dryer and the moisture sensor at the output of the process. 3. The thermal dryers are more heaily utilized than are strictly necessary since they are the primary control actuators in the current control strategy. Water that could hae been remoed instead by the more energy efficient acuum dewatering process, is thermally dried instead. This is a major source of energy inefficiency. To oercome these limitations, we are deeloping a new approach to control moisture content, using the acuum dewatering boxes as process control actuators, and in-process estimation of the moisture content of the paper along the length of the paper machine, as the paper is being produced. Results in the literature [4], [16], ours and other s research in Through Air Drying (TAD) [12], [6], [10], [11], [14], and preliminary studies indicate strongly that the magnitude of the air-flow through the wet sheet and the dependence on moisture content contains adequate information to infer the moisture content of the sheet. We call such indirect measurements surrogate measurements. Based on these surrogate measurements, our proposed control strategy is to apply these for local feedback and preemptie feedforward control. Since the moisture content measurements and the actuation are nearly co-located, high feedback gain can be used. The use of preemptie feedforward control would allow us to effectiely decouple disturbances upstream from affecting the downstream process. The oerall potential benefits would be improed accuracy in moisture content control, and more efficient use of energy (since energy use in the dryers can be minimized). In this paper, we inestigate a preemptie control strategy based on the aboe approach to ealuate the usefulness and feasibility of using multiple acuum dewatering boxes and surrogate measurement feedback for the control of moisture content. Since the system inoles continuous process dynamics, described by partial differential equations, a suitable discrete dynamic model in the form of an interconnected system, is first deeloped for control design. Preemptie control law is then deeloped. It can effectiely decouple upstream disturbance from propagating downstream. In addition, local feedback, enabled by the in-process surrogate measurements, enhances robustness to uncertain system parameters. Similar to paper manufacturing, in many other manufacturing processes, e.g. thermal processing of composite material as in tape laying, a substrate is transported successiely to be processed at multiple stations. The product requirements are often specified for the property at the end of the process. Moreoer, the processes are often described by partial differential equations. The modeling techniques as well as the control philosophy enunciated in this paper should also be applicable to these. The rest of the paper is organized as follows. The deelopment of the control design model is gien in Section 2. Section 3 presents the preemptie control algorithm. Section 4 presents the robustness analysis of the control scheme to measurement and model parameter accuracies. Simulation results are presented in section 5 to illustrate the usefulness of the approach. Sections 6 and 7 contain discussion and concluding remarks. 2 Dewatering model for Control Design Following the classical work in acuum dewatering [5], the rate of water remoal is assumed to be proportional to the square root of the applied pressure (or acuum) and to the water content: q = K Pc (1) where q and c are the water remoal rate and the amount of moisture per unit length of the sheet, and K is the transport coefficient. Assume that there are N dewatering boxes, each with length B m, and the constant speed of the paper machine is m/s. Let c(x,t) be the moisture content per unit length of the sheet at location x and time t. This can be conerted to the normal definition of moisture content, which is the amount of moisture per unit total weight of the paper, if the basis weight of the sheet is also known. By incorporating transport into (1), we obtain, ia a mass conseration argument: t c(x,t) = x c(x,t) K(x,t) P(x,t)c(x,t), (2) where the first term corresponds to the transport effect, and the second term corresponds to dewatering. We can consider P(x,t) = P i (t) when x is in the domain of one of the N dewatering box with index i = 1,...,N, and K(x,t) will be the transport coefficient of the sheet at x. Remark 1 Eq.(2) can be generalized for other processes that inole a product quality measure c, whose dynamics without transport, are gien by: dc dt = K g(u) c, where u is the control
3 input that affects the process rate and the process dynamics is linear in the quality measure c. 2.1 One-segment discrete model Although the partial differential equation description in Eq.(2) is complete, it is difficult to use for control design. Simplified discrete models will be more appropriate. To do this, we further assume that the transport coefficient K(x,t) = K i is constant for the i th acuum dewatering box. This is reasonable if the paper machine is operating at a nearly steady state condition. We further assume that the domain of each acuum dewatering box is represented by a single segment. Let c i (y,t) := c(x i + y,t) be the moisture content profile for dewatering box i, where x i is the location of the beginning of the i th dewatering box. Under steady state condition, the profile of the moisture content of the i th dewatering box is gien by c i (y, ) = c i (0, )e K i Pi ( ) y Our main assumption for the discretization of (2) is that within the segment that represents the dewatering box, the exponential profile in Eq.(3) holds at each instant of time. Based on this assumption, the total moisture content w i, defined below, can be used to describe the state of the segment. w i (t) is related to c i (0,t), and hence, to the moisture content profile (3) by B w i (t) = c i (y,t)dy = c i (0,t) 0 K i Pi (t) [ 1 e K i Pi (t) ] B. The state dynamics of w i, for i = 1,...,N (number of dewatering boxes) can now be deried using mass balance principle, which states that the rate of change of total water content within the segment must be equal to the net flow into the control olume. Thus, d dt w i(t) = [c i (B,t) c i 1 (B,t τ i )] K i Pi (t)w i (t), (4) where the first two terms correspond to the net flow due to the translation of the wet sheet and belt in the machine (process) direction, and the third term is due to acuum dewatering. τ i = L i / is the transit time for the sheet to trael between the i 1st and i th dewatering boxes which are L i apart. For i = 1, it is taken to be τ i=1 = 0. Notice that if we define (3) f i (t) := e K i Pi (t) B, (5) Headbox disturbances Wet sheet on translating wire Figure 2. W1 Cout2 W2 W3 Cout Box 1 Total water remoal Total air-flow Moisture content profile Cout1 Box2 Total water remoal Total air-flow Box3 Total water remoal Total air-flow To press s Schematic of the acuum dewatering section of the paper machine in which the one segment model is used to describe the dewatering boxes. we hae c i (B,t) = e K i where Pi (t) B c i (0) = K i Pi (t) f i (t) 1 f 1 (t) w i(t), so that d dt w i(t) = Ω i (t)w i (t) + c i 1,out (t τ i ), (6) Ω i (t) := K i Pi (t) 1 f i (t). (7) The exit moisture content is then related to w i 1 (t) by: c i 1,out (t) = K i 1 Pi 1 (t) f i 1 (t) 1 f i 1 (t) w i 1(t) for i > 1, (8) and c i=0,out (t) denotes the incoming moisture content entering the first acuum dewatering box from the headbox. If we had used n >> 1 (instead of 1) segments to represent each dewatering box, the equialent discretized model of Eq.(4) would become more and more accurate in approximating (2). For the purpose of control design, an adequately accurate model with fewest segments will be the most appropriate. Since the assumption in the model deriation is that the moisture content reaches steady state, it is expected that when the incoming moisture content c i 1,out or the pressure input P i are fast arying, modeling error would be worse. To assess to what extent this is the case, we hae conducted simulation studies comparing modeling errors (measured by the exit moisture content) between the models with arious number of segments and the model with n = 10 segments, which is taken to be the continuum model. Fig. 3 shows that, as expected, the percentage modeling error decreases as the number of segments n increases and for lower disturbance frequencies. Gien typical parameters of = 20m/s, B = 0.05m, and a 10Hz disturbances bandwidth in the incoming moisture content, the percentage modeling error of the one-segment model is less than 3%. Since the moisture content disturbances in the incoming slurry is expected to be only of the order of a few hertz, control design and analysis based on the one-segment model should be adequate.
