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#euler number matlab
priyaohia · 5 months
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Euler’s method is not the just one concept named after him. There are many other concepts named after him; Euler’s constant, Euler line of triangle, Euler’s equation of motion, Eulerian graphs, to name a few. He has worked on a variety of area including astronomy, logarithms, calculus, the motion of the moon and plenty more. It is not surprising that he is such a high figure of influence in the world of mathematics. His concepts made mathematical applications so understandable for everyone today.
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mmorgsome · 2 years
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Matlab symbolic math toolbox
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#Matlab symbolic math toolbox pdf
#Matlab symbolic math toolbox install
#Matlab symbolic math toolbox update
#Matlab symbolic math toolbox software
I downloaded this file 'Mathematica Symbolic Toolbox for MATLAB-Version 2.0. Mathematica_matlab xw64': The specified module could not be found'. Precompiled linux and windows executables are included. The Mathematica Symbolic Toolbox for MATLAB is implemented as a single MEX-file and the source code is included. Developed by MathWorks, MATLAB allows matrix manipulations, plotting of functions and. It allows numeric and symbolic calculations, with built-in functions including plotting commands. Interfacing, Matlab, Mathlink, code generation, matrices, matrix manipulation, external programs, matlab symbolic toolbox, mathematica symbolic toolbox, Related items Mathematica Symbolic Toolbox for MATLAB-Version 1.2. MATLAB (matrix laboratory) is a numerical computing environment and fourth-generation programming language. Franklin Math is an open source Java symbolic computer algebra system (CAS), with similarities to commercial math packages such as MATLAB or Mathematica. The toolbox provides libraries of functions in common mathematical areas such as calculus, linear algebra, algebraic and ordinary. You can create, run, and share symbolic math code using the MATLAB Live Editor. I downloaded two zip archives: 'Symbolic Math Toolbox (Common) 5.10' and 'Symbolic Math Toolbox 5.10'. Symbolic Math Toolbox provides functions for solving, plotting, and manipulating symbolic math equations. MATLAB has type called sym for symbolic variables and expressions, and these. Toolboxes include related functions and are add-ons to MATLAB. The symbolic math function is in the Symbolic Math Toolbox in MATLAB. However, I am not quite sure about where I have to place my files. Symbolic mathematics defines doing mathematics on symbols (not numbers). I know that I have to download the toolbox files, place them in some directory and then specify a path. I need to add a toolbox to my Matlab Student version.
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Euler Math Toolbox Euler is a powerful all-in-one numerical software and includes Maxima for seamless symbolic computat symbolic toolbox for scilab freeload - SourceForge Connect.
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How Do I install Matlab Symbolic Toolbox in My. Join the millions of engineers and scientists who use MATLAB, Simulink, and other add-on products to solve complex design. For the syntax for symbolic differentiation, see > help sym/diff. The MATLAB symbolic toolbox is very useful for checking calculus problems. Relationships between mathematical, MATLAB and Excel expressions. You can generate MATLAB functions, Simulink function blocks, and Simscape equations directly from symbolic expressions.Free Symbolic Math Toolbox Trial. Related materials: Tutorial on numerical solution of equations using MATLAB.
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You can share your symbolic work with other MATLAB users as live scripts or convert them to HTML or PDF for publication. Your computations can be performed either analytically or using variable-precision arithmetic, with the results displayed in mathematical typeset. You can perform dimensional computations and conversions using SI and US unit systems. Symbolic Math Toolbox lets you analytically perform differentiation, integration, simplification, transforms, and equation solving.
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Symbolic Math Toolbox in the live editor (mode in MATLAB) lets you interactively update and display Symbolic math computations. The toolbox provides functions in common mathematical areas such as calculus, linear algebra, algebraic and ordinary differential equations, equation simplification, and equation manipulation. This toolbox has a wide range of applications: To visualize analytical expressions in 2D and 3D and animate plots to create videos. Symbolic Math Toolbox provides functions for solving, plotting, and manipulating symbolic math equations. Название: Matlab Symbolic Math Toolbox User’s Guide
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Adaptive Control for Quadrotor UAVs Considering Time Delay: Study with Flight Payload- Juniper Publishers
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Abstract
Design of effective control for unmanned aerial vehicles (UAVs) requires consideration of several sources of uncertainty. These undesired uncertainties affect the flight stability and performance in an unpredictable manner. The existence of transmission delays caused by wireless communication and payload variation are among such critical challenges. Adaptive control (AC) can lead to high performance tracking in the presence of uncertainties. This paper presents the application of model reference adaptive control (MRAC) to quadrotor types of UAVs considering the time delay in the altitude control system. MATLAB system identification tool is applied to obtain the altitude motion model, without time delay, for the quadrotor. Proportional-plus-velocity (PV) and PV-MRAC altitude control systems are designed, by incorporating an estimated constant time delay. The designed controllers are validated using simulations and flight tested in an indoor environment. The robustness of the PV-MRAC controller is tested against the baseline non-adaptive PV controller using the quadrotor’s payload capability..
