Optimal Multingered Grasp Synthesis. J. A. Coelho Jr. R. A. Grupen. Department of Computer Science. approach. 2 Grasp controllers

Size: px
Start display at page:

Download "Optimal Multingered Grasp Synthesis. J. A. Coelho Jr. R. A. Grupen. Department of Computer Science. approach. 2 Grasp controllers"

Transcription

1 Optimal Multingere Grasp Synthesis J. A. Coelho Jr. R. A. Grupen Laboratory for Perceptual Robotics Department of Computer Science University of Massachusetts, Amherst, 3 Abstract This paper iscusses how grasp synthesis can be cast as a control composition problem. Two elemental grasp controllers are presente an compose into a general purpose grasp controller through the use of stanar optimal control techniques. The resulting grasp synthesis proceure is scalable on the number of contacts, is not tie to any specic object representation scheme, an can incorporate kinematic constraints into its resolution. grasp synthesis, an is computationally ecient with respect to the number of contacts. It also can be use to incorporate constraints relate to grasp execution (e.g., manipulator kinematics) into the synthesis process. The next section presents the elemental grasp controllers that constitute the basis for the grasp synthesis proceure, followe by the formulation of control composition as an optimal control problem. A simple grasp synthesis problem is then use to illustrate our approach. Introuction Grasp synthesis, as iealize by most researchers, consists in the o-line computation of a grasp con- guration that maximizes a certain grasp metric the author is intereste in [, 6, 7, 9,, ]. Typically, a complete moel [6, 7, ] or a smooth approximation [, 9] of the object geometry is assume. However, the synthesis proceure is computationally expensive [6] or it may involve exhaustive search over the object geometry [7, ]. Some approaches restrict the number of contacts accoring to the object imensionality ( contacts in D an 3D [], contacts in D [6], at least 3 contacts in 3D an contacts in D []), others constrain the object representation (polygons or polyhera are assume in [7, ], an smooth/parametric moels are require in [, 6, 9]). Alternatively, grasp synthesis can be cast as a control composition problem. The unerlying assumption is that a controller for executing wrench closure on general convex geometries can be constructe by composing control moules rawn from a set of basis controllers. This paper escribes how optimal control techniques can be use to solve the control composition problem. The resulting grasp synthesis proceure is not tie to any specic object representation scheme, is applicable to both - an 3-imensional Copyright c994 IEEE. Grasp controllers Grasp synthesis proceures are esigne aroun a grasp metric which is maximize uring the synthesis process. Grasp metrics usually emphasize one or more aspects of the resulting grasp conguration: capacity to resisting external isturbances [9], istance between contacts [], ratio between resulting wrenches an applie forces, or minimization of total forces applie to the object [7], grasp stability [], an others. A grasp conguration is stable if it can resist arbitrary perturbation wrenches. The approach taken observes that homogeneous grasp solutions base on frictionless point contacts moels can exploit whatever real contact friction exists to ilate the contact wrench envelope an therefore improve grasp robustness. Moreover, such grasp geometries can be use to squeeze the object within the \frictionless null space" to scale the size of the friction ilate wrench envelope. This section escribes two controllers, respectively the force closure (FC) controller an the moment closure (MC) controller, esigne to maximize grasp stability. Both controllers are base on estimates of the local wrench closure error surface. The FC controller erives its estimate on the basis of relative contact position alone, while the MC controller employs positions an normals to the contact surfaces. Contacts are assume to be frictionless point contacts an map

2 to forces an moments [; ] with respect to the object frame.. Stable grasp suciency metric In scoring a grasp conguration, it is useful to analyze the associate grasp matrix (also known as the grasp Jacobian). This matrix escribes the transformation from a set of forces applie by contacts on the object surface to a set of object frame wrenches. The grasp matrix W is ene as W = [W W : : :W n ], where W i is a six imensional vector of wrenches applie at the i th contact position. The null space of the frictionless grasp matrix e- nes a basis for a set of equivalent grasp geometries. However, the proceure for computing the null space of a matrix oes not allow for ierentiability an therefore cannot be use as a control surface. The same shortcomings plague other grasp metrics: they are computationally expensive an frequently involve optimization proceures or matrix analysis techniques that o not oer irectional information on which a grasp controller can be base. To overcome those shortcomings, a suciency metric was evise [8], base on the resiual wrench vector ~ = ~ T ~ = ~t? n ^! i! T ~t? n ^! i! ; () where ~ expresses the net wrench over j n contacts, ~t is a user-specie wrench closure bias, an ~! i is the wrench vector resulting from the i th interaction force. The elements t j [?; ] of ~t an the elements w ij [?; ] of ~w i are qualitative in the sense that they o not reect engineering units of force an torque, but express the relative ability of a contact conguration to transmit forces an torques through the object's surface. Minima in correspon to linear combinations of these qualitative wrenches which map into the grasp matrix's null space. By moving the contacts in irections that minimize, the grasp controller approaches the esire null grasp conguration. One plausible approach is to compute the graient of with respect to the contact coorinates i an move the contacts accoringly: i = ~t? n For the null grasp task, ~t = ~.! T? ~ t? n ^! i i i P i ^! i =? ~t? n =? n ~T G i i ^! i! T!i i n =? n GT i ~; () where G i is the wrench graient with respect to the contact coorinate i. In vectorial notation ~ =? n 6 4 G T G T. G T n ~ =? n GT ~: (3) Equation 3 evaluates to ~ in one of two conitions: (a) ~ = ~ an (b) when G T ~ = ~. The rst conition is the esire convergence criterion an can be use to suppress external perturbations by scaling grasp wrenches to span the task. The secon conition is equivalent to a local minimum of. This class of minima results when a local tangent to the wrench surface, G, is orthogonal to the resiual vector, ~. Both grasp controllers are base on Equation 3: what istinguishes them is exactly how ^! i varies with the contact coorinate, i.. Force closure controller The force closure (FC) controller is use to navigate frictionless point contacts on the continuous Gaussian sphere. This simplie system uses only relative contact position to eliminate the force closure component of the resiual (Equation ). If an are the angular coorinates on the Gaussian sphere, then the corresponing wrench omain moel of the object ~W (; ) = [F x F y F z M x M y M z ] becomes w = f x =?cos()cos() w 4 = m x = w = f y =?sin()cos() w 5 = m y = w 3 = f z =?sin() w 6 = m z = The suciency metric for the FC controller yiels: FC = " " " t fx + n t fy + n t fz + n cos( i )cos( i )# + sin( i )cos( i )# + sin( i )# (4)