4 % error Figure 3. Frequency of incoming disturbance/(/b) Discrepancy between arious discrete models and the 10 segment model as a function of the frequency of the inlet water content. Error is measured by the exiting moisture content and is presented as percentage of the exit magnitude of the 10 segment model. 2.2 Surrogate measurement of moisture content For the purpose of this paper, which is to present the adantages of surrogate measurements in the control of moisture content, we assume that the relationship q a = f air (c) is known, where q a is the air-flow per unit length of sheet with moisture content of c. Our current research relates to determining experimentally, this complex function that depends on many factors. Assuming that this can be done, the total air-flow through the sheet in the i th acuum dewatering box is a function of the total moisture content: B Q a,i (t) = f air (c i (y,t))dy = F air,i (w i (t),p i (t)) (9) 0 for some static function F air,i (, ). Since P i is a known control input, using air-flow as a surrogate measurement of the moisture content consists in inerting F air,i (,P i (t)) : w i (t) Q a,i. We assume that this function is inertible for the type of basis weight paper that is being considered. This would be the case if air flow is indeed a alid surrogate measurement of moisture content. 3 Preemptie Control using Surrogate Measurements 3.1 Control problem formulation The objectie of the control algorithm is to adjust the pressure settings in the acuum dewatering boxes based on the feedback of a) the air-flow through the dewatering boxes, and b) the actual moisture content measurement at the output reel of the machine, so that 1) the paper leaing the paper machine has the desired moisture content (normally about 5-6%); 2) the energy used in the dryer cans is minimized; 3) the paper does not seal. The control system will be subject to disturbances in the consistency, material properties, basis weight of the incoming slurry. Uncertainties in plant dynamics and parameters are also expected. Since we desire to utilize the minimal amount of energy in the dryer, we can assume that there is a target moisture content n=1 n=2 n=3 n=5 n=7 alue for the sheet just about to enter the press / dryer section. This target alue should be as low as possible (to minimize energy use of the dryer). The objectie of the control system is then to regulate the moisture content of the sheet as it enters the press / dryer section at the desired alue. Our approach to this control problem is to consider the moisture content profile along the length of the machine. In other words, we specify either a desired total moisture content alue w i or a target exit moisture content alue for each acuum dewatering box i. For simplicity, we define the problem using the total moisture content. Then, the goal of the moisture content profile control is to ensure that the desired total moisture content at each box is attained: i.e. lim t w i (t) w i, i = 1,...,N. We assume that w i, i = 1...N hae been designed and a set of feasible nominal operating pressures P i, i = 1,...,N exists so that together with the nominal incoming moisture content c 0,out, the plant model (6) is satisfied: where Ω i := K i P i 1 f i 0 = ẇ i = Ω i w i + c i 1,out (10), f i := e K i P i B, and K i 1 P i 1 f c i 1 i 1,out = 1 f w i 1 if i > 1 i 1. c 0,out = nominal slurry moisture content if i = 1 Although the ultimate control objectie is at the last dewatering box, i.e. w N (t) w N, the adantage of controlling the profile of moisture content, instead of at the exit alone is that dewatering will be ensured to occur gradually. This in turn minimizes the risk of saturating the control effort in the acuum dewatering boxes, and of sealing. The moisture content profile control concept is similar to the control of traffic profile for automated highway systems [8], and to the problem of transporting cut sheet paper in a copier / printer along a multiplily actuated paperpath so that the sheet arries at the registration station at the correct time [7]. 3.2 Preemptie control law Let e i := w i (t) w i be the moisture content error for the i th dewatering box. It can be shown that ė i (t) = Ω i (t)e i (t) + (Ω i Ω i (t))w i + c i 1,out (t τ i ), (11) where c i 1,out (t τ i ) := c i 1,out (t τ i ) c i 1,out. Notice that Ω i (t) 0 defined in (7) is a monotone increasing function of pressures, so it is inertible for any non-negatie alues. Moreoer, c i 1,out (t τ i ) is aailable using Eq.(8) if w i 1 (t τ i ) and
5 c_i-1,out incoming moisture content c_i-1,out estimated moisture content Smart Vacuum Dewatering Box pressure Figure 4. Controller Vacuum dewatering box Estimator Smart acuum dewatering box c_i,out outgoing moisture content c_i,out estimated outgoing moisture content P i 1 (t τ i ) are aailable. If surrogate measurements are aailable, w i 1 (t τ i ) can be estimated by inerting F air,i (,P i 1 ) in (9). The basic preemptie control strategy is to choose Ω i (t) as Ω i (t) = Ω i + 1 w i [λ f f,i c i 1,out (t τ i ) + λ f b,i e i (t) ] (12) where 1 λ f f,i 0 and λ f b,i 0 are the preemptie feedforward and feedback control gains respectiely. For i = 1, since measurement of the incoming moisture content is not aailable, λ f f,1 = 0. The resulting dynamics are then gien by: ė i (t) = { ( Ω i (t) + λ f b,i ) ei (t) + (1 λ f f,i ) c i 1,out (t τ i ) i > 1 ( Ω 1 (t) + λ f b,1 ) e1 (t) + c 0,out (t) i = 1. (13) Therefore, control law increases the conergence rate using local feedback and compensates for any discrepancy in the incoming moisture content to the present box. In particular, if λ f f,i is chosen to be 1, and λ f b,i 0, then the effect of any upstream disturbances hae been completely decoupled from the i-th box and ė i conerges to 0 exponentially. Using the relationship between the Ω i and c i 1,out in Eq.(10), the preemptie control law in Eq.(12) can be simplified: w i Ω i (t) = [ λ f f,i c i 1,out (t τ i ) + (1 λ f f,i ) c i 1,out] +λ f b,i e i (t). (14) incoming slurry from graity dewatering Smart V.D.box W Smart W Smart Smart... W W V.D.box V.D.box V.D.box W W W W Vacuum dewatering Figure 5. Press and Dryer Block diagram of the control scheme Moisture sensor W The bracketed term in Eq.(14) is a conex combination of the nominal and measured incoming moisture content. Thus, intuitiely, λ f f,i < 1 may be preferable if the estimate of c i 1,out (t) is inaccurate. Notice that for λ f f,i = 1, knowledge of neither Ω i nor of c i 1,out is necessary. Notice that in the control law (12), feedback information (i.e. the air-flow measurement) is utilized locally within the indiidual dewatering boxes and their immediate downstream neighbors. The localization can be conceptualized in terms of a Smart Vacuum Dewatering Box (Fig. 4) which has the ability to robustly control its own moisture content, and to proide an estimate of the moisture content to its neighbors. The complete control scheme which is made up of interconnected Smart Vacuum Dewatering boxes is shown in Fig Robustness analysis 4.1 Inaccuracy in w i estimation Our control scheme is based on the estimation of the moisture content using air-flow as the surrogate measurements. It is important to understand how accuracy in this estimation affects the performance of moisture content control. Assume that ŵ i is the estimate of w i and let w i = ŵ i w i be the estimation error. Then, using ŵ i instead of w i as feedback, the error dynamics become: ė i (t) = ( Ω i (t) + λ f b,i ) ei (t) + (1 λ f f,i ) c i 1,out (t τ i ) [ λ f f,i α i 1 (t τ i ) w i 1 (t τ i ) + λ f b,i w i (t) ] (15) where α i 1 (t) := K i 1 Pi 1 (t) f i 1 (t) 1 f i 1 (t). The ultimate error bound for e i is: e i (t ) (1 λ f f,i) c i 1,out + λ f f,i α i 1 w i 1 + λ f b,i w i where denotes the supremum of the magnitude of the argument, Ω i denotes the lower bound on Ω i (t). Based on typical operating ranges, we expect that 7.5s 1 K i Pi 125s 1, and the residence time B/ 0.003s. Hence, the ranges for B α i 1 (t) and for Ω i (t) are: 1 Bα i 1 (t) 0.7, and /B Ω i (t) 1.2/B. α i (t) generally are smaller and Ω i (i) are larger for boxes that are further downstream. Tighter bounds can be established if indiidual boxes are considered. Assuming that the estimation errors are the same for all dewatering boxes and is gien by w, we obtain e i (t ) (1 λ f f,i ) c i 1,out + B α ib λ f f,i + λ f b,i w (16)