Keywords: Adaptive control; Flight payload; Flight stability; MIT rule; PV control; Quadrotor; Time delay
Abbreviations : UAV: Unmanned Aerial Vehicles; AC: Adaptive Control; MRAC: Model Reference Adaptive Control; PV: Proportional-Plus-Velocity; UDP: User Datagram Protocols; CTA: Continuous Time Approximation; DDE: Delay Differential Equations; LTI : Linear Time-Invariant
Introduction
The application of autonomous control techniques to quadrotor types of unmanned aerial vehicles (UAVs) has been the focus of active research during the past decades. Design of control for aircraft requires several important considerations. There are numerous sources of uncertainty. For example, devices are ageing and wearing (e.g., actuator degradation), external disturbances, control input saturation, payload fluctuations, and potentially uncertain time delays in processing or communication [1]. These undesired nonlinearities affect the flight stability and performance of the controlled systems. Adaptive control (AC) is a candidate to resolve the issues, because of its ability to generate high performance tracking in the presence of uncertainties [1].
Safe, cooperative transportation of possibly large or bulky payloads by UAVs is extremely important in various missions, such as military operations, search and rescue, and personal assistants. Another huge area of application is in the service industry, where commercial quadrotor types of UAVs or drones are being used in the delivery of packages of varying masses. There are several substantial challenges and open research questions related to this application. For example, this task requires that hovering vehicles remain stable and balanced in flight as payload mass is added to the vehicle. If payload is not loaded centered or the vehicle properly trimmed for offset loads, the drone experiences bias forces that must be rejected [2]. Flying with a suspended load, known as slung load or sling load, can be a very challenging and sometimes hazardous task because the suspended load significantly alters the flight characteristics of the quadrotor [3,4].
Time delays exist in autonomous dynamic systems when signals are transmitted wirelessly. One of the challenges in designing effective control systems for UAVs is existence of signal transmission delay. The delay has nonlinear effects on the flight performance of autonomously controlled UAVs. For autonomous aerial robots, typical values of the time delay have been known to be around 0.4±0.2s [5] or 0.2s [6]. For large delays (e.g., larger than 0.2 s) the system response might not be stabilized or converged due to the dramatic increase in torque. This poses a significant challenge [7]. Since its effect is not trivial the delay need be estimated and considered in designing controllers.
Parrot AR. Drone 2.0, a commercialized drone, is controlled via WiFi network. Data streaming, commanding and reading the vehicle sensors are done using user datagram protocols (UDPs). The drone dynamics contains a time delay due to such communication. Refer to Section 2 for the drone's altitude control architecture. The overall time delay is attributed to:
I. The processing capability of the host computer,
II. The electronic devices processing the motion signals,
III. The measurement reading devices, e.g., the distance between the ultrasonic altitude sensor and the ground, and
IV. The software on the host computer for implementing the controllers.
For UAVs, wireless communication delays may not be critical when the controllers are on board. However, delays have significant effects when the control software is run on an external computer and signals are transmitted wirelessly. For example, the experiments presented in this paper were conducted using MATLAB/Simulink on an external computer, and decoding process of the navigation data (yaw, pitch, roll, altitude, etc.) contributes to the delay. Also, the numerical solvers introduce additional delay. Estimating delays is a challenging problem and has been an area of great research interest in fields as diverse as radar, sonar, seismology, geophysics, ultrasonic, controls, and communications [8,9]. A considerable number of system identification methods have been reported in the literature [10,11]. However, most of the existing methods for transfer function identification do not consider the process delay (or dead-time) or just assume knowledge of the delay [12]. Even though considerable efforts have been made on parameter estimation, there are still many open problems and there is no common approach in time-delay identification due to difficulty in formulation [13]. Several approaches for estimation of delay have been introduced in the literature [14-18]. In [14] for example, the finite dimensional Chebyshev spectral continuous time approximation (CTA) was used to solve delay differential equations (DDEs) for estimation of constant and time-varying delays.
