Collision avoidance with automatic braking and swerving

Size: px
Start display at page:

Download "Collision avoidance with automatic braking and swerving"

Transcription

1 Preprints of the 9th World Congress The International Federation of Automatic Control Cape Town, South Africa. August 4-9, 4 Collision aoidance with automatic braking and swering Carlo Ackermann Rolf Isermann Sukki Min Changwon Kim Institute of Automatic Control and Mechatronics, Technical Uniersity Darmstadt ( cackermann@iat.tu-darmstadt.de). Institute of Automatic Control and Mechatronics, Technical Uniersity Darmstadt ( risermann@iat.tu-darmstadt.de). Hyundai Motor Company, Seoul, Korea, ( sukkimin@hyundai.com) Hyundai Motor Company, Seoul, Korea, ( cwkim@hyundai.com) Abstract: To aoid collisions in longitudinal direction emergency braking is suitable in many situations. Howeer for higher elocites, an easie maneuer is better because it can be applied later than the braking maneuer if there is enough free space. This contribution inestigates methods for the decision-making of a collision aoidance system with regard to automatic braking and swering. The resulting system tries to use the latest possible point for interention if the drier does not react. This decision is based on certain time measures and distances. Further trajectory planning and control methods for swering are described and some simulations are gien. Keywords: Collision Aoidance; Trajectory planning; nlinear Control; Interactie ehicle control; Vehicle dynamics.. INTRODUCTION Collisions with other objects or ehicles on urban roads or highways in longitudinal direction can be aoided by automatic braking or swering, if the drier does not react in an early stage and in the right way, Isermann et al. []. This contribution extends former theoretical and experimental research for swering at higher speeds and takes into account the aailable free space. The assumed sensors are a suitable front radar system and a ideo camera and rear-left and rear-right radar systems. Some specialities of the inestigations are the calculation of the last instants to brake and to steer, which depend on the relatie elocitiy and are different. A decision making program will be deeloped which includes the estimation of aailable free space on the parallel lane considers seeral ehicles. The methods are deeloped by simulations with the comprehensie IPG CarMaker simulation enironment and include experimental results from earlier work.. CONSIDERED SCENARIO As automotie collision aoidance systems hae to consider seeral driing situations, the tested scenario has to be specified.. Sensor setup The different sensors used as shown in Fig.. A camera is installed at the windshield, which deliers information about the lane-width, the position of the ego ehicle on the lane and the lateral position of the front ehicles. Rear-left radar Rear-right radar Fig.. Schematic sensor arrangement y x Camera Front radar Three radar sensor systems (e.g. 4 or 77 GHz) are assumed, the front system detects objects driing in front of the ego ehicle. The other two radar sensors are installed at the left and right backside of the car. All radar sensors supply object lists. For each object the position relatiely to the ego ehicle and the difference elocity is proided relatiely to the obstacles. Because the rear radar sensors are turned, their information is transformed into the same coordinate system. Then Copyright 4 IFAC 694

2 9th IFAC World Congress Cape Town, South Africa. August 4-9, 4 RL High Speed Braking possible Steering possible Steering possible RM Fig.. Objects around the ego ehicle the distance and difference elocity is proided in X- and Y-coordiantes relatiely to the ego ehicle.. Objects In the following the ehicles next to the ego ehicle are considered. Four ehicles as shown in Fig. are assumed: Front-left, front-middle, rear-left, and rear-middle. The ehicles classified as left are the nearest objects on the left lane next to the ego-ehicle. The front-middle ehicle is the main object in front of the own car. For testing purposes in a first phase only the middle and the two left objects are considered in the CarMaker simulation enironment. Using the position of the ego ehicle and the object lists from the radar sensors and fusion with the camera Isermann et al. [], the releant objects can be selected. 3. Basic considerations 3. DECISION MAKING In the following it is assumed that the main object for collision aoidance is the car in front of the own () ehicle. The goal is to aoid the collision in the last possible moment. This can be either the last point to steer (LPS), then swering is the better maneuer, or the last point to brake (LPB), then braking is the better maneuer. LPB after LPS At lower elocities the braking maneuer is the maneuer which can be performed later. This is illustrated in Fig. 3. Low Speed Braking possible Steering possible Braking possible LPB LPS Fig. 4. Illustration of last point to brake and last point to steer at high elocities If swering is not possible because of missing free space, only the emergency braking helps to interent or mitigate the collision. But this has to be started at earlier time. So the information if an easie maneuer is possible at the last point to steer has to be aailable at the last point to brake. 3. Calculation of time interals For making a decision there are generally two possibilities. One is to consider the distances between all the objects. Howeer the distance has to be interpreted dependent on the elocities. The other possibility is to use time interals. These time interals indicate after which time a certain eent occurs or how long a certain eent takes. The adantage is, that only one alue has to be considered. Furthermore human reaction times can be used as reference alues. Therefore the decisions are based on time interals. They are calculated with the information from the enironmental sensors and definitions made before. Important time interals are the time to collision (TTC), the braking time (T brake ) and the easie time (T ea ). Based on these time interals the time to steer (TTS) and the time to brake (TTB) can be calculated. Time to Collision (TTC) Using the difference elocities and the distances it is possible to calculate the Time to Collision (TTC). The TTC represents the time after which a collision occurs if the two considered ehicles drie with the same elocity (Hayward [97]): LPS LPB Fig. 3. Illustration of last point to brake and last point to steer at low elocities This is the more easy case. When the last point to brake is reached, the system has to do a full braking automatically. LPS after LPB At higher elocities the braking distance is longer than the distance needed for the easie maneuer, Bender et al. [7]. This is outlined in Fig. 4. This case is more difficult than the other one. Generally the easie maneuer is the best way to aoid the collision. But an easie maneuer is of course only possible, if there is enough space sidewards and backwards to swere. So the assistance system has to ensure that the cars on the easie lane are far enough so that they are not endangered. TTC = s dx dx. () Braking Time If there is a negatie difference elocity to the car in front ( dx,fr < ), then the own car moes towards the car in front. Under the assumption that this ehicle moes with constant elocity, and a constant maximum deceleration for dry asphalt is assumed with a brake = 9.8 m s, for the braking time it holds (Ackermann et al. [4]): T brake ( dx, a brake ) = dx. () a brake Easie Time The easie time depends on the width, i.e. the lateral displacement y ea, from the easie maneuer and the maximum lateral acceleration a ea which depends on the road condition (Winner et al. [9]): T ea (y ea, a ea ) = yea a ea + τ s. (3) 695