6 which can be used for the design of the feedforward and the feedback gains. For example, if the uncertainty in the incoming moisture content to the i-th box is B c i,out (t) M i w, then the right hand side of (16) will be minimized if and ˆf i (t) = e ˆK i Pi (t) B λ f f,i = { 1 if M i > B α i 0 if M i < B α i. Since α i B is of the order of 1, roughly speaking, if the uncertainty in the incoming moisture content is larger than the accuracy of the moisture content measurement, then preemptie feedforward control should be used. If the aboe preemptie feedforward gain policy is used, then Eq.(16) reduces to: e i (t ) B min( Bα i,m i ) + λ f b,i w. Since Ω i > /B and α i B < 1, λ f b,i should be set to zero! Howeer, for any alue of λ f b,i, the ultimate bound for e i approximately equals the accuracy of the estimate for w i. This means that the feedback gain cannot significantly degrade the accuracy either. We will now show that λ f b,i does play a positie role in combating the effect of model uncertainty. 4.2 Uncertainty in K i We analyze the effect of uncertainty in the dewatering transport coefficients K i. Based on the analysis aboe, we assume that λ f f,i = 1. We also assume that the measurements of w i are correct and estimation of the incoming moisture content for the first box is accurate (c 0,out (t) = c 0,out ). Let ˆK i be the estimate of K i. Let us use the notation ˆΩ i (t) to denote the expression for Ω i (t) in Eq.(7) with K i substituted by ˆK i (including inside f i ), and let ĉ i 1,out (t) denote the expression of c i 1,out (t) in Eq.(8) with K i 1 substituted by ˆK i 1. Then, the computation of the control effort P i will be based on: In the actual situation, the pressure P i (t) would be computed based on ˆΩ i (t) in (17), but applied to Ω i (t) in (7) and then in turn to the error dynamics gien by (10) and (11). Since ˆΩ i (t) and Ω i (t) are positie there exists s i (t) > 0 such that Similarly, we can define so that s i (t) := Ω i(t) ˆΩ i (t) = K i ˆK i 1 ˆf i (t) 1 f i (t). (18) g i (t) := α i(t) ˆα i (t) = s i(t) f i(t) ˆf i (t) = s i(t)e (K i ˆK i ) P i (t) B (19) ĉ i 1,out (t) = ˆα i 1 (t)w i 1 (t) = 1 g i 1 (t) c i 1,out(t). The error dynamics for i = 2,...,N then become: ė i (t) = [ Ω i (t) + s i (t)λ f b ] ei (t) + and for i = 1, ( 1 s i(t) s i 1 (t) e(k i 1 ˆK i 1 ) P i 1 (t τ i ) B ) c i 1,out (t τ i ), (20) ė 1 (t) = [ Ω 1 (t) + s 1 (t)λ f b ] e1 (t) + (1 s 1 (t)) c 0,out (t) (21) Under normal operating conditions, we expect that the exponents in f i (t) and ˆf i (t) are in the range [0.025,0.4], so s i (t) is gien approximately by: w i ˆΩ i (t) = ĉ i 1,out (t τ i ) + λ f b,i e i (t) (17) s i (t) K i [1 (1 + ˆK i Pi (t)b/)] ˆK i [1 (1 + K i Pi (t)b/)] = 1. where ĉ i 1,out (t) ˆα i 1 (t) { }}{ ˆK = i 1 Pi 1 (t) ˆf i 1 (t) 1 ˆf i 1 (t) w i 1(t) for i > 1, = nominal incoming moisture content for i = 1 c 0,out Therefore, the dynamics of e i, i = 2...,N and i = 1, due to uncertain K i and K i 1 are approximately gien by: ė i (t) [ ] Ω i (t) + s i (t)λ f b,i ei (t) ( ) + 1 e (K i 1 ˆK i 1 ) P i 1 (t τ i ) B c i 1,out (t τ i ) ė 1 (t) [ Ω 1 (t) + s 1 (t)λ f b,1 ] e1 (t) (22)
7 From (22), we can obsere firstly that uncertainty in K i only has a benign effect on the feedback action by changing the effectie feebback gain from λ f b,i to s i (t)λ f b,i. In particular, for i = 1, uncertainty in K 1 does not introduce errors. Secondly, unlike the case of uncertain measurements w i (t), the feedback gain λ f b,i can be used positiely to combat the aderse effect introduced by the uncertainty in K i 1. For example, we can see that e i (t ) c i 1,out( ) Ω i ( ) + s i ( )λ f b,i 1 e K i 1 Pi 1 ( ) B, where s i ( ) is the lower bound of s i (t 0). Thus, by increasing λ f b,i, the effect of the uncertainty in K i 1 will be decreased. Total moisture content m Actual and desired total moisture contents (without control) Box 1 Box 2 Box 3 Box 4 Box 5 Box 6 Box 7 Box 8 Box 9 5 Simulations The proposed control system is simulated for paper machine with N=10 dewatering boxes of length B = 0.05m and with machine speed of 20m/s. The transport coefficient K i decreases from K 1 = 0.6s 1 Pa 1/2 to K 10 = 0.1s 1 Pa 1/2, and the desired total moisture contents, which are designed based on increasing nominal pressures from 4500Pa to 70000Pa, decreases from w 1 = to w 10 = The nominal incoming moisture content c out,0 is 15kg/m. In all situations, λ f f,i = 1, λ f b,i = /B = 400sec 1. To be realistic, saturation limits (about ±10% of nominal alues) are imposed on the input pressures. Table lookup is used to inert the nonlinear function Ω i (t) (specified by the control law (14)) to obtain P i (t). First, we consider the situation when there are a 10Hz sinusoidal disturbance (10%) at the incoming moisture content, and a 7Hz sinuoidal disturbance (8%) before the 5th dewatering box. The latter simulates a leaking water pipe in the middle of the factory. Figure 6 shows the total moisture contents with and without the preemptie controller. Without control, moisture content deiation at box 10 is about 10%. With control, the moisture content w i conerges to the desired alues for the 4th and the last box. At the other boxes, the effect of the disturbances has been significantly attenuated. Conergence does not occurs for some of the boxes because of saturation at the upper pressure limits. Figure 7 shows the situation when 10% inaccuracy in moisture content measurements are introduced. Notice that the moisture content conerges to region close to the desired alue with an accuracy commensurate with the accuracy of the moisture content estimation. Thus, the accuracy of the moisture content estimation is ery important to the proposed scheme. Figure 8 shows the moisture content of the last dewatering box when all the transport coefficients are 10% different from nominal, with feedback (λ f b,i = 400/s) and without feedback (λ f b,i = 0). Een without feedback, only about 2% error is introduced. When feedback control is applied, the error is further reduced to 1.29%. Total moisture content m Box Time s Solid actual W i Dashed desired W i Actual and desired total moisture contents (with control) Box 4 Box 1 Box 2 Box 5 Box 3 Box 6 Box 7 Box 8 Box 9 Box Time s Figure 6. Desired and actual total moisture content (w i, i = 1,...,N) when a 10Hz, 10% ariation moisture content disturbance, and a 7Hz, 8% ariation disturbance are introduced at the first dewatering and the 5th box respectiely. Top: no control; bottom: with preemptie control. Wi Nominal and archieed Wi with 10% biased measurements Box 2 Box 5 Box Time(s) Figure 7. Time trajectories of total moisture content at boxes 2, 5, 10 when 10% error in estimation of the moisture content is introduced.