In this paper, the constant delay applied in the drone's altitude control system was estimated using an approach based on analytical solutions to DDEs [19,20]. The time delay has been estimated as 0.36s in [21,22]. The altitude dynamics was assumed to be linear time-invariant (LTI) first order and the time delay, assumed to be single constant, was incorporated into the model as an explicit parameter. Experimental data and analytical solutions of infinite dimensional continuous DDEs were used for estimation. Measured transient responses were compared to time domain descriptions obtained by using the dominant characteristic roots based on the Lambert W function written in terms of system parameters including the delay. Proportional (P) time-delay control system, retarded type, was used to generate the responses for estimation of the delay.
The contribution of this paper is the identification of altitude motion model, without time delay, for the drone and the extension of incorporating the estimated time delay of 0.36 sin the design of an AC system. Then, validating the controller using the payload capability of the quadrotor. A model reference adaptive control (MRAC) based on the MIT rule is designed. In general, the MIT rule cannot guarantee stability [23], so the MRAC is combined with a tuned proportional-plus- velocity (PV) controller. To validate the robustness of the PV- MRAC controller, the results are compared to a baseline nonadaptive PV-controller.
This paper continues with the description of quadrotor's altitude dynamics and the AR. Drone 2.0 control system in Section 2. The altitude model identification and the design of the PV and PV-MRAC control systems are presented in Section 3. Simulations and experiments setups are presented in Section 4. In Section 5results are summarized. Concluding remarks and future work are presented in Section 6.
Quadrotor Altitude Dynamics and Control System
The notation for a typical quadrotor model is shown in Figure 1. Quadrotors has three main coordinate systems attached to it; the body-fixed frame,{b},the vehicle frame, {v} and the global inertial frame,{ w }. There are two other coordinate systems, not shown, that are of interest, the vehicle-1 frame,{v1} ,and vehicle-2 frame, {v2} [24,25]. The configuration of a quadrotor is represented by six degrees of freedom in terms of position, (xw ,yw,zw)T and the attitude defined using the Euler angles (roll, pitch, and yaw), (Øv2,θv1,φv)T, which gives a 12-state equation of motion [26]. The AR. Drone quadrotor platform adopted for this work has the same architecture design shown in Figure 1.
The quadrotor has four rotors, labelled 1 to 4, mounted at the end of each cross arm. The rotors are driven by electric motors powered by electronic speed controllers. Each rotor is controlled independently by nested feedback loops as shown in Figure 2. The inner attitude control loop uses on-board accelerometers and gyros to control the roll, pitch, and yaw while the outer position control loop uses estimates of position and velocity of the center of mass to control the trajectory in three dimensions [27]. The components of angular velocity of the robot in the body frame are p, q, and r.
The vehicle's total mass is m and d is distance from the motor to the center of mass. The total upward thrust,u(t) , on the vehicle is given by Where ωi(t) is the rotore angular speed and KF>0 is the thrust constant [26]. In addition to forces, each rotor produces a moment perpendicular to the plane of rotation of the blade, Mi(t) .The equation of motion in the z-direction can be obtained as [24,27]
Linearizing (1) at an operating point that corresponds to a nominal hover state, z0 , where the roll and pitch angles are small and the nominal thrusts, F0 , from the propellers satisfy . At the hover state the average motor angular speed, F0= mg , is given by Then, the change in the vertical acceleration can be derived as [27-29]
Thus, only the rotor's average angular speed, ωF(t), necessary to generate F (t) needs to be controlled to regulate the altitude, z(t) , of the quadrotor, since m ,and kF are g constants.
According to the AR. Drone 2.0 SDK documentation, z(t) is controlled by applying a reference vertical speed , as control input. The motion commands for the drone are encoded under a specific protocol, where high-level control signals, including , are normalized between -1 and 1to prevent damage. The drone's flight management system sampling time, Ts , is 0.065 s, which is also the sampling time at which the control law is executed and the navigation data received.
The control block diagram for the drone's altitude motion regulation is shown in Figure 3. The desired height and the actual system response are denoted zdes(t) and z(t) , respectively. The dynamics is implemented using (2), used to determine ωf(t) from the actual drone vertical speed, z(t) . The rotors rotate at equal speed,ωf(t) , which will generate F(t) to make z (t) reach the reference (zdes (t) = 1m). These computations take place in the on-board control system programmed in C. The simulation setup used is shown in Figure 4. The overall time delay,Td, single constant, in the system is represented as actuator time delay, as an explicit plant parameter. G(s) is the plant model for the combined motor and rigid body altitude dynamics without uncertainty effect.