3 9th IFAC World Congress Cape Town, South Africa. August 4-9, 4 τ s is the steering loss time and can be assumed with.s. Time to Brake (TTB) The time to brake gies the time after which a braking maneuer has to be started to preent the collision. If the TTB is smaller than, a collision can not be aoided by braking. TTB = TTC fm T brake. (4) Time to Steer (TTS) The time to steer gies the time after which an easie maneuer has to be started to preent the collision. If the TTC is smaller than, a collision can not be aoided by steering. 3.3 Selection of free space TTS = TTC fm T ea. (5) For making a decision the cars on the other lanes are considered. For simplification only the left lane is considered. Other lanes, if present, can be considered similarly. The sensor based object detection obseres the ehicles on the left lane in front and behind the ego ehicle. These two cars represent the highest potential risk. In the following a forecast of free space selection is made for the last point to steer. Assuming that the cars are moing with constant elocity, it is checked, if the easie maneuer will be possible at the last point to steer (LPS). Some equations for the forecast calculate if the easie maneuer will be possible when the last possible point to steer is reached (TTS = TTC fm T ea = ). TTS TTC fl T brake,fl TTC fl T ea TTS T ea T brake,fl Fig. 5. Graphical illustration for front-left target Front-left target Assuming constant elocities, T brake,fl and T ea stay constant and TTC fl decreases continously. Performing the easie maneuer at TTS =, TTC fl will decrease by TTS from the moment of calculation to TTS =. For the front-left target the TTC to the front-left object minus the braking and the easie time has to be higher than the TTS, because first the swering and then the braking is assumed: TTC fl T brake,fl T ea > TTS. (6) With the relation TTS = TTC fm T ea this leads to: TTC fl T brake,fl > TTC fm. (7) Rear-left target The same is done for the rear-left target with the difference that now the braking time of the rearleft ehicle is considered, which leads to: TTC rl T brake,rl > TTC fm. (8) The question if the easie maneuer will be possible at TTS = can now be answered by the following equation:, if TTC fl T brake,fl > TTC fm eapossible = TTC rl T brake,rl > TTC fm,, else. (9) 3.4 Decision rules w these calcuations are used for making a decision for the assistance system. This decision will then be gien to the collision aoidance control. For small difference elocities the braking distance is smaller than the easie distance. For big difference elocities this is opposite. The intersection can be calculated ery easily: dx;brake=ea = a brake yea a ea. () Because the system should interent at the last possible point, for difference elocities smaller than dx;brake=ea braking is better than swering, Stählin et al. [7]. For higher difference elocities the swering is the better maneuer but can only be performed when there is enough space on the easie lane. Example: Assuming a brake = 9.8 m s, a ea = 7 m s and y ea = 3.6m the intersection elocity is dx;brake=ea = 9.9 m s = 7.6 km h. Braking time reached TTC fm < T brake Easie time smaller than braking time T ea < T brake Emergency brake Easie maneuer possible? Fig. 6. Flowchart for decision making Emergency steer Easie time reached TTC fm < T ea Fig. 6 shows how the decision is made. When the braking time is reached, the system checks if the easie time is smaller than the braking time. If not, braking is in eery case the better maneuer and the system starts to brake. If not, it is considered if an easie maneuer will be possible at the last point to steer. If this is not the case, the emergency braking is performed too. If an easie maneuer will be possible, the system performs the easie maneuer at the last point to steer. 4. DESIGN OF TRAJECTORY CONTROL After the treatment of the decision-making this section deals with the control of the lateral and longitudinal dynamics of the ehicle. First, the controller for the braking maneuer is presented. Then a method for planning an easie trajectory is introduced. Finally a controller for the steering system is presented to drie along the calculated trajectory. 696

4 9th IFAC World Congress Cape Town, South Africa. August 4-9, 4 4. Brake control Because only a fullbraking is needed it is sufficient to apply maximum braking to the ehicle. The assumed maximal possible deceleration is a break = 9.8 m s for dry roads. 4. Trajectory planning For the easie maneuer the required trajectory is subject to the steering controller. The manipulated ariable is the steering angle. There are different possibilities for planning an easie trajectory. In eery case it is important to limit the lateral acceleration. Otherwise the physical limits can be exceeded. y in m Fig. 7. Transfer function t in s A simple way is to create the trajectory as a step response. In Schmitt [] a fourth order transfer function was used to predict the lane-change-trajectory for the PRORETA project. This can be also used for an easie maneuer. The following transfer function is considered: G(s) = ( + T s) 4. () This function is obtained from the transfer function G(s) = K ( + T s)( + T s)...( + T n s) B () and the assumption that all time constants match, Isermann and Münchhof []. The fourth order transfer function can also be written as a state space system: ẏ Y ȧ = Y j Y T 4 4 T 3 6 T 4 T y Y + a Y jy T 4 y ref. (3) When the easie maneuer is started, y ref is set to a step function of size B. Then an easie trajectory in timedomain y(t) follows as a step-response. T affects the shape of the trajectory and has to be determined in a way that the maximum jerk and the maximum lateral acceleration are respected. Determination of parameter T For determination of the time constant T the maximum lateral acceleration is considered, because it is included in the state ector. The maximum lateral acceleration occurs at t ay,max = T (3 3). (4) which is obtained by the solution in the time-domain of the step-response from Eq. (3). For a Y,max then holds a Y,max = B T e (3 3) ( (3 3) (3 ) 3) 3 6 (5).3 B T. w the time constant T can be determined in dependence of B and a Y,max : 4.3 Steering control Planning y y des a y,des T = B.3. a Y,max (6) -. ψ des PD Fig. 8. Structure of steering controller For steering control a two-degree-of-freedom structure is used, consisting of a feedforward and a feedback controller. Feedforward control The trajectory planning leads to the following state space system is gien: ẏ ref Y,ref ȧ Y,ref j Y,ref = T 4 4 T 3 6 T 4 T FF δ FB y ref Y,ref a Y,ref j Y,ref δ FF + δ des T 4 B ref. (7) When the easie maneuer is started, B ref as input signal is set to B. Then an easie trajectory in time-domain y ref (t) is gien as a step-response of this state space model. Furthermore a y,ref (t) is calculated. This can be used for feedforward-control. With the desired lateral acceleration the desired yawrate ψ ref can be calculated: ψ ref = a Y,ref. (8) Using the desired yawrate it is possible to calculate a desired steering angle, Schorn and Isermann [6]: δ ψ = i S l + SG. (9) 697