8 W Uncertain K, results for Box 10 with and without feedback without feedback with feedback Box 10 desired alue 7 Conclusions A new approach for the control of moisture content for paper manufacturing has been proposed. The approach makes use of acuum dewatering and surrogate in-process measurement of the moisture content based on air-flow measurements. Potentially, such an approach can compensate preemptiely for any upstream disturbances. A preemptie control algorithm for the interconnected acuum dewatering system based on a discrete control model has been deeloped. Analysis and simulations show that the algorithm is effectie and robust to measurement inaccuracy and to uncertainty in system parameters Figure 8. Time (s) Time trajectories of moisture content at boxes 2, 5, 10 with 10% error in the transport coefficients K i s. 6 Discussion Analysis and simulations in sections 4 and 5 suggest that if accurate in-process moisture measurements are aailable, moisture content can be quite accurately controlled such that the moisture content at the dewatering boxes downstream become decoupled from the upstream disturbances. In addition, certain amount of robustness to uncertainty in transport coefficients can also be tolerated, especially if the feedback gains λ f b,i s are increased. Direct adaptie technique based on (21) or (22) may be possible (especially for small uncertainty in K i ). The difficulty here lies in that K i is nonlinearly embedded in the error dynamics. The effect of control saturation, as demonstrated in the simulations, is that the disturbances cannot be eliminated completely by one dewatering box. Howeer, as the error is propagated downstream, the size of the disturbance also decreases so that the error can eentually be eliminated in the downstream boxes without saturating the control. Since the actual requirement is to control the moisture content at the last dewatering box, this may not pose a signficant problem. The question of whether to eliminate error using ery few dewatering boxes with little saturation limits, or using a larger number of boxes with stricter saturation limits is interesting. This is similar to the controllability analysis of a multiply actuated paper path of a printer / copier [7]. Since the aailability and accuracy of the moisture content estimates from air-flow measurement is critical to the success of our approach, our current research aims to experimentally deelop such a model. Other possibilities that we are exploring include deeloping adaptie calibration techniques for the air-flow-moisture relationship based on existing actual moisture content measurement at the end of the process, and deeloping control for the actual exit moisture content (instead of total moisture content) for each dewatering box. References [1] Anonymous. Paper Industry Research Needs. Tappi Foundation, Atlanta, GA, [2] K. J. Astrom. Control problems in paper making. In IBM Scientific Computing Symposium, [3] K. J. Astrom. Computer control of a paper machine - an application of linear stochastic control theory. IBM Journal of Re. De., 11: , [4] E. Brundrett and D. Baines. The flow of air through wet paper. Tappi Journal, 49(3), [5] E. Cowan. A theory of drainage relation to the wire section of the paper machine. Pulp and Paper Magazine fo Canada, 38, [6] Y. Cui, S. Ramaswamy, and C. Tourigny. through air drying of tissue and towel. Tappi Journal, 82(44): , [7] M. Krucinski, C. Cloet, M. Tomizuka, R. Horowitz, and P. Y. Li. Intersheet spacing control and controllability of a copier paperpath. In Proceedings of the IEEE Conference on Control Applications, Trieste, Italy, [8] P. Li, R. Horowitz, Alarez, J. Frankel, and A. Robertson. An Automated Highway Link Layer Controller for Traffic Flow Stabilization. Transportation Research - Part C: Emerging Technology, pages 11 37, Feb [9] A. Lizr. Linear quadratic self-tuning regulators in paper-machine control systems. In Proc. of the 2nd IFAC workshop, pages , [10] O. Polat, R. H. Crotogino, and W. J. M. Douglas. Transport phenomena analysis of through air drying of paper. Industrial Engineering Chemistry Research, 31(3):736, [11] O. Polat, W. J. M. Douglas, and R. H. Crotogino. Experimental study of through air drying of paper. In Proceedings of Drying 1987, page 290, [12] S. Ramaswamy, Y. Cui, and C. Tourigny. analysis of conectie heat and mass transfer in through air drying of paper. In AIChE Symposium Series on Fundamental Adances and Innoations in the Pulp and Paper Industry, olume 95, pages 89 98, [13] M. Rao, Q. Zia, and Y. Ying. Modeling and adanced control for process industries - applications to paper making processes. Springer-Verlag, [14] M. Tietz and E. U. Schlunder. Through air drying of paper Par 1: Suction drum design from constant air flow data. Chemical Engineering and Processing, 32: , [15] H. Wang. Applying neuro-fuzzy modelling and model to md moisture content systems in paper machines. In Proceedings of the IEEE Conference on Control Applications, pages , [16] O. Washburn and J. Buchanan. The surface and tensile fractures of groundwood handsheets as obsered with scanning electron microscopy. Pulp Paper Magazine of Canada, 65(2):52 64, [17] Q. Xia, M. Rao, and J. Qian. Model algorithmic control (mac) for paper machines. In Proceedings of the IEEE Conference on Control Applications, pages , [18] Q. Xia, M. Rao, X. Shen, and H. Zhu. Adaptie control of basis weight and moisture content for a paperboard machine. Journal of Process Control, 3(4): , 1993.
Probabilistic Engineering Design
Probabilistic Engineering Design Chapter One Introduction 1 Introduction This chapter discusses the basics of probabilistic engineering design. Its tutorial-style is designed to allow the reader to quickly
More informationPosition in the xy plane y position x position
Robust Control of an Underactuated Surface Vessel with Thruster Dynamics K. Y. Pettersen and O. Egeland Department of Engineering Cybernetics Norwegian Uniersity of Science and Technology N- Trondheim,
More informationReversal in time order of interactive events: Collision of inclined rods
Reersal in time order of interactie eents: Collision of inclined rods Published in The European Journal of Physics Eur. J. Phys. 27 819-824 http://www.iop.org/ej/abstract/0143-0807/27/4/013 Chandru Iyer
More informationTransmission lines using a distributed equivalent circuit
Cambridge Uniersity Press 978-1-107-02600-1 - Transmission Lines Equialent Circuits, Electromagnetic Theory, and Photons Part 1 Transmission lines using a distributed equialent circuit in this web serice
More informationSELECTION, SIZING, AND OPERATION OF CONTROL VALVES FOR GASES AND LIQUIDS Class # 6110
SELECTION, SIZIN, AND OERATION OF CONTROL VALVES FOR ASES AND LIUIDS Class # 6110 Ross Turbiille Sales Engineer Fisher Controls International Inc. 301 S. First Aenue Marshalltown, Iowa USA Introduction
More informationTrajectory Estimation for Tactical Ballistic Missiles in Terminal Phase Using On-line Input Estimator
Proc. Natl. Sci. Counc. ROC(A) Vol. 23, No. 5, 1999. pp. 644-653 Trajectory Estimation for Tactical Ballistic Missiles in Terminal Phase Using On-line Input Estimator SOU-CHEN LEE, YU-CHAO HUANG, AND CHENG-YU
More informationMATHEMATICAL MODELLING AND IDENTIFICATION OF THE FLOW DYNAMICS IN
MATHEMATICAL MOELLING AN IENTIFICATION OF THE FLOW YNAMICS IN MOLTEN GLASS FURNACES Jan Studzinski Systems Research Institute of Polish Academy of Sciences Newelska 6-447 Warsaw, Poland E-mail: studzins@ibspan.waw.pl
More informationDynamic Vehicle Routing with Moving Demands Part II: High speed demands or low arrival rates
ACC 9, Submitted St. Louis, MO Dynamic Vehicle Routing with Moing Demands Part II: High speed demands or low arrial rates Stephen L. Smith Shaunak D. Bopardikar Francesco Bullo João P. Hespanha Abstract
More informationMean-variance receding horizon control for discrete time linear stochastic systems
Proceedings o the 17th World Congress The International Federation o Automatic Control Seoul, Korea, July 6 11, 008 Mean-ariance receding horizon control or discrete time linear stochastic systems Mar
More informationVISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION
VISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION Predict Obsere Explain Exercise 1 Take an A4 sheet of paper and a heay object (cricket ball, basketball, brick, book, etc). Predict what will
More informationAnalysis of cylindrical heat pipes incorporating the e ects of liquid±vapor coupling and non-darcian transportða closed form solution
International Journal of Heat and Mass Transfer 42 (1999) 3405±341 Analysis of cylindrical heat pipes incorporating the e ects of liquid±apor coupling and non-darcian transportða closed form solution N.