3 The graient of Equation 4 with respect to k yiels: z FC k = (A k + B k) = sin( k + k ) (5) where A k, B k, an k are constants inepenent of k : A k = n B k =? n tfy + n tfx + n i6=k (sin( i )cos( i )) A cos(k ) i6=k (cos( i )cos( i )) A cos(k ) ^r φ r o φ o θo N ^ r θ y k = tan? (A k =B k ) Equation 5 emonstrates that the suciency metric employing the force closure moel generates a unimoal error function..3 Moment closure controller Reasoning in terms of surface curvature, a scale version of the FC controller can capture the local shape of the suciency metric for all positive an negative curvatures: the scaling constant is proportional to r, where r is the raius of curvature. However, as r! the FC graient vanishes, since forces remain constant on planar surface facets. The moment closure (MC) controller minimizes the moment resiual by ajusting each contact position on the local surface facet. We use the perpenicular of a plane, (r ; ; ), to parameterize the contact plane. Figure illustrates the parameterization an the geometry from which the wrench graient is erive. The forces transmitte through any planar face are constant at all contact positions on that face. The moments applie to the object, ~m = ~r f, ~ vary linearly with surface coorinate an pass through zero where the perpenicular passes through the plane. The resulting wrench moel is: w = f x =?cos( )cos( ) w = f y =?sin( )cos( ) w 3 = f z =?sin( ) w 4 = m x =?r sin( )cos( ) + r sin( ) w 5 = m y =?r sin( )sin( )? r cos( ) w 6 = m z = r cos( ) (6) where ( ^r ; r^ ) are the surface coorinates of the contact in the plane. Note that this approximation yiels x Figure : The Moment Closure Moel erive from a Parametric Object Plane constant contact forces which implies that control is erive from the moment iagrams exclusively; thus the esignation \moment closure". The moment closure suciency metric can be written as follows: MC = i wi MC = "t wi? n wi MC ; (7) i w i # Figure (a) shows the plot of both the force closure metric (Equation 4, ashe curve) an the plot for the suciency metric (Equation, soli curve), for the square shape, contacts. Those plots are obtaine by xing the black contact at the origin =, an moving the white contact counterclockwise over the object surface. Figure (b) shows the complete object moel; in the same gure, the suciency metric's local minima are marke over the object surface with triangles, an the white contact is positione over the metric's global minimum. Figure (c) shows the corresponing constant curvature unit Gaussian sphere, an its global (an only) minimum. Figure illustrates how the FC controller may contribute to grasp synthesis: it is a global approximation of every manifol geometry with no local minima. This heuristic control surface selects combinations of faces that minimize the force closure resiual.

4 .75 MC error FC error y x 3 Control composition as an optimal control problem Error Degrees (a) (b) y x (c) A small an somewhat constraine version of the grasp synthesis problem was chosen to illustrate our approach, namely the null grasp task of planar, convex objects with contacts. There is no theoretical impeiment in generalizing this technique to multicontact grasp of 3D objects. For the general control composition problem, the only requirements are continuity of the metric being optimize, an ierentiability of the constituent controllers. The problem Figure : (a) Suciency metric error plot, for the complete object moel (soli curve) an for the smoothe object moel (ashe curve). (b) The triangles mark the position of the suciency metric local minima on the object surface. (c) FC object moel. In this case, the global minima for both metrics coincie on = 8 o. (a) β θ (b) β.4 Controller properties The FC controller is base on contact positions exclusively; the contacts navigate the surface of the continuous Gaussian sphere, an the resulting controller can be mae globally convex [4]. The MC controller consiers both contact position an normal; the resulting control surface is piecewise convex. Each controller encoes a moel of how local contact geometry transforms contact forces into contact wrenches, but no explicit moel of the object itself is ever require { only local sensory information. Moreover, it is possible to assign an inepenent asynchronous controller to each contact. As a consequence, the complexity of the composite controller grows linearly with the number of contacts. In [4, 5], knowlege-base heuristic rules, learning techniques, an pre-imaging control are use in the composition of the FC an MC controllers. These techniques o not require a complete moel of the object; control actions can be compute irectly from sensor reaings of contact positions an normals. Although this is probably the most aequate paraigm for the control of real-worl complex systems, one can o better if complete or very goo moels about the problem is available, using optimal control techniques. Portraying the composition of controllers as an optimal control problem illustrates a general solution strategy that can be use in other omains to solve complex control problems. Figure 3: (a) Initial conguration (b) Final conguration. aresse in this paper consists of activating the FC an MC controllers, so as to minimize the number of control steps require to take the system from a initial to a nal (unknown) conguration (see Figure 3). For simplicity, we will consier that just one contact moves over the object surface, while the other stays xe at its initial position. Also, we will assume that the activation for the MC controller is constraine to be (? ), where [; ] is the activation for the FC controller. 3. Problem formulation Maximize Subject to _(t) =? () = : V = [; ] Z T FC()? MC () t + (? ) MC() In the formulation above, MC is the wrench closure error (Equation 7). For two contact grasps of square geometries, MC () can be written as MC () = E + ( tan? ) ; 6