5 9th IFAC World Congress Cape Town, South Africa. August 4-9, 4 SG is the so-called understeer gradient and describes the steering behaiour depending on the elocity, Gillespie [99], Kiencke and Nielsen []: SG = c α,rl r + c α,f l f. () c α,f c α,r l Feedback control Schorn [7] inestigated different controllers. Finally he ended up in the relatiely simple PD-Controller, which is also used here. As the one track ehicle model shows, the lateral behaiour depends on the elocity. Therefore M different controllers depending on the elocity of the ehicle are applied. The controller outputs are weighted with membership or actiation functions and summarized as shown in Fig. 9. This approach uses local linear models (Fink et al. [999]). y Controller Controller... Controller M 95 m km/h km/h m 5 km/h Fig.. Maneuer : High difference elocity, swering possible 95 m 5 km/h km/h m 5 km/h Fig.. Maneuer : High difference elocity, swering not possible 5. Decision erification For better illustration the maximum deceleration is now assumed with 5 m s, because then the time interal between the last point to steer and the last point to brake is larger. Fig. 9. Structure of elocity dependent controllers δ fb The output of the local linear controller network is obtained from the weighted controller outputs: using δ fb = M δ LLM,i Φ i () () i= free space forecast action RL &RL steering braking LPB LPS Φ i () = µ i () M j= µ j() as actiation function. with 5. RESULTS ( µ i () = exp ( c i ) ) σ i () This section summarizes the results of the collision aoidance part. After introducing different testing scenarios, the results are presented. Here only the case of a large difference elocity is considered as an example. 5. Scenarios Maneuer : High difference elocity, swering possible In the first maneuer the ego ehicle dries with km h. In front of the own car is another ehicle, which dries ery slow. On the left lane dries a car with higher speed, which will not disturb the easie maneuer. Maneuer : High difference elocity, swering not possible The second maneuer is nearly the same like the first one. Only the car on the left dries with a higher elocity. So this car will block the easie maneuer. Fig.. Decision for scenario Fig. depicts the decision for scenario. At about. seconds at the last point to brake the decision is made. Because the forecast determines a free road, the easie maneuer is started at 3.4 seconds which is the last point to steer. free space forecast action RL &RL steering braking LPB LPS Fig. 3. Decision for scenario 698

6 9th IFAC World Congress Cape Town, South Africa. August 4-9, 4 In Fig. 3 the decision is also made at. seconds. But in this case the forecast determines a ehicle on the left lane at the last point to steer. So an emergency braking maneuer is started immediately. Hence it is illustrated, that the forecast determines the blocked lane already at the last point to brake een if there is enough space at this time instant, but not later. 5.3 Steering control y in m meas. ref (a) Control ariable δ in rad 4 Fig. 4. Steering control ay in m/s (b) Lateral acceleration ff fb (c) Manipulated steering angle For the steering the controller described before is used. In Fig. 4 the reference and the drien trajectory, the lateral acceleration and the steering angle diided in feedforward and feedback part are shown. The car follows the trajectory well and the collision is aoided. 6. CONCLUSION A drier assistance system was presented, which uses either the brake for the preenting of collisions or the steering. For swering knowledge on ehicles of the adjacent roadway is required. A method was presented which takes the aailability of the free space into account. Finally a decision is made based on the elocities, distances, gien maximum accelerations and the estimated free space to aoid the collision. Stability limits of driing physics are considered by the specification of maximum lateral acceleration and maximum deceleration. These alues hae to be chosen depending on the road condition. The system tries to use the latest possible point for interention if the drier does not react. The next step is to optimize the deeloped system. Presently the drier has the possibility to interent until the last possible point. But then the system reacts fully automatically. Therefore a warning system could be introduced. Further the inclusion of an appropriate interpretation of the drier s intentions can be inestigated. To reduce the easie time also a combination of braking and swering is conceiable. SYMBOLS ehicle elocity m/s a Y lateral acceleration m/s ψ yaw rate rad/s δ H steering wheel angle rad i S steering ratio c α cornering stiffness N/rad l wheel base m TTC time to collision s T brake braking time s T ea easie time s s dx distance in x-direction m s dy distance in y-direction m dx difference elocity in x-direction m/s REFERENCES Carlo Ackermann, Rolf Isermann, Sukki Min, and Changwon Kim. Design of a decision maker for an easie or braking maneuer. In 4th Stuttgart International Symposium, 4. Ea Bender, Michael Darms, Matthias Schorn, Ulrich Stählin, Rolf Isermann, Hermann Winner, and Kurt Landau. Anti collision system proreta on the way to the collision aoiding ehicle: Part : Basics of the system. ATZ Worldwide, 9(4): 3, 7. Alexander Fink, Olier Nelles, and Martin Fischer. Linearization based and local model based controller design. In European Control Conference, 999. Thomas D. Gillespie. Fundamentals of ehicle dynamics. Society of Automotie Engineers, Warrendale and PA, 99. John C. Hayward. Near miss determination through use of a scale of danger. Report no. TTSC75. The Pennsylania State Uniersity, 97. Rolf Isermann and Marco Münchhof. Identification of dynamical systems. Springer-Verlag, Berlin,. Rolf Isermann, Roman Mannale, and Ken Schmitt. Collision-aoidance systems proreta: situation analysis and interention control. Control Engineering Practice, ():36 46,. Uwe Kiencke and Lars Nielsen. Automotie control systems. Springer-Verlag, Berlin and New York,. Ken Schmitt. Situationsanalyse für ein Fahrerassistenzsystem zur Vermeidung on Überholunfällen auf Landstraßen, olume 763 of Fortschrittberichte VDI Reihe. VDI Verlag,. Matthias Schorn. Quer- und Längsregelung eines Personenkraftwagens für ein Fahrerassistenzsystem zur Unfallermeidung, olume 65 of Fortschrittberichte VDI Reihe. VDI-Verlag, Düsseldorf, 7. Matthias Schorn and Rolf Isermann. Automatic steering and braking for a collision aoidance ehicle. In 4th IFAC-Symposium on Mechatronic Systems: -4 September, 6. Ulrich Stählin, Matthias Schorn, and Rolf Isermann. Collision aoidance braking and steering strategies for an adanced drier assistance system. In 7th Stuttgart International Symposium, 7. Hermann Winner, Stephan Hakuli, and Gabriele Wolf. Handbuch Fahrerassistenzsysteme. ATZ- MTZ-Fachbuch. Vieweg + Teubner, Wiesbaden,

Statement: This paper will also be published during the 2017 AUTOREG conference.