Altitude Model and Design of Controllers
Altitude Model
Quadrotor altitude motion has second-order dynamics (Equation 1 & 2). Black-box approach was used to determine the model for the drone altitude control. MATLAB system identification toolbox App was applied to obtained LTI SISO ARX transfer function, stable system, without time delay, as
Measured data, recorded from the drone's altitude motion response, was imported into the App for the modeling process.The input data was the reference vertical speed, , constrained to [-1 1] m/s, and the output data was the vertical height, z(t). A suitable P-feedback controller was used to obtain the data. The model has a fit to estimation (best fit) of91.04%, final prediction error (FPE) of 0.000200948, and mean squared error (MSE) of 0.0001864.The system is completely state controllable and completely observable. See Figure 5 for the open-loop unit step response of the plant.
Non-adaptive control: PV
The conceptual application of this control strategy is common in angular position of DC motors, typically the control of robot manipulators [30]. PV-control, unlike proportionalplus-derivative (PD) control, does not induce numerator dynamics. The setup of the PV control system is shown in Figure 6, where Kp and Kv are the proportional (position) and velocity (derivative) gains, respectively. The transfer function of the time-delay closed-loop system is given as
Note, if G(s)= 1/s, a first order plant, used in [19,20] for the estimation of the delay, then this time-delay system will be neutral type, see [21,22] for analysis of such control system. Also, if G(s)= 1/s and then we have a P-control,retarded type time-delay, system.
Adaptive control: PV-MRAC
The primary function of adaptive controller is to accommodate uncertainties, which may introduce nonlinearities on the system dynamics. There are several broad categories of AC, and in this brief MRAC is applied. The type of MRAC depends on the adjustable mechanism, and one of the modern ones is the MIT rule. The setup of the MIT rule MRAC is shown in Figure 7, where Gp(s) and Gm(s) are transfer functions of the plant (including the uncertainties) and the reference model respectively, and yp(t) and ym(t) are their respectively outputs.
The reference signal is r(t) , is an updating parameter, γ> 0 is a tuning parameter, and the control input signal, u(t) — θ(t)r(t) , where n is the order of the system. The constant k for the plant is unknown (e.g. is the effect of quadrotor payload fluctuations or time-delay or both).CO is chosen as multiplied of Gm(s)by a desired constant, ka , so that and can matched. The tracking error, e(t)=yp(t)-ym(t),given by
Next is to define a cost function, J [θ(t)] , in terms of e(t) . The goal here is to adjust θ(t) to minimize J related to e(t) , so that as t increases e(t) → 0 . One simplest way is to expressed [23,31-34]. The rule employs a feed-forward gain adaption to update θ , as shown below [23,32-34].
Where, is sensitivity derivative of the system, and it is evaluated under assumption that θ varies slowly [23,33,34].
Now, θ(t)=[θ1(t)θ2(t)] since quadrotor altitude motion dynamics is a second-order system, then . The reference model is selected based on desired transient specifications, given in the form as [23,32]
where r(t)=zdes(t). Substituting into (8), and simplifying, we obtain
And substituting (9) into (5), and then differentiating with respect θ1(t) and θ2(t) , to obtain
If the reference model is close to the plant, then their characteristic equations can be equally approximated ,then the MIT update rule, from (6) and (10), can be written as
It is important to note that the MIT rule by itself does not guarantee error convergence or stability [23,32-34], so the MRAC is combined with a tuned PV controller. An MRAC designed using the MIT rule is very sensitive to the amplitudes of the signals. As a general rule, the value of γ is kept small.Tuning of γ is crucial to the adaptation rate and stability of the control system [23,32-34].
Simulations and Experiments
The MATLAB/Simulink program was developed for the experiments. The vertical speed control input constraints, [-1,1] ms(-1) , are applied using the saturation block. The estimated time delay of 0.36s obtained in [21,22] was implemented using the transport delay block. The experiments were conducted in an office environment with the drone's indoor hull attached. The drone is connected to the host PC through WiFi (Figure 8). Data streaming, commanding and reading, are done using UDPs. UDP is a communication protocol that offers a limited amount of service when messages are exchange between computers in a network that uses IP.