5 where E is a constant corresponing to the force error incurre in positioning the moving contact in the various faces of the square. For the face corresponing to =, E = ; for faces corresponing to = = an = 3=, E = :5, an for the face corresponing to =, E =. Similarly, FC () is the force closure error, expresse as FC () = :5 ( + cos(? )); being the angle for the xe contact. In the evelopment that follows, the rst an secon erivatives of MC () an FC () with respect to will be require: MC = tan? 4 cos MC 8 + (tan? ) sin = 6 cos 4 FC =?:5 sin(? ) FC =?:5 cos(? ) The Hamiltonian function for the problem can now be expresse as H(t; ; ; ) =? MC () + (t) t : The costate variable is the Lagrangian multiplier require by the metho [, 3]. The Maximum Principle conitions are H(t; ; ; ) H(t; ; ; ) 8t [; T ] (8) _(t) = H =? _(t) =? H FC() = MC + (t)( FC (T ) = + (? ) WC() (9) + (? ) MC ) () Equation 8 means that the resulting Hamiltonian H is to be maximize over time, an (t) is the activation policy that maximizes it. Notice that selecting such that H = oes not cover all cases, because of the constraine range of values can assume it might be the case that correspons to one value in the limits of the close interval [; ]. Activation This is the case for the problem we are intereste in; for this example, H oes not epen on : H =?( FC? MC ): Therefore, the time optimal policy for this particular problem implies switching from to an back. This optimal pattern can be easily compute by integrating Equations 9 an above over time:. Initialize ;. Compute H H ; if make = ; 3. Compute t+ = _ t t; 4. Compute t+ = _ t t; > ; select = ; otherwise, 5. Check for convergence on ; return to () above if not converge. 4 Results In all results, we use () = 5, an t = :. The metho is not sensitive to the values chosen for these parameters; an ample range of values can be use. However, selecting a low initial value for may result in solutions corresponing to local minima. The xe contact is statione at =?:46365 raians Time MC active FC active Figure 4: Time optimal activation pattern uring the grasp. = correspons to full activation of the FC controller, while = correspons to full activation of the MC controller. Figure 4 shows the optimal activation pattern for as a function of time. Figure 4 also isplays the corresponing areas on the object surface where the controllers were selecte: gray areas correspon to where

6 in the object the MC controller was selecte ( = ), an white areas label the those areas in which the FC controller receive full activation ( = ). Contact Angle Time Figure 5: Evolution of with time. Figure 5 shows how varies with time. Starting from () = :, the contact progresses steaily to the optimal solution (T ) = 3:65 raians. Firstorer iscontinuities are present whenever the moving contact changes faces on the square. 5 Conclusion As long as the metric chosen to be optimize oesn't epen on the intermeiate activations (t), the time optimal activation policy will always be a bang-bang type solution, no matter the object being graspe. Another interesting aspect is the fact that this approach also yiels an eective grasp controller: just by evaluating H one can ecie on the next activation. What remains to be etermine is how robust this controller is with respect to object geometries, an uncertain actuation an sensory information. Because this approach essentially involves integration over time, it is not clear how to revise the control history incrementally: presumably, a object moel is being continuously or perioically upate, an sensory ata may yiel iscontinuities in the state information. How to accommoate such changes in the control scheme is yet to be etermine. Acknowlegements This work is supporte in part by NSF CDA- 8957, IRI-9697, IRI-989, an CNPq 7/9.6 (National Research Council, Brazil). References [] Bryson, A., an Ho, Y.-C. Applie Optimal Control: Optimization, Estimation, an Control. Hemisphere Publishing Corporation, New York, NY, 975. [] Chen, I., an Burick, J. Fining antipoal point grasps on irregularly shape objects. In Proc. 99 IEEE Int. Conf. Robotics Automat. (Nice, FRANCE, May 99), vol. 3, pp. 78{83. [3] Chiang, A. Elements of Dynamic Optimization. McGraw-Hill, Inc., New York, NY, 99. [4] Coelho Jr., J. Eective multingere grasp synthesis. Master's thesis, UMass, Department of Computer Science, Amherst, MA, Sept [5] Coelho Jr., J., an Grupen, R. Control preimaging for multingere grasp synthesis. In Proc. 994 IEEE Int. Conf. Robotics Automat. (San Diego, CA, May 994). [6] Faverjon, B., an Ponce, J. On computing two- nger force-closure graps of curve objects. In Proc. 99 IEEE Int. Conf. Robotics Automat. (Sacramento, CA, May 99), vol., pp. 44{ 49. [7] Ferrari, C., an Canny, J. Planning optimal grasps. In Proc. 99 IEEE Int. Conf. Robotics Automat. (Nice, FRANCE, May 99), vol. 3, pp. 9{95. [8] Grupen, R., Coelho Jr, J., an Souccar, K. Online grasp estimator: A partione state space approach. Tech. Rep. COINS Technical Report 9-75, COINS Department, University of Massachusetts, Oct. 99. [9] Guo, G., Gruver, W., an Jin, K. Grasp planning for multingere robot hans. In Proc. 99 IEEE Int. Conf. Robotics Automat. (Nice, FRANCE, May 99), vol. 3, pp. 84{89. [] Jameson, J., an Leifer, L. Automatic grasping: An optimization approach. IEEE Trans. Syst., Man, Cybern. SMC-7, 5 (Sept./Oct. 987). [] Nguyen, V. Constructing stable grasps. The Int. J. Robotics Res. 8, (989), 6{37.