Statement: This paper will also be published during the 2017 AUTOREG conference. Model Predictie Control for Autonomous Lateral Vehicle Guidance M. Sc. Jochen Prof. Dr.-Ing. Steffen Müller TU Berlin, Institute of Automotie Engineering Germany Statement: This paper will also be published

More information

Detection of Critical Driving Situations using Phase Plane Method for Vehicle Lateral Dynamics Control by Rear Wheel Steering

Detection 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 information

Planning of Optimal Collision Avoidance Trajectories with Timed Elastic Bands

Planning of Optimal Collision Avoidance Trajectories with Timed Elastic Bands Preprints of the 19th World Congress The International Federation of Automatic Control Cape Town, South Africa. August -9, 1 Planning of Optimal Collision Avoidance Trajectories with Timed Elastic Bands

More information

Drive train. Steering System. Figure 1 Vehicle modeled by subsystems

Drive train. Steering System. Figure 1 Vehicle modeled by subsystems Proceedings of the XII International Symposium on Dynamic Problems of Mechanics (DINAME 7), P.S.Varoto and M.A.Trindade (editors), ABCM, Ilhabela, SP, Brazil, February 6 - March, 7 Wheel Dynamics Georg

More information

The single track model

The single track model The single track model Dr. M. Gerdts Uniersität Bayreuth, SS 2003 Contents 1 Single track model 1 1.1 Geometry.................................... 1 1.2 Computation of slip angles...........................

More information

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS SUBAREA I. COMPETENCY 1.0 UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS MECHANICS Skill 1.1 Calculating displacement, aerage elocity, instantaneous elocity, and acceleration in a gien frame of reference

More information

Robust Real-time Optimal Autonomous Highway Driving Control System: Development and Implementation

Robust Real-time Optimal Autonomous Highway Driving Control System: Development and Implementation Preprints of the 9th World Congress The International Federation of Automatic Control Cape Town, South Africa. August 24-29, 24 Robust Real-time Optimal Autonomous Highway Driing Control System: Deelopment

More information

Frames of Reference, Energy and Momentum, with

Frames of Reference, Energy and Momentum, with Frames of Reference, Energy and Momentum, with Interactie Physics Purpose: In this lab we will use the Interactie Physics program to simulate elastic collisions in one and two dimensions, and with a ballistic

More information

A Comparative Study of Vision-Based Lateral Control Strategies for Autonomous Highway Driving

A Comparative Study of Vision-Based Lateral Control Strategies for Autonomous Highway Driving A Comparatie Study of Vision-Based ateral Control Strategies for Autonomous Highway Driing J. Košecká, R. Blasi, C. J. Taylor and J. Malik Department of Electrical Engineering and Computer Sciences Uniersity

More information

We provide two sections from the book (in preparation) Intelligent and Autonomous Road Vehicles, by Ozguner, Acarman and Redmill.

We provide two sections from the book (in preparation) Intelligent and Autonomous Road Vehicles, by Ozguner, Acarman and Redmill. We provide two sections from the book (in preparation) Intelligent and Autonomous Road Vehicles, by Ozguner, Acarman and Redmill. 2.3.2. Steering control using point mass model: Open loop commands We consider

More information

Nonlinear Lateral Control of Vision Driven Autonomous Vehicles*

Nonlinear Lateral Control of Vision Driven Autonomous Vehicles* Paper Machine Intelligence & Robotic Control, Vol. 5, No. 3, 87 93 (2003) Nonlinear ateral Control of Vision Drien Autonomous Vehicles* Miguel Ángel Sotelo Abstract: This paper presents the results of

More information

Position in the xy plane y position x position

Position 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 information

Purpose of the experiment

Purpose of the experiment Impulse and Momentum PES 116 Adanced Physics Lab I Purpose of the experiment Measure a cart s momentum change and compare to the impulse it receies. Compare aerage and peak forces in impulses. To put the

More information

Brake applications and the remaining velocity Hans Humenberger University of Vienna, Faculty of mathematics

Brake applications and the remaining velocity Hans Humenberger University of Vienna, Faculty of mathematics Hans Humenberger: rake applications and the remaining elocity 67 rake applications and the remaining elocity Hans Humenberger Uniersity of Vienna, Faculty of mathematics Abstract It is ery common when

More information

DO PHYSICS ONLINE. WEB activity: Use the web to find out more about: Aristotle, Copernicus, Kepler, Galileo and Newton.

DO PHYSICS ONLINE. WEB activity: Use the web to find out more about: Aristotle, Copernicus, Kepler, Galileo and Newton. DO PHYSICS ONLINE DISPLACEMENT VELOCITY ACCELERATION The objects that make up space are in motion, we moe, soccer balls moe, the Earth moes, electrons moe, - - -. Motion implies change. The study of the

More information

Estimation of Tire-Road Friction by Tire Rotational Vibration Model

Estimation of Tire-Road Friction by Tire Rotational Vibration Model 53 Research Report Estimation of Tire-Road Friction by Tire Rotational Vibration Model Takaji Umeno Abstract Tire-road friction is the most important piece of information used by active safety systems.