More informationReal Gas Thermodynamics. and the isentropic behavior of substances. P. Nederstigt
Real Gas Thermodynamics and the isentropic behaior of substances. Nederstigt ii Real Gas Thermodynamics and the isentropic behaior of substances by. Nederstigt in partial fulfillment of the requirements
More informationAstrometric Errors Correlated Strongly Across Multiple SIRTF Images
Astrometric Errors Correlated Strongly Across Multiple SIRTF Images John Fowler 28 March 23 The possibility exists that after pointing transfer has been performed for each BCD (i.e. a calibrated image
More informationTheory of Network Communication
Theory of Network Communication Dr. Christian Scheideler Johns Hopkins Uniersity, Sept. 9 2002 Introduction The goal of this lecture is to gie an introduction to the state of the art in the theory of network
More information4. A Physical Model for an Electron with Angular Momentum. An Electron in a Bohr Orbit. The Quantum Magnet Resulting from Orbital Motion.
4. A Physical Model for an Electron with Angular Momentum. An Electron in a Bohr Orbit. The Quantum Magnet Resulting from Orbital Motion. We now hae deeloped a ector model that allows the ready isualization
More informationOptimal Switching of DC-DC Power Converters using Approximate Dynamic Programming
Optimal Switching of DC-DC Power Conerters using Approximate Dynamic Programming Ali Heydari, Member, IEEE Abstract Optimal switching between different topologies in step-down DC-DC oltage conerters, with
More informationTools for Investigation of Dynamics of DC-DC Converters within Matlab/Simulink
Tools for Inestigation of Dynamics of DD onerters within Matlab/Simulink Riga Technical Uniersity, Riga, Latia Email: pikulin03@inbox.l Dmitry Pikulin Abstract: In this paper the study of complex phenomenon
More informationPatterns of Non-Simple Continued Fractions
Patterns of Non-Simple Continued Fractions Jesse Schmieg A final report written for the Uniersity of Minnesota Undergraduate Research Opportunities Program Adisor: Professor John Greene March 01 Contents
More informationState-space Modelling of Hysteresis-based Control Schemes
European Control Conference (ECC) July 7-9,, Zürich, Switzerland. State-space Modelling of Hysteresis-based Control Schemes Soumya Kundu Ian A. Hiskens Abstract The paper deelops a state-space model for
More informationNonlinear Disturbance Decoupling for a Mobile Robotic Manipulator over Uneven Terrain
Nonlinear Disturbance Decoupling for a Mobile Robotic Manipulator oer Uneen Terrain Joel Jimenez-Lozano Bill Goodwine Department of Aerospace and Mechanical Engineering Uniersity of Noe Dame Noe Dame IN
More informationSection 6: PRISMATIC BEAMS. Beam Theory
Beam Theory There are two types of beam theory aailable to craft beam element formulations from. They are Bernoulli-Euler beam theory Timoshenko beam theory One learns the details of Bernoulli-Euler beam
More informationExponential stability of PI control for Saint-Venant equations
Exponential stability of PI control for Saint-Venant equations Georges Bastin and Jean-Michel Coron February 28, 218 Abstract We consider open channels represented by Saint-Venant equations that are monitored
More informationDetection of Critical Driving Situations using Phase Plane Method for Vehicle Lateral Dynamics Control by Rear Wheel Steering
Proceedings of the 7th World Congress The International Federation of Automatic Control Seoul, Korea, July 6-, 28 Detection of Critical Driing Situations using Phase Plane Method for Vehicle Lateral Dynamics
More informationFinal Exam (Solution) Economics 501b Microeconomic Theory
Dirk Bergemann and Johannes Hoerner Department of Economics Yale Uniersity Final Exam (Solution) Economics 5b Microeconomic Theory May This is a closed-book exam. The exam lasts for 8 minutes. Please write
More informationLecture 1. 1 Overview. 2 Maximum Flow. COMPSCI 532: Design and Analysis of Algorithms August 26, 2015
COMPSCI 532: Design and Analysis of Algorithms August 26, 205 Lecture Lecturer: Debmalya Panigrahi Scribe: Allen Xiao Oeriew In this lecture, we will define the maximum flow problem and discuss two algorithms
More informationDynamic Vehicle Routing with Heterogeneous Demands
Dynamic Vehicle Routing with Heterogeneous Demands Stephen L. Smith Marco Paone Francesco Bullo Emilio Frazzoli Abstract In this paper we study a ariation of the Dynamic Traeling Repairperson Problem DTRP
More informationModeling Hydraulic Accumulators for use in Wind Turbines
The 13th Scandinaian International Conference on Fluid Power, SICFP213, une 3-5, 213, Linköping, Sweden Modeling Hydraulic Accumulators for use in Wind Turbines Henrik Brun Hansen and Peter Windfeld Rasmussen
More informationSolution to 1-D consolidation of non-homogeneous soft clay *
Xie et al. / J Zhejiang Uni SCI 25 6A(Suppl. I):29-34 29 Journal of Zhejiang Uniersity SCIENCE ISSN 19-395 http://www.zju.edu.cn/jzus E-mail: jzus@zju.edu.cn Solution to 1-D consolidation of non-homogeneous
More information0 a 3 a 2 a 3 0 a 1 a 2 a 1 0
Chapter Flow kinematics Vector and tensor formulae This introductory section presents a brief account of different definitions of ector and tensor analysis that will be used in the following chapters.