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

Tutorial Test 5 2D welding robot

Tutorial Test 5 2D welding robot Tutorial Test 5 D weling robot Phys 70: Planar rigi boy ynamics The problem statement is appene at the en of the reference solution. June 19, 015 Begin: 10:00 am En: 11:30 am Duration: 90 min Solution.

More information

Problems Governed by PDE. Shlomo Ta'asan. Carnegie Mellon University. and. Abstract

Problems Governed by PDE. Shlomo Ta'asan. Carnegie Mellon University. and. Abstract Pseuo-Time Methos for Constraine Optimization Problems Governe by PDE Shlomo Ta'asan Carnegie Mellon University an Institute for Computer Applications in Science an Engineering Abstract In this paper we

More information

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:

More information

Calculus and optimization

Calculus and optimization Calculus an optimization These notes essentially correspon to mathematical appenix 2 in the text. 1 Functions of a single variable Now that we have e ne functions we turn our attention to calculus. A function

More information

and from it produce the action integral whose variation we set to zero:

and from it produce the action integral whose variation we set to zero: Lagrange Multipliers Monay, 6 September 01 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine

More information

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain Nonlinear Aaptive Ship Course Tracking Control Base on Backstepping an Nussbaum Gain Jialu Du, Chen Guo Abstract A nonlinear aaptive controller combining aaptive Backstepping algorithm with Nussbaum gain

More information

Chapter 2 Lagrangian Modeling

Chapter 2 Lagrangian Modeling Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie

More information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations Optimize Schwarz Methos with the Yin-Yang Gri for Shallow Water Equations Abessama Qaouri Recherche en prévision numérique, Atmospheric Science an Technology Directorate, Environment Canaa, Dorval, Québec,

More information

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1 Assignment 1 Golstein 1.4 The equations of motion for the rolling isk are special cases of general linear ifferential equations of constraint of the form g i (x 1,..., x n x i = 0. i=1 A constraint conition

More information

Chapter 9 Method of Weighted Residuals

Chapter 9 Method of Weighted Residuals Chapter 9 Metho of Weighte Resiuals 9- Introuction Metho of Weighte Resiuals (MWR) is an approimate technique for solving bounary value problems. It utilizes a trial functions satisfying the prescribe

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

6. Friction and viscosity in gasses

6. Friction and viscosity in gasses IR2 6. Friction an viscosity in gasses 6.1 Introuction Similar to fluis, also for laminar flowing gases Newtons s friction law hols true (see experiment IR1). Using Newton s law the viscosity of air uner

More information

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching Time Optimization in Discretized Hybrid Dynamical Systems Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set

More information

Modeling time-varying storage components in PSpice

Modeling time-varying storage components in PSpice Moeling time-varying storage components in PSpice Dalibor Biolek, Zenek Kolka, Viera Biolkova Dept. of EE, FMT, University of Defence Brno, Czech Republic Dept. of Microelectronics/Raioelectronics, FEEC,

More information

Qubit channels that achieve capacity with two states

Qubit channels that achieve capacity with two states Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March

More information

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y Ph195a lecture notes, 1/3/01 Density operators for spin- 1 ensembles So far in our iscussion of spin- 1 systems, we have restricte our attention to the case of pure states an Hamiltonian evolution. Toay

More information

SYNCHRONOUS SEQUENTIAL CIRCUITS

SYNCHRONOUS SEQUENTIAL CIRCUITS CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents

More information

G j dq i + G j. q i. = a jt. and

G j dq i + G j. q i. = a jt. and Lagrange Multipliers Wenesay, 8 September 011 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine

More information

Thermal runaway during blocking

Thermal runaway during blocking Thermal runaway uring blocking CES_stable CES ICES_stable ICES k 6.5 ma 13 6. 12 5.5 11 5. 1 4.5 9 4. 8 3.5 7 3. 6 2.5 5 2. 4 1.5 3 1. 2.5 1. 6 12 18 24 3 36 s Thermal runaway uring blocking Application

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

Analytic Scaling Formulas for Crossed Laser Acceleration in Vacuum

Analytic Scaling Formulas for Crossed Laser Acceleration in Vacuum October 6, 4 ARDB Note Analytic Scaling Formulas for Crosse Laser Acceleration in Vacuum Robert J. Noble Stanfor Linear Accelerator Center, Stanfor University 575 San Hill Roa, Menlo Park, California 945

More information

Conservation Laws. Chapter Conservation of Energy

Conservation Laws. Chapter Conservation of Energy 20 Chapter 3 Conservation Laws In orer to check the physical consistency of the above set of equations governing Maxwell-Lorentz electroynamics [(2.10) an (2.12) or (1.65) an (1.68)], we examine the action