More information

( ) Momentum and impulse Mixed exercise 1. 1 a. Using conservation of momentum: ( )

( ) Momentum and impulse Mixed exercise 1. 1 a. Using conservation of momentum: ( ) Momentum and impulse Mixed exercise 1 1 a Using conseration of momentum: ( ) 6mu 4mu= 4m 1 u= After the collision the direction of Q is reersed and its speed is 1 u b Impulse = change in momentum I = (3m

More information

Chapter 1: Kinematics of Particles

Chapter 1: Kinematics of Particles Chapter 1: Kinematics of Particles 1.1 INTRODUCTION Mechanics the state of rest of motion of bodies subjected to the action of forces Static equilibrium of a body that is either at rest or moes with constant

More information

Space Probe and Relative Motion of Orbiting Bodies

Space Probe and Relative Motion of Orbiting Bodies Space robe and Relatie Motion of Orbiting Bodies Eugene I. Butiko Saint etersburg State Uniersity, Saint etersburg, Russia E-mail: e.butiko@phys.spbu.ru bstract. Seeral possibilities to launch a space

More information

A Study on Performance Analysis of V2V Communication Based AEB System Considering Road Friction at Slopes

A Study on Performance Analysis of V2V Communication Based AEB System Considering Road Friction at Slopes , pp. 71-80 http://dx.doi.org/10.14257/ijfgcn.2016.9.11.07 A Study on Performance Analysis of V2V Communication Based AEB System Considering Road Friction at Slopes Sangduck Jeon 1, Jungeun Lee 1 and Byeongwoo

More information

Analysis of Forward Collision Warning System. Based on Vehicle-mounted Sensors on. Roads with an Up-Down Road gradient

Analysis of Forward Collision Warning System. Based on Vehicle-mounted Sensors on. Roads with an Up-Down Road gradient Contemporary Engineering Sciences, Vol. 7, 2014, no. 22, 1139-1145 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ces.2014.49142 Analysis of Forward Collision Warning System Based on Vehicle-mounted

More information

Realization of Hull Stability Control System for Continuous Track Vehicle with the Robot Arm

Realization of Hull Stability Control System for Continuous Track Vehicle with the Robot Arm Adanced Science and Technology Letters Vol.86 (Ubiquitous Science and Engineering 05), pp.96-0 http://dx.doi.org/0.457/astl.05.86.0 Realization of Hull Stability Control System for Continuous Track Vehicle

More information

Equivalence of Multi-Formulated Optimal Slip Control for Vehicular Anti-Lock Braking System

Equivalence 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 information

متلب سایت MatlabSite.com

متلب سایت MatlabSite.com Vehicle Velocity Estimation based on Data fusion by Kalman Filtering for ABS Melika Amiri Graduate student in electrical engineering, Islamic Azad uniersity, Science and Research ehran, Iran Melika_64@yahoo.com

More information

Reversal in time order of interactive events: Collision of inclined rods

Reversal 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 information

Would you risk your live driving drunk? Intro

Would you risk your live driving drunk? Intro Martha Casquete Would you risk your lie driing drunk? Intro Motion Position and displacement Aerage elocity and aerage speed Instantaneous elocity and speed Acceleration Constant acceleration: A special

More information

VISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION

VISUAL 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 information

The hierarchical real-time control of high speed trains for automatic train operation

The 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 information

The Kinetic Theory of Gases

The 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 information

Dynamics ( 동역학 ) Ch.2 Motion of Translating Bodies (2.1 & 2.2)

Dynamics ( 동역학 ) Ch.2 Motion of Translating Bodies (2.1 & 2.2) Dynamics ( 동역학 ) Ch. Motion of Translating Bodies (. &.) Motion of Translating Bodies This chapter is usually referred to as Kinematics of Particles. Particles: In dynamics, a particle is a body without

More information

A possible mechanism to explain wave-particle duality L D HOWE No current affiliation PACS Numbers: r, w, k

A 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 information

(a) During the first part of the motion, the displacement is x 1 = 40 km and the time interval is t 1 (30 km / h) (80 km) 40 km/h. t. (2.

(a) During the first part of the motion, the displacement is x 1 = 40 km and the time interval is t 1 (30 km / h) (80 km) 40 km/h. t. (2. Chapter 3. Since the trip consists of two parts, let the displacements during first and second parts of the motion be x and x, and the corresponding time interals be t and t, respectiely. Now, because

More information

Kinetic plasma description

Kinetic plasma description Kinetic plasma description Distribution function Boltzmann and Vlaso equations Soling the Vlaso equation Examples of distribution functions plasma element t 1 r t 2 r Different leels of plasma description

More information

Displacement, Time, Velocity

Displacement, Time, Velocity Lecture. Chapter : Motion along a Straight Line Displacement, Time, Velocity 3/6/05 One-Dimensional Motion The area of physics that we focus on is called mechanics: the study of the relationships between

More information

State-space Modelling of Hysteresis-based Control Schemes

State-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 information

Note on Posted Slides. Motion Is Relative

Note on Posted Slides. Motion Is Relative Note on Posted Slides These are the slides that I intended to show in class on Tue. Jan. 9, 2014. They contain important ideas and questions from your reading. Due to time constraints, I was probably not

More information

Alternative non-linear predictive control under constraints applied to a two-wheeled nonholonomic mobile robot

Alternative 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 information

General Lorentz Boost Transformations, Acting on Some Important Physical Quantities

General Lorentz Boost Transformations, Acting on Some Important Physical Quantities General Lorentz Boost Transformations, Acting on Some Important Physical Quantities We are interested in transforming measurements made in a reference frame O into measurements of the same quantities as

More information

Lesson 2: Kinematics (Sections ) Chapter 2 Motion Along a Line

Lesson 2: Kinematics (Sections ) Chapter 2 Motion Along a Line Lesson : Kinematics (Sections.-.5) Chapter Motion Along a Line In order to specify a position, it is necessary to choose an origin. We talk about the football field is 00 yards from goal line to goal line,

More information

(a)!! d = 17 m [W 63 S]!! d opposite. (b)!! d = 79 cm [E 56 N] = 79 cm [W 56 S] (c)!! d = 44 km [S 27 E] = 44 km [N 27 W] metres. 3.

(a)!! d = 17 m [W 63 S]!! d opposite. (b)!! d = 79 cm [E 56 N] = 79 cm [W 56 S] (c)!! d = 44 km [S 27 E] = 44 km [N 27 W] metres. 3. Chapter Reiew, pages 90 95 Knowledge 1. (b). (d) 3. (b) 4. (a) 5. (b) 6. (c) 7. (c) 8. (a) 9. (a) 10. False. A diagram with a scale of 1 cm : 10 cm means that 1 cm on the diagram represents 10 cm in real

More information

Algebra Based Physics. Motion in One Dimension. 1D Kinematics Graphing Free Fall 2016.notebook. August 30, Table of Contents: Kinematics

Algebra Based Physics. Motion in One Dimension. 1D Kinematics Graphing Free Fall 2016.notebook. August 30, Table of Contents: Kinematics Table of Contents: Kinematics Algebra Based Physics Kinematics in One Dimension 06 03 www.njctl.org Motion in One Dimension Aerage Speed Position and Reference Frame Displacement Aerage Velocity Instantaneous

More information

A-level Mathematics. MM03 Mark scheme June Version 1.0: Final

A-level Mathematics. MM03 Mark scheme June Version 1.0: Final -leel Mathematics MM0 Mark scheme 660 June 0 Version.0: Final Mark schemes are prepared by the Lead ssessment Writer and considered, together with the releant questions, by a panel of subject teachers.