More information4 Fundamentals of Continuum Thermomechanics
4 Fundamentals of Continuum Thermomechanics In this Chapter, the laws of thermodynamics are reiewed and formulated for a continuum. The classical theory of thermodynamics, which is concerned with simple
More informationMOTION OF FALLING OBJECTS WITH RESISTANCE
DOING PHYSICS WIH MALAB MECHANICS MOION OF FALLING OBJECS WIH RESISANCE Ian Cooper School of Physics, Uniersity of Sydney ian.cooper@sydney.edu.au DOWNLOAD DIRECORY FOR MALAB SCRIPS mec_fr_mg_b.m Computation
More informationDynamic Vehicle Routing for Translating Demands: Stability Analysis and Receding-Horizon Policies
1 Dynamic Vehicle Routing for Translating Demands: Stability Analysis and Receding-Horizon Policies Shaunak D. Bopardikar Stephen L. Smith Francesco Bullo João P. Hespanha Abstract We introduce a problem
More informationAlternative non-linear predictive control under constraints applied to a two-wheeled nonholonomic mobile robot
Alternatie non-linear predictie control under constraints applied to a to-heeled nonholonomic mobile robot Gaspar Fontineli Dantas Júnior *, João Ricardo Taares Gadelha *, Carlor Eduardo Trabuco Dórea
More informationIntroduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles
Introduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles by James Doane, PhD, PE Contents 1.0 Course Oeriew... 4.0 Basic Concepts of Thermodynamics... 4.1 Temperature
More informationMagnetic Fields Part 3: Electromagnetic Induction
Magnetic Fields Part 3: Electromagnetic Induction Last modified: 15/12/2017 Contents Links Electromagnetic Induction Induced EMF Induced Current Induction & Magnetic Flux Magnetic Flux Change in Flux Faraday
More informationFUZZY FINITE ELEMENT METHOD AND ITS APPLICATION
TRENDS IN COMPUTATIONAL STRUCTURAL MECHANICS W.A. Wall, K.U. Bletzinger and K. Schweizerhof (Eds.) CIMNE, Barcelona, Spain 2001 FUZZY FINITE ELEMENT METHOD AND ITS APPLICATION B. Möller*, M. Beer, W. Graf
More informationSimulations of bulk phases. Periodic boundaries. Cubic boxes
Simulations of bulk phases ChE210D Today's lecture: considerations for setting up and running simulations of bulk, isotropic phases (e.g., liquids and gases) Periodic boundaries Cubic boxes In simulations
More informationLECTURE NOTE THERMODYNAMICS (GEC 221)
LETURE NOTE ON THERMODYNAMIS (GE ) Thermodynamics is the branch of science that treats the arious phenomena of energy and related properties of matter especially the relationship between heat, work and
More informationParameters Identification of Equivalent Circuit Diagrams for Li-Ion Batteries
Parameters Identification of Equialent Circuit Diagrams for Li-Ion eries Ahmad ahmoun, Helmuth Biechl Uniersity of Applied ciences Kempten Ahmad.ahmoun@stud.fh-empten.de, biechl@fh-empten.de Abstract-eries
More informationOn resilience of distributed routing in networks under cascade dynamics
On resilience of distributed routing in networks under cascade dynamics Ketan Sala Giacomo Como Munther A. Dahleh Emilio Frazzoli Abstract We consider network flow oer graphs between a single origin-destination
More informationDESIGN METHOD BASED ON THE CONCEPT OF EMERGENCE AND ITS APPLICATION
DESIGN METHOD BASED ON THE CONCEPT OF EMERGENCE AND ITS APPLICATION Koichiro Sato¹ and Yoshiyuki Matsuoka 2 ¹ Graduate School of Science and Technology, Keio Uniersity, Yokohama, Japan Koichiro_Sato@a7.keio.jp,
More informationLect-19. In this lecture...
19 1 In this lecture... Helmholtz and Gibb s functions Legendre transformations Thermodynamic potentials The Maxwell relations The ideal gas equation of state Compressibility factor Other equations of
More informationRelativistic Energy Derivation
Relatiistic Energy Deriation Flamenco Chuck Keyser //4 ass Deriation (The ass Creation Equation ρ, ρ as the initial condition, C the mass creation rate, T the time, ρ a density. Let V be a second mass
More informationChapter 7: The Second Law of Thermodynamics
Chapter 7: he Second Law of hermodynamics he second law of thermodynamics asserts that processes occur in a certain direction and that the energy has quality as well as quantity he first law places no
More informationChapter 14 Thermal Physics: A Microscopic View
Chapter 14 Thermal Physics: A Microscopic View The main focus of this chapter is the application of some of the basic principles we learned earlier to thermal physics. This will gie us some important insights
More informationME224 Lab 5 - Thermal Diffusion
ME4 Lab 5 ME4 Lab 5 - hermal Diffusion (his lab is adapted from IBM-PC in the laboratory by B G homson & A F Kuckes, Chapter 5) 1. Introduction he experiments which you will be called upon to do in this
More informationComputing Laboratory A GAME-BASED ABSTRACTION-REFINEMENT FRAMEWORK FOR MARKOV DECISION PROCESSES
Computing Laboratory A GAME-BASED ABSTRACTION-REFINEMENT FRAMEWORK FOR MARKOV DECISION PROCESSES Mark Kattenbelt Marta Kwiatkowska Gethin Norman Daid Parker CL-RR-08-06 Oxford Uniersity Computing Laboratory
More informationChapter 6: Operational Amplifiers
Chapter 6: Operational Amplifiers Circuit symbol and nomenclature: An op amp is a circuit element that behaes as a VCVS: The controlling oltage is in = and the controlled oltage is such that 5 5 A where
More informationUNIVERSITY OF TRENTO ITERATIVE MULTI SCALING-ENHANCED INEXACT NEWTON- METHOD FOR MICROWAVE IMAGING. G. Oliveri, G. Bozza, A. Massa, and M.