The drone navigation data (from the sensors, cameras, battery, etc.) are received, and the control signals are sent, using AT commands. AT commands are combination of short text strings sent to the drone to control its actions. The drone has ultrasound sensor (at the bottom) for ground altitude measurement. It has 1GHz 32-bit ARM Cortex A8 processor, 1GB DDR2 RAM at 200MHz, and USB 2.0 high speed for extensions. The drone�s total mass (including the indoor hull), m, is 453g.
Figure 9 shows the Simulink diagram developed for conducting the PV control system simulations. For the PV control, a high pass filter (HPF) with damping ratio, was used for the derivative controller. A natural frequency value, ωf =38 rad/s, for the filter was selected by tuning and the use of the Bode plot. The filter�s cut off frequency was determined as 0.90 Hz. Figure 10 shows the Simulink diagram developed to simulate a unit-step response for the PV-MRAC control system. The same HPF was applied in the control system.
Flight payload: disturbance rejection
To demonstrate the robustness of the PV-MRAC controller, it was tested against the PV controller using the payload capability of the drone. To accomplish this, the three cases below were considered.
Case 1: point-mass load: before flight: Masking tape was used to attach point-mass loads at the top of the drone before (Figure 11). The controllers were tested using different masses. This setup was used to determine the stability bounds within which the changing mass-inertia parameters of the system due to the acquired payload will not destabilize the drone. The mass is assumed to be close to the drone�s center of mass.
Case 2: cable-suspended point-mass load: Here, a 100g point-mass load was attached to the end of an approximately 45cm length of rope, which was hooked to the drone before flight (Figure 12). Masking tape was used to hold firm the rope across the top and the bottom of the drone. In this second case, apart from the drone carrying an extra payload, the suspension system created an oscillating (pendulum) disturbances to the system. The rope is assumed to be massless and is attached to the drone�s center of mass.
apart from the drone carrying an extra payload, the suspension system created an oscillating (pendulum) disturbances to the system. The rope is assumed to be massless and is attached to the drone's center of mass.
Case 3: point-mass load: during flight: In this setup, the designed controllers were used to demonstrate the stability behavior of the drone undergoing a range of instantaneous step payload changes. Here, the masses were attached to a sticking masking tape at the top of the drone, after it has stabilized to the desired height, =1m, see Figure13.
Results and Discussion
The drone response contains a 'dead-time' due 1) time delay in the control system and 2) the time between when the realtime application from MATLAB/Simulink is connected to the drone and when the controller is switched on. Consequently, for ease of analyzing the experiments data, some of the drone's responses plots are shifted to start at (0s,0m). For example, see Figure 14 for the drone altitude responses using a P-control system.
Note from Figure 14 that, for a P-control system, if there is no delay ( T d=0) in the system and KP > 0 , there should be no overshoot in the response. Also, increase in Kp should not destabilize the system. However, as seen in Figure 14, when Kp >1, the output has a nonzero overshoot. Moreover, when Kp ≥ 5 , the amplitude of the response grows over time and the system becomes unstable. This is partly due to the time delay in the system, which introduces nonlinearity on the dynamics. Therefore, the delay does have nontrivial effects on response and need be precisely estimated and considered in designing effective control.
Non-adaptive control: pv
The controller gains were obtained by tuning. Figure 14 & 15 show the simulation and experimental responses, respectively. It can be observed that as the value kv value increases Mo decreases, but the responses becomes slower. The PV controller with kv= 0.3 and kp=2-0 gives the best stable control system performance, with rise time tr (10%-90%range) of 1.30 s and M0 = 2.03% .The results in Figure 16 and Table 1 compares simulated and experimented with and without the time-delay effects on the control system, with Kv = 03 and kv=2-0It can be observed from the rise time values the importance of incorporating the time delay into the design of the control system.
MATLAB-based software package [35] was used to study the equation, 1+(kp+KvS)e-stdG(s) =0 , from (4). The closed-loop system stability of the time-delay system, by solving the characteristic characteristic roots within a specified region are then plotted for various kv values with k p= 2.0 . Figure 17 shows the shows the spectrum distribution of the characteristic roots. When the rightmost (i.e., dominant) roots for each case are considered k v- 0.3 the value yields the most stable rightmost root ( spectrum distribution of the characteristic roots. When the R(s)=-3.10).
Adaptive control: PV-MRAC
Figure 18&19 show simulated and experimented responses, respectively, for different values. It can be seen that, increasing γ makes the response faster but it introduces oscillations, while decreasing γmakes the response slower leading to an unstable system. The results show that there is a range of values of to achieve stabilization, assuming the other tuning parameters remains constant. The results in Figure 20 and Table 2 compares simulated and experimented with and without the time-delay effects. Here again, the results show the effect of including the time delay in the control systems design. Note that, using the PV controller and MRAC controller parameters on their own never stabilized the system.