More information

Chapter (3) Motion. in One. Dimension

Chapter (3) Motion. in One. Dimension Chapter (3) Motion in One Dimension Pro. Mohammad Abu Abdeen Dr. Galal Ramzy Chapter (3) Motion in one Dimension We begin our study o mechanics by studying the motion o an object (which is assumed to be

More information

Centripetal force. Objectives. Assessment. Assessment. Equations. Physics terms 5/13/14

Centripetal force. Objectives. Assessment. Assessment. Equations. Physics terms 5/13/14 Centripetal force Objecties Describe and analyze the motion of objects moing in circular motion. Apply Newton s second law to circular motion problems. Interpret free-body force diagrams. 1. A race car

More information

Motion in Two and Three Dimensions

Motion in Two and Three Dimensions PH 1-1D Spring 013 Motion in Two and Three Dimensions Lectures 5,6,7 Chapter 4 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 4 Motion in Two and Three Dimensions In this chapter

More information

Draft 01PC-73 Sensor fusion for accurate computation of yaw rate and absolute velocity

Draft 01PC-73 Sensor fusion for accurate computation of yaw rate and absolute velocity Draft PC-73 Sensor fusion for accurate computation of yaw rate and absolute velocity Fredrik Gustafsson Department of Electrical Engineering, Linköping University, Sweden Stefan Ahlqvist, Urban Forssell,

More information

Note: the net distance along the path is a scalar quantity its direction is not important so the average speed is also a scalar.

Note: the net distance along the path is a scalar quantity its direction is not important so the average speed is also a scalar. PHY 309 K. Solutions for the first mid-term test /13/014). Problem #1: By definition, aerage speed net distance along the path of motion time. 1) ote: the net distance along the path is a scalar quantity

More information

Three-dimensional Guidance Law for Formation Flight of UAV

Three-dimensional Guidance Law for Formation Flight of UAV ICCAS25 Three-dimensional Guidance aw for Formation Flight of UAV Byoung-Mun Min * and Min-Jea Tahk ** * Department of Aerospace Engineering KAIST Daejeon Korea (Tel : 82-42-869-3789; E-mail: bmmin@fdcl.kaist.ac.kr)

More information

Physics 1: Mechanics

Physics 1: Mechanics Physics 1: Mechanics Đào Ngọc Hạnh Tâm Office: A1.53, Email: dnhtam@hcmiu.edu.n HCMIU, Vietnam National Uniersity Acknowledgment: Most of these slides are supported by Prof. Phan Bao Ngoc credits (3 teaching

More information

MOTION OF FALLING OBJECTS WITH RESISTANCE

MOTION 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 information

A new Framework for the Analysis of Simultaneous Events

A new Framework for the Analysis of Simultaneous Events A new ramework for the Analysis of Simultaneous ents Christoph Barz Rolf Göpffarth Peter Martini Andre Wenzel Uniersity of Bonn Institute of Computer Science IV Roemerstr. 164 D-53117 Bonn Germany {barzrggmartiniwenzel}@cs.uni-bonn.de

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 7-4: CONSERVATION OF ENERGY AND MOMENTUM IN COLLISIONS LSN 7-5: ELASTIC COLLISIONS IN ONE DIMENSION LSN 7-6: INELASTIC COLLISIONS Questions From

More information

FEEDFORWARD COMPENSATION FOR LATERAL CONTROL OF HEAVY VEHICLES FOR AUTOMATED HIGHWAY SYSTEM (AHS)

FEEDFORWARD COMPENSATION FOR LATERAL CONTROL OF HEAVY VEHICLES FOR AUTOMATED HIGHWAY SYSTEM (AHS) Copyright IFAC 5th Triennial World Congress, Barcelona, Spain FEEDFORWARD COMPENSATION FOR LATERAL CONTROL OF HEAVY VEHICLES FOR AUTOMATED HIGHWAY SYSTEM (AHS) Meihua Tai, Masayoshi Tomizuka Department

More information

Physics 2A Chapter 3 - Motion in Two Dimensions Fall 2017

Physics 2A Chapter 3 - Motion in Two Dimensions Fall 2017 These notes are seen pages. A quick summary: Projectile motion is simply horizontal motion at constant elocity with ertical motion at constant acceleration. An object moing in a circular path experiences

More information

Simulations of Space Probes and their Motions Relative to the Host Orbital Station

Simulations of Space Probes and their Motions Relative to the Host Orbital Station Simulations of Space robes and their Motions Relatie to the Host Orbital Station Eugene I. Butiko St. etersburg State Uniersity, St. etersburg, Russia Abstract Launching a space probe from an orbiting

More information

Chapter 2 Motion Along a Straight Line

Chapter 2 Motion Along a Straight Line Chapter Motion Along a Straight Line In this chapter we will study how objects moe along a straight line The following parameters will be defined: (1) Displacement () Aerage elocity (3) Aerage speed (4)

More information

Experiments of Earthquake Early Warning to Expressway Drivers using Plural Driving Simulators

Experiments of Earthquake Early Warning to Expressway Drivers using Plural Driving Simulators nd International Conference on Urban Disaster Reduction November ~9, Experiments of Earthquake Early Warning to Expressway Drivers using Plural Driving Simulators Fumio Yamazaki 1*, Yoshihisa Maruyama

More information

FREEWAY WEAVING. Highway Capacity Manual 2000 CHAPTER 24 CONTENTS EXHIBITS

FREEWAY WEAVING. Highway Capacity Manual 2000 CHAPTER 24 CONTENTS EXHIBITS CHAPTER 24 FREEWAY WEAVING CONTENTS I. INTRODUCTION... 24-1 Scope of the Methodology...24-1 Limitations of the Methodology...24-1 II. METHODOLOGY...24-1 LOS...24-2 Weaing Segment Parameters...24-3 Determining