More information

Calculus of Variations

Calculus of Variations 16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t

More information

TMA 4195 Matematisk modellering Exam Tuesday December 16, :00 13:00 Problems and solution with additional comments

TMA 4195 Matematisk modellering Exam Tuesday December 16, :00 13:00 Problems and solution with additional comments Problem F U L W D g m 3 2 s 2 0 0 0 0 2 kg 0 0 0 0 0 0 Table : Dimension matrix TMA 495 Matematisk moellering Exam Tuesay December 6, 2008 09:00 3:00 Problems an solution with aitional comments The necessary

More information

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21 Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting

More information

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v Math Fall 06 Section Monay, September 9, 06 First, some important points from the last class: Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v passing through

More information

Interpolated Rigid-Body Motions and Robotics

Interpolated Rigid-Body Motions and Robotics Interpolate Rigi-Boy Motions an Robotics J.M. Selig Faculty of Business, Computing an Info. Management. Lonon South Bank University, Lonon SE AA, U.K. seligjm@lsbu.ac.uk Yaunquing Wu Dept. Mechanical Engineering.

More information

The Principle of Least Action

The Principle of Least Action Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of

More information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments 2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor

More information

Technion - Computer Science Department - M.Sc. Thesis MSC Constrained Codes for Two-Dimensional Channels.

Technion - Computer Science Department - M.Sc. Thesis MSC Constrained Codes for Two-Dimensional Channels. Technion - Computer Science Department - M.Sc. Thesis MSC-2006- - 2006 Constraine Coes for Two-Dimensional Channels Keren Censor Technion - Computer Science Department - M.Sc. Thesis MSC-2006- - 2006 Technion

More information

Optimization of Geometries by Energy Minimization

Optimization of Geometries by Energy Minimization Optimization of Geometries by Energy Minimization by Tracy P. Hamilton Department of Chemistry University of Alabama at Birmingham Birmingham, AL 3594-140 hamilton@uab.eu Copyright Tracy P. Hamilton, 1997.

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

Relation between the propagator matrix of geodesic deviation and the second-order derivatives of the characteristic function

Relation between the propagator matrix of geodesic deviation and the second-order derivatives of the characteristic function Journal of Electromagnetic Waves an Applications 203 Vol. 27 No. 3 589 60 http://x.oi.org/0.080/0920507.203.808595 Relation between the propagator matrix of geoesic eviation an the secon-orer erivatives

More information

Numerical Integrator. Graphics

Numerical Integrator. Graphics 1 Introuction CS229 Dynamics Hanout The question of the week is how owe write a ynamic simulator for particles, rigi boies, or an articulate character such as a human figure?" In their SIGGRPH course notes,

More information

Slide10 Haykin Chapter 14: Neurodynamics (3rd Ed. Chapter 13)

Slide10 Haykin Chapter 14: Neurodynamics (3rd Ed. Chapter 13) Slie10 Haykin Chapter 14: Neuroynamics (3r E. Chapter 13) CPSC 636-600 Instructor: Yoonsuck Choe Spring 2012 Neural Networks with Temporal Behavior Inclusion of feeback gives temporal characteristics to

More information

IERCU. Institute of Economic Research, Chuo University 50th Anniversary Special Issues. Discussion Paper No.210

IERCU. Institute of Economic Research, Chuo University 50th Anniversary Special Issues. Discussion Paper No.210 IERCU Institute of Economic Research, Chuo University 50th Anniversary Special Issues Discussion Paper No.210 Discrete an Continuous Dynamics in Nonlinear Monopolies Akio Matsumoto Chuo University Ferenc

More information

Experiment 2, Physics 2BL

Experiment 2, Physics 2BL Experiment 2, Physics 2BL Deuction of Mass Distributions. Last Upate: 2009-05-03 Preparation Before this experiment, we recommen you review or familiarize yourself with the following: Chapters 4-6 in Taylor

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,

More information

Diagonalization of Matrices Dr. E. Jacobs

Diagonalization of Matrices Dr. E. Jacobs Diagonalization of Matrices Dr. E. Jacobs One of the very interesting lessons in this course is how certain algebraic techniques can be use to solve ifferential equations. The purpose of these notes is

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

Distributed coordination control for multi-robot networks using Lyapunov-like barrier functions

Distributed coordination control for multi-robot networks using Lyapunov-like barrier functions IEEE TRANSACTIONS ON 1 Distribute coorination control for multi-robot networks using Lyapunov-like barrier functions Dimitra Panagou, Dušan M. Stipanović an Petros G. Voulgaris Abstract This paper aresses

More information

Euler equations for multiple integrals

Euler equations for multiple integrals Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................