UNIVERSITY OF TRENTO DIPARTIMENTO DI INGEGNERIA E SCIENZA DELL INFORMAZIONE 3823 Poo Trento (Italy), Via Sommarie 4 http://www.disi.unitn.it ITERATIVE MULTI SCALING-ENHANCED INEXACT NEWTON- METHOD FOR
More informationVariance Reduction for Stochastic Gradient Optimization
Variance Reduction for Stochastic Gradient Optimization Chong Wang Xi Chen Alex Smola Eric P. Xing Carnegie Mellon Uniersity, Uniersity of California, Berkeley {chongw,xichen,epxing}@cs.cmu.edu alex@smola.org
More informationOPTIMIZATION OF FLOWS AND ANALYSIS OF EQUILIBRIA IN TELECOMMUNICATION NETWORKS
OPTIMIZATION OF FLOWS AND ANALYSIS OF EQUILIBRIA IN TELECOMMUNICATION NETWORKS Ciro D Apice (a, Rosanna Manzo (b, Luigi Rarità (c (a, (b, (c Department of Information Engineering and Applied Mathematics,
More informationERAD THE SEVENTH EUROPEAN CONFERENCE ON RADAR IN METEOROLOGY AND HYDROLOGY
Multi-beam raindrop size distribution retrieals on the oppler spectra Christine Unal Geoscience and Remote Sensing, TU-elft Climate Institute, Steinweg 1, 68 CN elft, Netherlands, c.m.h.unal@tudelft.nl
More informationPOSITION CONTROL OF AN INTERIOR PERMANENT MAGNET SYNCHRONOUS MOTOR BY USING ADAPTIVE BACK STEPPING ALGORITHM
Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 3, May-Jun 212, pp.27-276 POSITION CONTROL OF AN INTERIOR PERMANENT MAGNET SYNCHRONOUS MOTOR BY USING ADAPTIVE BACK STEPPING
More informationThe perturbed Riemann problem for the chromatography system of Langmuir isotherm with one inert component
Aailable online at www.tjnsa.com J. Nonlinear Sci. Appl. 9 2016, 5382 5397 Research Article The perturbed Riemann problem for the chromatography system of Langmuir isotherm with one inert component Pengpeng
More informationCONSTRUCTION PROCESS NUMERICAL SIMULATION AND SEISMIC ASSESSMENT OF MALLORCA CATHEDRAL
CONSTRUCTION PROCESS NUMERICAL SIMULATION AND SEISMIC ASSESSMENT OF MALLORCA CATHEDRAL Roca, Pere 1 ; Pelà, Luca 2 ; Cerera, Miguel 3 ; Clemente, Roberto 4 1 PhD, Professor, Technical Uniersity of Catalonia
More informationTwo-Dimensional Variational Analysis of Near-Surface Moisture from Simulated Radar Refractivity-Related Phase Change Observations
ADVANCES IN ATMOSPHERIC SCIENCES, VOL. 30, NO. 2, 2013, 291 305 Two-Dimensional Variational Analysis of Near-Surface Moisture from Simulated Radar Refractiity-Related Phase Change Obserations Ken-ichi
More informationCollective Risk Models with Dependence Uncertainty
Collectie Risk Models with Dependence Uncertainty Haiyan Liu and Ruodu Wang ebruary 27, 2017 Abstract We bring the recently deeloped framework of dependence uncertainty into collectie risk models, one
More informationEconometrics II - EXAM Outline Solutions All questions have 25pts Answer each question in separate sheets
Econometrics II - EXAM Outline Solutions All questions hae 5pts Answer each question in separate sheets. Consider the two linear simultaneous equations G with two exogeneous ariables K, y γ + y γ + x δ
More informationEvolution Analysis of Iterative LMMSE-APP Detection for Coded Linear System with Cyclic Prefixes
Eolution Analysis of Iteratie LMMSE-APP Detection for Coded Linear System with Cyclic Prefixes Xiaoun Yuan Qinghua Guo and Li Ping Member IEEE Department of Electronic Engineering City Uniersity of Hong
More informationTarget Trajectory Estimation within a Sensor Network
Target Trajectory Estimation within a Sensor Network Adrien Ickowicz IRISA/CNRS, 354, Rennes, J-Pierre Le Cadre, IRISA/CNRS,354, Rennes,France Abstract This paper deals with the estimation of the trajectory
More informationA Regularization Framework for Learning from Graph Data
A Regularization Framework for Learning from Graph Data Dengyong Zhou Max Planck Institute for Biological Cybernetics Spemannstr. 38, 7076 Tuebingen, Germany Bernhard Schölkopf Max Planck Institute for
More informationSIMULATIONS OF CHARACTERISTICS OF TUNED LIQUID COLUMN DAMPER USING AN ELLIPTICAL FLOW PATH ESTIMATION METHOD
October -7, 008, Beijing, China SIMULATIONS OF CHARACTERISTICS OF TUNED LIQUID COLUMN DAMPER USING AN ELLIPTICAL FLOW PATH ESTIMATION METHOD P. Chaiiriyawong, S. Limkatanyu and T. Pinkaew 3 Lecturer, Dept.
More informationA possible mechanism to explain wave-particle duality L D HOWE No current affiliation PACS Numbers: r, w, k
A possible mechanism to explain wae-particle duality L D HOWE No current affiliation PACS Numbers: 0.50.-r, 03.65.-w, 05.60.-k Abstract The relationship between light speed energy and the kinetic energy
More informationAdsorption of Pure Methane, Nitrogen, and Carbon Dioxide and Their Mixtures on San Juan Basin Coal
Adsorption of Pure Methane, Nitrogen, and Carbon Dioxide and Their Mixtures on San Juan Basin Coal Topical Report January, 2001 March, 2002 K. A. M. Gasem R. L. Robinson, Jr. S.R. Reees Contract No. DE-FC26-00NT40924
More informationFu Yuhua 1. Beijing, China
85 An Example of Guiding Scientific Research with hilosophical rinciples Based on Uniqueness of Truth and Neutrosophy eriing Newton's Second Law and the like Fu Yuhua 1 1 CNOOC Research Institute Beijing,
More informationCross Directional Control
Cross Directional Control Graham C. Goodwin Day 4: Lecture 4 16th September 2004 International Summer School Grenoble, France 1. Introduction In this lecture we describe a practical application of receding
More informationNotes on Linear Minimum Mean Square Error Estimators
Notes on Linear Minimum Mean Square Error Estimators Ça gatay Candan January, 0 Abstract Some connections between linear minimum mean square error estimators, maximum output SNR filters and the least square
More informationOnline Companion to Pricing Services Subject to Congestion: Charge Per-Use Fees or Sell Subscriptions?
Online Companion to Pricing Serices Subject to Congestion: Charge Per-Use Fees or Sell Subscriptions? Gérard P. Cachon Pnina Feldman Operations and Information Management, The Wharton School, Uniersity
More informationThe Kinetic Theory of Gases
978-1-107-1788-3 Classical and Quantum Thermal Physics The Kinetic Theory of Gases CHAPTER 1 1.0 Kinetic Theory, Classical and Quantum Thermodynamics Two important components of the unierse are: the matter
More informationSEG/San Antonio 2007 Annual Meeting
Characterization and remoal of errors due to magnetic anomalies in directional drilling Nathan Hancock * and Yaoguo Li Center for Graity, Electrical, and Magnetic studies, Department of Geophysics, Colorado
More informationVelocity, Acceleration and Equations of Motion in the Elliptical Coordinate System
Aailable online at www.scholarsresearchlibrary.com Archies of Physics Research, 018, 9 (): 10-16 (http://scholarsresearchlibrary.com/archie.html) ISSN 0976-0970 CODEN (USA): APRRC7 Velocity, Acceleration
More informationV. Transistors. 3.1 III. Bipolar-Junction (BJT) Transistors
V. Transistors 3.1 III. Bipolar-Junction (BJT) Transistors A bipolar junction transistor is formed by joining three sections of semiconductors with alternatiely different dopings. The middle section (base)
More informationDynamic Vehicle Routing with Moving Demands Part II: High speed demands or low arrival rates
Dynamic Vehicle Routing with Moing Demands Part II: High speed demands or low arrial rates Stephen L. Smith Shaunak D. Bopardikar Francesco Bullo João P. Hespanha Abstract In the companion paper we introduced
More informationA study of jacking force for a curved pipejacking
Journal of Rock Mechanics and Geotechnical Engineering. 200, 2 (4): 298 304 A study of jacking force for a cured pipejacking K. J. Shou, J. M. Jiang Department of Ciil Engineering, National Chung Hsing
More informationChapter 1. The Postulates of the Special Theory of Relativity