More information

1 INTRODUCTION 2 PROBLEM DEFINITION

1 INTRODUCTION 2 PROBLEM DEFINITION Autonomous cruise control with cut-in target vehicle detection Ashwin Carvalho, Alek Williams, Stéphanie Lefèvre & Francesco Borrelli Department of Mechanical Engineering University of California Berkeley,

More information

Parameters Identification of Equivalent Circuit Diagrams for Li-Ion Batteries

Parameters 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 information

A universal model-free and safe adaptive cruise control mechanism

A universal model-free and safe adaptive cruise control mechanism A uniersal model-free and safe adaptie cruise control mechanism Thomas Berger and Anna-Lena Rauert Abstract We consider the problem of ehicle following, where a safety distance to the leader ehicle is

More information

DYNAMICS. Kinematics of Particles VECTOR MECHANICS FOR ENGINEERS: Tenth Edition CHAPTER

DYNAMICS. Kinematics of Particles VECTOR MECHANICS FOR ENGINEERS: Tenth Edition CHAPTER Tenth E CHAPTER 11 VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Ferdinand P. Beer E. Russell Johnston, Jr. Phillip J. Cornwell Lecture Notes: Brian P. Self California Polytechnic State Uniersity Kinematics

More information

Low Complexity MPC Schemes for Integrated Vehicle Dynamics Control Problems

Low Complexity MPC Schemes for Integrated Vehicle Dynamics Control Problems AVEC 8 Low Complexity MPC Schemes for Integrated Vehicle Dynamics Control Problems Paolo Falcone, a Francesco Borrelli, b H. Eric Tseng, Jahan Asgari, Davor Hrovat c a Department of Signals and Systems,

More information

Note on Posted Slides. Chapter 3 Pre-Class Reading Question. Chapter 3 Reading Question : The Fine Print. Suggested End of Chapter Items

Note on Posted Slides. Chapter 3 Pre-Class Reading Question. Chapter 3 Reading Question : The Fine Print. Suggested End of Chapter Items Note on Posted Slides These are the slides that I intended to show in class on Wed. Jan. 9, 2013. They contain important ideas and questions from your reading. Due to time constraints, I was probably not

More information

Trajectory Estimation for Tactical Ballistic Missiles in Terminal Phase Using On-line Input Estimator

Trajectory 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 information

Motion in Two and Three Dimensions

Motion in Two and Three Dimensions PH 1-A Fall 014 Motion in Two and Three Dimensions Lectures 4,5 Chapter 4 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 4 Motion in Two and Three Dimensions In this chapter

More information

Magnetic braking: Finding the effective length over which the eddy currents form

Magnetic braking: Finding the effective length over which the eddy currents form Magnetic braking: Finding the effectie length oer which the eddy currents form Scott B. Hughes Physics Department, The College of Wooster, Wooster, Ohio 44691 May 5, 2000 This experiment uses a square

More information

4-vectors. Chapter Definition of 4-vectors

4-vectors. Chapter Definition of 4-vectors Chapter 12 4-ectors Copyright 2004 by Daid Morin, morin@physics.harard.edu We now come to a ery powerful concept in relatiity, namely that of 4-ectors. Although it is possible to derie eerything in special

More information

Feb 6, 2013 PHYSICS I Lecture 5

Feb 6, 2013 PHYSICS I Lecture 5 95.141 Feb 6, 213 PHYSICS I Lecture 5 Course website: faculty.uml.edu/pchowdhury/95.141/ www.masteringphysics.com Course: UML95141SPRING213 Lecture Capture h"p://echo36.uml.edu/chowdhury213/physics1spring.html

More information

Frontiers in Heat Pipes. Available at

Frontiers in Heat Pipes. Available at Frontiers in Heat Pipes Aailable at www.thermalfluidscentral.org AN EXPERIMENTAL INVESTIGATION OF THE THICKNESS OF THE LIQUID-FILM DEPOSITED AT THE TRAILING END OF A LIQUID PLUG MOVING IN THE CAPILLARY

More information

THE FIFTH DIMENSION EQUATIONS

THE FIFTH DIMENSION EQUATIONS JP Journal of Mathematical Sciences Volume 7 Issues 1 & 013 Pages 41-46 013 Ishaan Publishing House This paper is aailable online at http://www.iphsci.com THE FIFTH DIMENSION EQUATIONS Niittytie 1B16 03100

More information

, remembering that! v i 2

, remembering that! v i 2 Section 53: Collisions Mini Inestigation: Newton s Cradle, page 34 Answers may ary Sample answers: A In Step, releasing one end ball caused the far ball on the other end to swing out at the same speed

More information

Modeling Highway Traffic Volumes

Modeling Highway Traffic Volumes Modeling Highway Traffic Volumes Tomáš Šingliar1 and Miloš Hauskrecht 1 Computer Science Dept, Uniersity of Pittsburgh, Pittsburgh, PA 15260 {tomas, milos}@cs.pitt.edu Abstract. Most traffic management

More information

Collective circular motion of multi-vehicle systems with sensory limitations

Collective circular motion of multi-vehicle systems with sensory limitations Proceedings of the 44th IEEE Conference on Decision and Control, and the European Control Conference 2005 Seille, Spain, December 12-15, 2005 MoB032 Collectie circular motion of multi-ehicle systems with

More information

ERAD THE SEVENTH EUROPEAN CONFERENCE ON RADAR IN METEOROLOGY AND HYDROLOGY

ERAD 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 information

0 a 3 a 2 a 3 0 a 1 a 2 a 1 0

0 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 information

1. Linear Motion. Table of Contents. 1.1 Linear Motion: Velocity Time Graphs (Multi Stage) 1.2 Linear Motion: Velocity Time Graphs (Up and Down)

1. Linear Motion. Table of Contents. 1.1 Linear Motion: Velocity Time Graphs (Multi Stage) 1.2 Linear Motion: Velocity Time Graphs (Up and Down) . LINEAR MOTION www.mathspoints.ie. Linear Motion Table of Contents. Linear Motion: Velocity Time Graphs (Multi Stage). Linear Motion: Velocity Time Graphs (Up and Down).3 Linear Motion: Common Initial

More information

Last Time: Start Rotational Motion (now thru mid Nov) Basics: Angular Speed, Angular Acceleration

Last Time: Start Rotational Motion (now thru mid Nov) Basics: Angular Speed, Angular Acceleration Last Time: Start Rotational Motion (now thru mid No) Basics: Angular Speed, Angular Acceleration Today: Reiew, Centripetal Acceleration, Newtonian Graitation i HW #6 due Tuesday, Oct 19, 11:59 p.m. Exam

More information

10. Yes. Any function of (x - vt) will represent wave motion because it will satisfy the wave equation, Eq

10. 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 information

Lecture #8-6 Waves and Sound 1. Mechanical Waves We have already considered simple harmonic motion, which is an example of periodic motion in time.