More information

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu

More information

Multivariable Calculus: Chapter 13: Topic Guide and Formulas (pgs ) * line segment notation above a variable indicates vector

Multivariable Calculus: Chapter 13: Topic Guide and Formulas (pgs ) * line segment notation above a variable indicates vector Multivariable Calculus: Chapter 13: Topic Guie an Formulas (pgs 800 851) * line segment notation above a variable inicates vector The 3D Coorinate System: Distance Formula: (x 2 x ) 2 1 + ( y ) ) 2 y 2

More information

Application of the homotopy perturbation method to a magneto-elastico-viscous fluid along a semi-infinite plate

Application of the homotopy perturbation method to a magneto-elastico-viscous fluid along a semi-infinite plate Freun Publishing House Lt., International Journal of Nonlinear Sciences & Numerical Simulation, (9), -, 9 Application of the homotopy perturbation metho to a magneto-elastico-viscous flui along a semi-infinite

More information

Influence of weight initialization on multilayer perceptron performance

Influence of weight initialization on multilayer perceptron performance Influence of weight initialization on multilayer perceptron performance M. Karouia (1,2) T. Denœux (1) R. Lengellé (1) (1) Université e Compiègne U.R.A. CNRS 817 Heuiasyc BP 649 - F-66 Compiègne ceex -

More information

The Kepler Problem. 1 Features of the Ellipse: Geometry and Analysis

The Kepler Problem. 1 Features of the Ellipse: Geometry and Analysis The Kepler Problem For the Newtonian 1/r force law, a miracle occurs all of the solutions are perioic instea of just quasiperioic. To put it another way, the two-imensional tori are further ecompose into

More information

The Principle of Least Action and Designing Fiber Optics

The Principle of Least Action and Designing Fiber Optics University of Southampton Department of Physics & Astronomy Year 2 Theory Labs The Principle of Least Action an Designing Fiber Optics 1 Purpose of this Moule We will be intereste in esigning fiber optic

More information

ELECTRON DIFFRACTION

ELECTRON DIFFRACTION ELECTRON DIFFRACTION Electrons : wave or quanta? Measurement of wavelength an momentum of electrons. Introuction Electrons isplay both wave an particle properties. What is the relationship between the

More information

A study on ant colony systems with fuzzy pheromone dispersion

A study on ant colony systems with fuzzy pheromone dispersion A stuy on ant colony systems with fuzzy pheromone ispersion Louis Gacogne LIP6 104, Av. Kenney, 75016 Paris, France gacogne@lip6.fr Sanra Sanri IIIA/CSIC Campus UAB, 08193 Bellaterra, Spain sanri@iiia.csic.es

More information

Applications of the Wronskian to ordinary linear differential equations

Applications of the Wronskian to ordinary linear differential equations Physics 116C Fall 2011 Applications of the Wronskian to orinary linear ifferential equations Consier a of n continuous functions y i (x) [i = 1,2,3,...,n], each of which is ifferentiable at least n times.

More information

The effect of nonvertical shear on turbulence in a stably stratified medium

The effect of nonvertical shear on turbulence in a stably stratified medium The effect of nonvertical shear on turbulence in a stably stratifie meium Frank G. Jacobitz an Sutanu Sarkar Citation: Physics of Fluis (1994-present) 10, 1158 (1998); oi: 10.1063/1.869640 View online:

More information

An inductance lookup table application for analysis of reluctance stepper motor model

An inductance lookup table application for analysis of reluctance stepper motor model ARCHIVES OF ELECTRICAL ENGINEERING VOL. 60(), pp. 5- (0) DOI 0.478/ v07-0-000-y An inuctance lookup table application for analysis of reluctance stepper motor moel JAKUB BERNAT, JAKUB KOŁOTA, SŁAWOMIR

More information

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE Journal of Soun an Vibration (1996) 191(3), 397 414 THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE E. M. WEINSTEIN Galaxy Scientific Corporation, 2500 English Creek

More information

Perturbation Analysis and Optimization of Stochastic Flow Networks

Perturbation Analysis and Optimization of Stochastic Flow Networks IEEE TRANSACTIONS ON AUTOMATIC CONTROL, VOL. XX, NO. Y, MMM 2004 1 Perturbation Analysis an Optimization of Stochastic Flow Networks Gang Sun, Christos G. Cassanras, Yorai Wari, Christos G. Panayiotou,

More information

SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE. Bing Ye Wu

SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE. Bing Ye Wu ARCHIVUM MATHEMATICUM (BRNO Tomus 46 (21, 177 184 SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE Bing Ye Wu Abstract. In this paper we stuy the geometry of Minkowski plane an obtain some results. We focus

More information

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k A Proof of Lemma 2 B Proof of Lemma 3 Proof: Since the support of LL istributions is R, two such istributions are equivalent absolutely continuous with respect to each other an the ivergence is well-efine

More information

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France APPROXIMAE SOLUION FOR RANSIEN HEA RANSFER IN SAIC URBULEN HE II B. Bauouy CEA/Saclay, DSM/DAPNIA/SCM 91191 Gif-sur-Yvette Ceex, France ABSRAC Analytical solution in one imension of the heat iffusion equation

More information

Simulation of Angle Beam Ultrasonic Testing with a Personal Computer

Simulation of Angle Beam Ultrasonic Testing with a Personal Computer Key Engineering Materials Online: 4-8-5 I: 66-9795, Vols. 7-73, pp 38-33 oi:.48/www.scientific.net/kem.7-73.38 4 rans ech ublications, witzerlan Citation & Copyright (to be inserte by the publisher imulation

More information

Optimization of a point-mass walking model using direct collocation and sequential quadratic programming

Optimization of a point-mass walking model using direct collocation and sequential quadratic programming Optimization of a point-mass walking moel using irect collocation an sequential quaratic programming Chris Dembia June 5, 5 Telescoping actuator y Stance leg Point-mass boy m (x,y) Swing leg x Leg uring

More information

Chapter 4. Electrostatics of Macroscopic Media

Chapter 4. Electrostatics of Macroscopic Media Chapter 4. Electrostatics of Macroscopic Meia 4.1 Multipole Expansion Approximate potentials at large istances 3 x' x' (x') x x' x x Fig 4.1 We consier the potential in the far-fiel region (see Fig. 4.1