Chapter 1 The Postulates of the Special Theory of Relatiity Imagine a railroad station with six tracks (Fig. 1.1): On track 1a a train has stopped, the train on track 1b is going to the east at a elocity
More informationA matrix Method for Interval Hermite Curve Segmentation O. Ismail, Senior Member, IEEE
International Journal of Video&Image Processing Network Security IJVIPNS-IJENS Vol:15 No:03 7 A matrix Method for Interal Hermite Cure Segmentation O. Ismail, Senior Member, IEEE Abstract Since the use
More informationTowards Green Distributed Storage Systems
Towards Green Distributed Storage Systems Abdelrahman M. Ibrahim, Ahmed A. Zewail, and Aylin Yener Wireless Communications and Networking Laboratory (WCAN) Electrical Engineering Department The Pennsylania
More informationInvestigation on Ring Valve Motion and Impact Stress in Reciprocating Compressors
Purdue Uniersity Purdue e-pubs International Compressor Engineering Conference School of Mechanical Engineering 2010 Inestigation on Ring Vale Motion and Impact Stress in Reciprocating Compressors Yu Wang
More informationInterpreting enzyme and receptor kinetics: keeping it simple, but not too simple 1
Nuclear Medicine and Biology 30 (2003) 819 826 www.elseier.com/locate/nucmedbio Interpreting enzyme and receptor kinetics: keeping it simple, but not too simple 1 Kenneth A. Krohn *, Jeanne M. Link Department
More informationarxiv: v1 [stat.ml] 15 Feb 2018
1 : A New Algorithm for Streaming PCA arxi:1802.054471 [stat.ml] 15 Feb 2018 Puyudi Yang, Cho-Jui Hsieh, Jane-Ling Wang Uniersity of California, Dais pydyang, chohsieh, janelwang@ucdais.edu Abstract In
More informationThe hierarchical real-time control of high speed trains for automatic train operation
Computers in Railways XIV 17 The hierarchical real-time control of high speed trains for automatic train operation Q. Y. Wang, P. Wu, Z. C. Liang & X. Y. Feng Southwest Jiaotong Uniersity, China Abstract
More informationAerodynamic Admittance Function of Tall Buildings
Aerodynamic Admittance Function o Tall Buildings in hou a Ahsan Kareem b a alou Engineering Int l, Inc., 75 W. Campbell Rd, Richardson, T, USA b Nataz odeling Laboratory, Uniersity o Notre Dame, Notre
More informationModeling and Simulation of Wet-end White Water System in the Paper Mill
Korean J. Chem. Eng., 21(2), 358-364 (2004) Modeling and Simulation of Wet-end White Water System in the Paper Mill Yeong-Koo Yeo, Sung Chul Yi, Jae Yong Ryu and Hong Kang* Dept. of Chemical Engineering,
More informationSLIP MODEL PERFORMANCE FOR MICRO-SCALE GAS FLOWS
3th AIAA Thermophysics Conference 3- June 3, Orlando, Florida AIAA 3-5 SLIP MODEL PERFORMANCE FOR MICRO-SCALE GAS FLOWS Matthew J. McNenly* Department of Aerospace Engineering Uniersity of Michigan, Ann
More informationNetwork Flow Problems Luis Goddyn, Math 408
Network Flow Problems Luis Goddyn, Math 48 Let D = (V, A) be a directed graph, and let s, t V (D). For S V we write δ + (S) = {u A : u S, S} and δ (S) = {u A : u S, S} for the in-arcs and out-arcs of S
More informationNoise constrained least mean absolute third algorithm
Noise constrained least mean absolute third algorithm Sihai GUAN 1 Zhi LI 1 Abstract: he learning speed of an adaptie algorithm can be improed by properly constraining the cost function of the adaptie
More informationBAYESIAN PREMIUM AND ASYMPTOTIC APPROXIMATION FOR A CLASS OF LOSS FUNCTIONS
TH USHNG HOUS ROCDNGS OF TH ROMANAN ACADMY Series A OF TH ROMANAN ACADMY Volume 6 Number 3/005 pp 000-000 AYSAN RMUM AND ASYMTOTC AROMATON FOR A CASS OF OSS FUNCTONS Roxana CUMARA Department of Mathematics
More informationModel Predictive Control of a Continuous Vacuum Crystalliser in an Industrial Environment: A Feasibility Study
N. MOLDOVÁNYI and J. ABONYI, Model Predictie Control of a Continuous, Chem. Biochem. Eng. Q. 23 (2) 195 205 (2009) 195 Model Predictie Control of a Continuous Vacuum Crystalliser in an Industrial Enironment:
More informationExperimental link of coarsening rate and volume distribution in dry foam
August 2012 EPL, 99 (2012 48003 doi:.1209/0295-5075/99/48003 www.epljournal.org Eperimental link of coarsening rate and olume distribution in dry foam J. Lambert 1, F. Graner 2,3, R. Delannay 1 and I.
More informationEquivalence of Multi-Formulated Optimal Slip Control for Vehicular Anti-Lock Braking System
Preprints of the 19th World Congress The International Federation of Automatic Control Cape Town, South Africa. August 24-29, 214 Equialence of Multi-Formulated Optimal Slip Control for Vehicular Anti-Lock
More informationExploiting Source Redundancy to Improve the Rate of Polar Codes
Exploiting Source Redundancy to Improe the Rate of Polar Codes Ying Wang ECE Department Texas A&M Uniersity yingang@tamu.edu Krishna R. Narayanan ECE Department Texas A&M Uniersity krn@tamu.edu Aiao (Andre)
More informationMach i n e che st. 165 min. 2 0 m i n. 20 m in. 3 min. 20 min. Figure 1. Typical mean chest residence times throughout a papermaking system
Potential Application of Predictive Tensile Strength Models in Paper Manufacture: Part II Integration of a Tensile Strength Model with a Dynamic Paper Machine Material Balance Simulation W. Scott Paper
More informationCollective circular motion of multi-vehicle systems with sensory limitations
Collectie circular motion of multi-ehicle systems with sensory limitations Nicola Ceccarelli, Mauro Di Marco, Andrea Garulli, Antonello Giannitrapani Dipartimento di Ingegneria dell Informazione Uniersità
More informationLIMITING THE MOVEMENTS OF TRANSFORMER TAPS TO CONTROL VOLTAGE AND REACTIVE POWER
LIMITING THE MOVEMENTS OF TRANSFORMER TAPS TO CONTROL VOLTAGE AND REACTIVE POWER T. Minakawa and Y. Ichikawa Tohoku Electric Company 3-7-1, Ichiban-cho, Aoba-ku, Sendai, Miyagi 98,J APAN S. Hayashi, K.
More information10. Yes. Any function of (x - vt) will represent wave motion because it will satisfy the wave equation, Eq
CHAPER 5: Wae Motion Responses to Questions 5. he speed of sound in air obeys the equation B. If the bulk modulus is approximately constant and the density of air decreases with temperature, then the speed
More informationD(s) G(s) A control system design definition
R E Compensation D(s) U Plant G(s) Y Figure 7. A control system design definition x x x 2 x 2 U 2 s s 7 2 Y Figure 7.2 A block diagram representing Eq. (7.) in control form z U 2 s z Y 4 z 2 s z 2 3 Figure
More informationOn the influence of horizontal temperature stratification of seawater on the range of underwater sound signals. H. Lichte, Kiel, Germany
On the influence of horizontal temperature stratification of seawater on the range of underwater sound signals Original title: Über den Einfluß horizontaler Temperaturschichtung des Seewassers auf die
More informationOn the Linear Threshold Model for Diffusion of Innovations in Multiplex Social Networks
On the Linear Threshold Model for Diffusion of Innoations in Multiplex Social Networks Yaofeng Desmond Zhong 1, Vaibha Sriastaa 2 and Naomi Ehrich Leonard 1 Abstract Diffusion of innoations in social networks
More informationRelation between compressibility, thermal expansion, atom volume and atomic heat of the metals
E. Grüneisen Relation between compressibility, thermal expansion, atom olume and atomic heat of the metals Annalen der Physik 6, 394-40, 1908 Translation: Falk H. Koenemann, 007 1 Richards (1907) and his
More informationChapter 4: Techniques of Circuit Analysis
Chapter 4: Techniques of Circuit Analysis This chapter gies us many useful tools for soling and simplifying circuits. We saw a few simple tools in the last chapter (reduction of circuits ia series and
More information