Lecture #8-6 Waves and Sound 1. Mechanical Waves We have already considered simple harmonic motion, which is an example of periodic motion in time. Lecture #8-6 Waes and Sound 1. Mechanical Waes We hae already considered simple harmonic motion, which is an example of periodic motion in time. The position of the body is changing with time as a sinusoidal

More information

Chapter 3 Motion in a Plane

Chapter 3 Motion in a Plane Chapter 3 Motion in a Plane Introduce ectors and scalars. Vectors hae direction as well as magnitude. The are represented b arrows. The arrow points in the direction of the ector and its length is related

More information

Why does Saturn have many tiny rings?

Why does Saturn have many tiny rings? 2004 Thierry De Mees hy does Saturn hae many tiny rings? or Cassini-Huygens Mission: New eidence for the Graitational Theory with Dual Vector Field T. De Mees - thierrydemees @ pandora.be Abstract This

More information

Modeling Hydraulic Accumulators for use in Wind Turbines

Modeling 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 information

Physics 4A Solutions to Chapter 4 Homework

Physics 4A Solutions to Chapter 4 Homework Physics 4A Solutions to Chapter 4 Homework Chapter 4 Questions: 4, 1, 1 Exercises & Problems: 5, 11, 3, 7, 8, 58, 67, 77, 87, 11 Answers to Questions: Q 4-4 (a) all tie (b) 1 and tie (the rocket is shot

More information

Spiral length design

Spiral length design Spiral length design Nazmul Hasan *1 1 SNC-AVAIN INC. Transportation Diision,1800-1075 West Georgia Street, Vanocuer, British Columbia, Canada V6E C9, Tel: 604-66-555, Fax: 604-66-7688, Nazmul.Hasan@snclaalin.com

More information

DYNAMICS. Kinematics of Particles Engineering Dynamics Lecture Note VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER

DYNAMICS. Kinematics of Particles Engineering Dynamics Lecture Note VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER 27 The McGraw-Hill Companies, Inc. All rights resered. Eighth E CHAPTER 11 VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Ferdinand P. Beer E. Russell Johnston, Jr. Kinematics of Particles Lecture Notes: J.

More information

PY1008 / PY1009 Physics Rotational motion

PY1008 / PY1009 Physics Rotational motion PY1008 / PY1009 Physics Rotational motion M.P. Vaughan Learning Objecties Circular motion Rotational displacement Velocity Angular frequency, frequency, time period Acceleration Rotational dynamics Centripetal

More information

Tools for Investigation of Dynamics of DC-DC Converters within Matlab/Simulink

Tools 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 information

>

> The grade length should include 5% of the length of the ertical cures at the start and end of the grade. With two consecutie upgrades, 50% of the length of the ertical cure joining them should be included.

More information

Are the two relativistic theories compatible?

Are the two relativistic theories compatible? Are the two relatiistic theories compatible? F. Selleri Dipartimento di Fisica - Uniersità di Bari INFN - Sezione di Bari In a famous relatiistic argument ("clock paradox") a clock U 1 is at rest in an

More information

Cases of integrability corresponding to the motion of a pendulum on the two-dimensional plane

Cases of integrability corresponding to the motion of a pendulum on the two-dimensional plane Cases of integrability corresponding to the motion of a pendulum on the two-dimensional plane MAXIM V. SHAMOLIN Lomonoso Moscow State Uniersity Institute of Mechanics Michurinskii Ae.,, 99 Moscow RUSSIAN

More information

Chapter 11 Collision Theory

Chapter 11 Collision Theory Chapter Collision Theory Introduction. Center o Mass Reerence Frame Consider two particles o masses m and m interacting ia some orce. Figure. Center o Mass o a system o two interacting particles Choose

More information

Distribution of relative velocities of particles in turbulent flows

Distribution of relative velocities of particles in turbulent flows Distribution of relatie elocities of particles in turbulent flows B. Mehlig Department of Physics, Göteborg Uniersity, Sweden Bernhard.Mehlig@physics.gu.se Financial support by Vetenskapsrådet, the Platform

More information

Collective circular motion of multi-vehicle systems with sensory limitations

Collective 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 information

PROBLEM Copyright McGraw-Hill Education. Permission required for reproduction or display. SOLUTION. ω = 29.6 rad/s. ω = = 36 3.

PROBLEM Copyright McGraw-Hill Education. Permission required for reproduction or display. SOLUTION. ω = 29.6 rad/s. ω = = 36 3. PROLEM 15.1 The brake drum is attached to a larger flywheel that is not shown. The motion of the brake drum is defined by the relation θ = 36t 1.6 t, where θ is expressed in radians and t in seconds. Determine

More information

4. 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. 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 information

So now that we ve mentioned these terms : kinetic, potential, work we should try to explain them more. Let s develop a model:

So now that we ve mentioned these terms : kinetic, potential, work we should try to explain them more. Let s develop a model: Lecture 12 Energy e are now at the point where we can talk about one of the most powerful tools in physics, energy. Energy is really an abstract concept. e hae indicators of energy (temperature, elocity

More information

Single-track models of an A-double heavy vehicle combination

Single-track models of an A-double heavy vehicle combination Single-track models of an A-double heavy vehicle combination PETER NILSSON KRISTOFFER TAGESSON Department of Applied Mechanics Division of Vehicle Engineering and Autonomous Systems Vehicle Dynamics Group

More information

Section 6: PRISMATIC BEAMS. Beam Theory

Section 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 information

HSC Physics Core 9.2 Space! Part 2: Launching into orbit! Overview of Part 2:!

HSC Physics Core 9.2 Space! Part 2: Launching into orbit! Overview of Part 2:! Go to the ideo lesson for this slide deck: h2p://edrolo.com.au/subjects/physics/hsc- physics/space- part- 2/escape- elocity/lesson/ HSC Physics Core 9.2 Space Part 2: Launching into orbit Oeriew of Part

More information