More information

STATISTICAL LIKELIHOOD REPRESENTATIONS OF PRIOR KNOWLEDGE IN MACHINE LEARNING

STATISTICAL LIKELIHOOD REPRESENTATIONS OF PRIOR KNOWLEDGE IN MACHINE LEARNING STATISTICAL LIKELIHOOD REPRESENTATIONS OF PRIOR KNOWLEDGE IN MACHINE LEARNING Mark A. Kon Department of Mathematics an Statistics Boston University Boston, MA 02215 email: mkon@bu.eu Anrzej Przybyszewski

More information

6.003 Homework #7 Solutions

6.003 Homework #7 Solutions 6.003 Homework #7 Solutions Problems. Secon-orer systems The impulse response of a secon-orer CT system has the form h(t) = e σt cos(ω t + φ)u(t) where the parameters σ, ω, an φ are relate to the parameters

More information

DOUBLE PENDULUM VIBRATION MOTION IN FLUID FLOW

DOUBLE PENDULUM VIBRATION MOTION IN FLUID FLOW ENGINEERING FOR RURA DEEOPMENT Jelgava,.-.5.5. DOUBE PENDUUM IBRATION MOTION IN FUID FOW Janis iba, Maris Eiuks, Martins Irbe Riga Technical University, atvia janis.viba@rtu.lv, maris.eiuks@rtu.lv, martins.irbe@rtu.lv

More information

Quantum Mechanics in Three Dimensions

Quantum Mechanics in Three Dimensions Physics 342 Lecture 20 Quantum Mechanics in Three Dimensions Lecture 20 Physics 342 Quantum Mechanics I Monay, March 24th, 2008 We begin our spherical solutions with the simplest possible case zero potential.

More information

Null Space Grasp Control: Theory and Experiments

Null Space Grasp Control: Theory and Experiments 13 1 Null Space Grasp Control: Theory and Experiments Robert Platt Jr., Andrew H. Fagg, Roderic A. Grupen Abstract A key problem in robot grasping is that of positioning the manipulator contacts so that

More information

Separation of Variables

Separation of Variables Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical

More information

Harmonic Modelling of Thyristor Bridges using a Simplified Time Domain Method

Harmonic Modelling of Thyristor Bridges using a Simplified Time Domain Method 1 Harmonic Moelling of Thyristor Briges using a Simplifie Time Domain Metho P. W. Lehn, Senior Member IEEE, an G. Ebner Abstract The paper presents time omain methos for harmonic analysis of a 6-pulse

More information

3-D FEM Modeling of fiber/matrix interface debonding in UD composites including surface effects

3-D FEM Modeling of fiber/matrix interface debonding in UD composites including surface effects IOP Conference Series: Materials Science an Engineering 3-D FEM Moeling of fiber/matrix interface eboning in UD composites incluing surface effects To cite this article: A Pupurs an J Varna 2012 IOP Conf.

More information

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Course Project for CDS 05 - Geometric Mechanics John M. Carson III California Institute of Technology June

More information

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers Optimal Variable-Structure Control racking of Spacecraft Maneuvers John L. Crassiis 1 Srinivas R. Vaali F. Lanis Markley 3 Introuction In recent years, much effort has been evote to the close-loop esign

More information

Chapter 2 Governing Equations

Chapter 2 Governing Equations Chapter 2 Governing Equations In the present an the subsequent chapters, we shall, either irectly or inirectly, be concerne with the bounary-layer flow of an incompressible viscous flui without any involvement

More information

Rank, Trace, Determinant, Transpose an Inverse of a Matrix Let A be an n n square matrix: A = a11 a1 a1n a1 a an a n1 a n a nn nn where is the jth col

Rank, Trace, Determinant, Transpose an Inverse of a Matrix Let A be an n n square matrix: A = a11 a1 a1n a1 a an a n1 a n a nn nn where is the jth col Review of Linear Algebra { E18 Hanout Vectors an Their Inner Proucts Let X an Y be two vectors: an Their inner prouct is ene as X =[x1; ;x n ] T Y =[y1; ;y n ] T (X; Y ) = X T Y = x k y k k=1 where T an

More information

Center of Gravity and Center of Mass

Center of Gravity and Center of Mass Center of Gravity an Center of Mass 1 Introuction. Center of mass an center of gravity closely parallel each other: they both work the same way. Center of mass is the more important, but center of gravity

More information

Appendix: Proof of Spatial Derivative of Clear Raindrop

Appendix: Proof of Spatial Derivative of Clear Raindrop Appenix: Proof of Spatial erivative of Clear Rainrop Shaoi You Robby T. Tan The University of Tokyo {yous,rei,ki}@cvl.iis.u-tokyo.ac.jp Rei Kawakami Katsushi Ikeuchi Utrecht University R.T.Tan@uu.nl Layout

More information

Math 115 Section 018 Course Note

Math 115 Section 018 Course Note Course Note 1 General Functions Definition 1.1. A function is a rule that takes certain numbers as inputs an assigns to each a efinite output number. The set of all input numbers is calle the omain of

More information

initial configuration initial configuration end

initial configuration initial configuration end Design of trajectory stabilizing feeback for riftless at systems M. FLIESS y J. L EVINE z P. MARTIN x P. ROUCHON { ECC95 Abstract A esign metho for robust stabilization of riftless at systems aroun trajectories

More information

1 Introuction In the past few years there has been renewe interest in the nerson impurity moel. This moel was originally propose by nerson [2], for a

1 Introuction In the past few years there has been renewe interest in the nerson impurity moel. This moel was originally propose by nerson [2], for a Theory of the nerson impurity moel: The Schrieer{Wol transformation re{examine Stefan K. Kehrein 1 an nreas Mielke 2 Institut fur Theoretische Physik, uprecht{karls{universitat, D{69120 Heielberg, F..