Flight payload: disturbance rejection
Figure 21-23 show the responses for the three cases considered in introducing disturbances to the drone, see Section 4.1. In general, the results confirm that the PV-MRAC offers several benefits over the fixed-gain approach, PV controller. The PV-MRAC was found to offer enhanced robustness to the change in mass uncertainty and the oscillating disturbances.
Case 1: point-mass load: before flight
Figure 21 shows the altitude responses for the PV and PV-MRAC controllers for the case of attaching 130g point- mass load at the top of the drone. For the PV-MRAC, it was observed that beyond 130g the oscillations were larger, which destabilizes the drone. The drone's stability bounds reached at 130g for the PV-MRAC. For the PV control, it can be seen that with 130g attached, the drone was destabilized. The drone's stability bounds reached at 120g for the PV control. The difference in performance of the controllers was obvious, the adaptive controller allowed safe operation and landing, while the PV controller failed to prevent instability and sometimes resulted in a crash landing.
Case 2: cable-suspended point-mass load
The case of attaching 100g suspended point-mass load, which introduced oscillating disturbances, both controllers achieved the task of rising to the desired height, however, the PV-MRAC controller still performed better, see Figure 22. The PV-MRAC controller response has smaller oscillations about the desired height value compared to the PV controller response.
Case 3: point-mass load: during flight
Figure 23 show the responses for the PV and PV-MRAC controllers, respectively, for the case when instantaneous point-mass load of 135g was attached at the top of the drone. As it can be observed, the PV controller failed to prevent instability and resulted in a crash landing, but the adaptive controller maintained the stability and allowed safe operation and landing. The drone's stability bounds reached at 125g and 135g using the PV and PV-MRAC controllers, respectively.
Conclusion
This paper has presented a second order LTI SISO ARX altitude motion model, without time delay, for a quadrotor types of UAVs. The effect of time delay on the drone's altitude response was analysed including system stability conditions for the tuned PV control system. The non-adaptive PV controller was designed for improved transient responses based on the rightmost roots calculated using the estimated delay value. Also, the MRAC based on the MIT rule was designed by incorporating the time delay. The MRAC is combined with a tuned PV controller, since the MIT rule MRAC on its own cannot guarantee stability.?
The robustness of the PV-MRAC controller was validated by comparing its performance to that of the non-adaptive PV controller, using the payload capability of the drone and the introduction of oscillating disturbances to the system. It was shown that the PV-MRAC offers several benefits over the fixed- gain approach of the PV controller. The PV-MRAC was found to offer enhanced robustness  to the parametric (uncertainty in mass) and the oscillating disturbances. The difference in performance of the controllers was obvious. The adaptive controller allowed safe operation and landing while the PV controller failed to prevent instability and sometimes resulted in a crash landing. The drone's stability bounds reached at 120g and 130g for added attached mass-inertia using the PV and PV-MRAC controllers, respectively. In the case of the instantaneous introduction of the mass-inertia, the drone's stability bounds reached at 125g and 135g using the PV and PV-MRAC controllers, respectively.
Future work could involve comparing the performance of the MRAC based on the MIT rule to that based on the Lyapunov stability arguments, including composite adaptation. Composite MRAC adapts to both estimation and tracking errors. Also, multi-axis dynamics of the drone system considering attitude and lateral motions (x and y) can be considered. This problem is significantly more challenging, since the equation of motions are coupled and more complex than that of the altitude motion.
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thecoroutfitters · 5 years
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taliemsite-blog · 6 years
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The Matlab/Simulink model of the Supergen (Sustainable Power Generation and Supply) Wind 5 MW xemplar wind turbine, which has been employed by a number of researchers at various institutions and Universities over the last decade, is reported. It is subsequently improved, especially in speed, to acilitate wind farm modelling, which usually involves duplicating wind turbine models. The improvement is achieved through various stages, including prewarping, discretisation using Heun’s method in addition to Euler method, and conversion to C. Results are presented to demonstrate that improvement in speed is significant and that the resulting wind turbine model can be used for wind farm modelling more fficiently. It is important to highlight that improvement in speed is achieved without compromising the omplexity of the turbine model; that is, each turbine included in a wind farm is neither simplified nor ompromised. The use of the wind farm model for testing a wind farm controller that has recently been introduced is also demonstrated.
#mechanical #Power  #researchers  #improvement
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