More information

4. Important theorems in quantum mechanics

4. Important theorems in quantum mechanics TFY4215 Kjemisk fysikk og kvantemekanikk - Tillegg 4 1 TILLEGG 4 4. Important theorems in quantum mechanics Before attacking three-imensional potentials in the next chapter, we shall in chapter 4 of this

More information

Exam 2 Review Solutions

Exam 2 Review Solutions Exam Review Solutions 1. True or False, an explain: (a) There exists a function f with continuous secon partial erivatives such that f x (x, y) = x + y f y = x y False. If the function has continuous secon

More information

How to Minimize Maximum Regret in Repeated Decision-Making

How to Minimize Maximum Regret in Repeated Decision-Making How to Minimize Maximum Regret in Repeate Decision-Making Karl H. Schlag July 3 2003 Economics Department, European University Institute, Via ella Piazzuola 43, 033 Florence, Italy, Tel: 0039-0-4689, email:

More information

Bohr Model of the Hydrogen Atom

Bohr Model of the Hydrogen Atom Class 2 page 1 Bohr Moel of the Hyrogen Atom The Bohr Moel of the hyrogen atom assumes that the atom consists of one electron orbiting a positively charge nucleus. Although it oes NOT o a goo job of escribing

More information

Chapter 6: Energy-Momentum Tensors

Chapter 6: Energy-Momentum Tensors 49 Chapter 6: Energy-Momentum Tensors This chapter outlines the general theory of energy an momentum conservation in terms of energy-momentum tensors, then applies these ieas to the case of Bohm's moel.

More information

A Path Planning Method Using Cubic Spiral with Curvature Constraint

A Path Planning Method Using Cubic Spiral with Curvature Constraint A Path Planning Metho Using Cubic Spiral with Curvature Constraint Tzu-Chen Liang an Jing-Sin Liu Institute of Information Science 0, Acaemia Sinica, Nankang, Taipei 5, Taiwan, R.O.C., Email: hartree@iis.sinica.eu.tw

More information

4.2 First Differentiation Rules; Leibniz Notation

4.2 First Differentiation Rules; Leibniz Notation .. FIRST DIFFERENTIATION RULES; LEIBNIZ NOTATION 307. First Differentiation Rules; Leibniz Notation In this section we erive rules which let us quickly compute the erivative function f (x) for any polynomial

More information

Module FP2. Further Pure 2. Cambridge University Press Further Pure 2 and 3 Hugh Neill and Douglas Quadling Excerpt More information

Module FP2. Further Pure 2. Cambridge University Press Further Pure 2 and 3 Hugh Neill and Douglas Quadling Excerpt More information 5548993 - Further Pure an 3 Moule FP Further Pure 5548993 - Further Pure an 3 Differentiating inverse trigonometric functions Throughout the course you have graually been increasing the number of functions

More information

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Preprints of the 9th Worl Congress The International Feeration of Automatic Control Cape Town, South Africa. August -9, Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Zhengqiang

More information

Angles-Only Orbit Determination Copyright 2006 Michel Santos Page 1

Angles-Only Orbit Determination Copyright 2006 Michel Santos Page 1 Angles-Only Orbit Determination Copyright 6 Michel Santos Page 1 Abstract This ocument presents a re-erivation of the Gauss an Laplace Angles-Only Methos for Initial Orbit Determination. It keeps close

More information

Both the ASME B and the draft VDI/VDE 2617 have strengths and

Both the ASME B and the draft VDI/VDE 2617 have strengths and Choosing Test Positions for Laser Tracker Evaluation an Future Stanars Development ala Muralikrishnan 1, Daniel Sawyer 1, Christopher lackburn 1, Steven Phillips 1, Craig Shakarji 1, E Morse 2, an Robert

More information

inflow outflow Part I. Regular tasks for MAE598/494 Task 1

inflow outflow Part I. Regular tasks for MAE598/494 Task 1 MAE 494/598, Fall 2016 Project #1 (Regular tasks = 20 points) Har copy of report is ue at the start of class on the ue ate. The rules on collaboration will be release separately. Please always follow the

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

24th European Photovoltaic Solar Energy Conference, September 2009, Hamburg, Germany

24th European Photovoltaic Solar Energy Conference, September 2009, Hamburg, Germany 4th European hotovoltaic Solar Energy Conference, 1-5 September 9, Hamburg, Germany LOCK-IN THERMOGRAHY ON CRYSTALLINE SILICON ON GLASS (CSG) THIN FILM MODULES: INFLUENCE OF ELTIER CONTRIBUTIONS H. Straube,

More information

Students need encouragement. So if a student gets an answer right, tell them it was a lucky guess. That way, they develop a good, lucky feeling.

Students need encouragement. So if a student gets an answer right, tell them it was a lucky guess. That way, they develop a good, lucky feeling. Chapter 8 Analytic Functions Stuents nee encouragement. So if a stuent gets an answer right, tell them it was a lucky guess. That way, they evelop a goo, lucky feeling. 1 8.1 Complex Derivatives -Jack

More information