1 Coordinate Systems and Vectors Kinematics in Two-Dimensions: Projectile Motion 8.01 W02D1 Announcements Problem Set 1 Due Week 02 Tuesday at 9 pm Math Review Week Tuesday at 9 pm in 26-152 Register your clicker on the website Register your group on the website. Exam 1 Thursday September 18 from 7:30-9:30 pm Cartesian Coordinate System 1. An origin as the reference point 2. A set of coordinate axes with scales and labels 3. Choice of positive direction for each axis Coordinate system: used to describe the position of a point in space and consists of Cartesian Coordinate System2 Vector A vector is a quantity that has both direction and magnitude. The magnitude of is denoted by | A≡A |ASpatial Properties of Vectors Vectors can exist at any point P in space. Vector equality: Any two vectors that have the same direction and magnitude are equal no matter where in space they are located. Vector Addition ABLet and be two vectors. Define a new vector , the “vector addition” of and , by the geometric construction shown in either figure = +C A B AB “head-to-tail” “parallelogram”3 Vector Decomposition in Two Dimensions Consider a vector x- and y- components: Magnitude: Direction: ( 0)x yA , A ,=AAx= A cos(θ), Ay= Asin(θ) A = Ax2+ Ay2AyAx=Asin(θ)A cos(θ)= tan(θ) θ= tan−1( Ay/ Ax)Group Problem: Displacement Vector A person runs 250 m along the Infinite Corridor at MIT from Mass Ave to the end of Building 8, turns right at the end of the corridor and runs 178 m to the end of Building 2, and then turns right and runs 30 m down the hall. What is the direction and magnitude of the displacement vector between start and finish? Concept Question: Magnitudes and Components Can a component of a vector have a magnitude greater than the magnitude of the vector? 1. Yes. 2. No. 3. Depends on the vector in question.4 Unit Vectors and Components The idea of multiplication by real numbers allows us to define a set of unit vectors at each point in space with Then vector decomposition with components vectors: and components: Thus ( )ˆ ˆˆ, ,i j k1, 1, 1ˆ ˆˆ| | | | | |= = =i j kx x y y z zˆ ˆˆA , A , A= = =A i A j A k x y zˆ ˆˆA A A= + +A i j k( )x y zA , A , A=A A =Ax+Ay+AzVector Addition Vector Sum: Components A = A cos(θA)ˆi + Asin(θA)ˆj B = B cos(θB)ˆi + Bsin(θB)ˆj= +C A B Cx= Ax+ Bx, Cy= Ay+ ByCx= C cos(θC) = Acos(θA)+ B cos(θB)Cy= C sin(θC) = Asin(θA) + Bsin(θB)ˆ ˆ ˆ ˆ( ) ( ) cos( ) sin( )x x y y C CA B A B C Cθ θ= + + + = +C i j i jVector Description of Two-Dimensional Motion Position Displacement Velocity Acceleration ˆ ˆ( ) ( ) ( )t x t y t= +r i j( ) ( )ˆ ˆ ˆ ˆ( ) ( ) ( )x ydx t dy tt v t v tdt dt= + ≡ +v i j i j( )( )ˆ ˆ ˆ ˆ( ) ( ) ( )yxx ydv tdv tt a t a tdt dt= + ≡ +a i j i jˆ ˆ( ) ( ) ( )t x t y tΔ = Δ + Δr i j5 Position, Velocity, and Accelerations in Different Reference Frames Reference Systems Use coordinate system as a ‘reference frame’ to describe the position, velocity, and acceleration of objects. Position Vectors in Different Reference Frames Two reference frames, Frame 1 denoted by O1 and Frame 2 denoted by O2. Origins do not coincide. Object has different position vectors in different frames 1 2= +r R r 6 Law of Addition of Velocities Suppose an object is moving; then, observers in different reference frames will measure different velocities Velocity of Frame 2 with respect to Frame 1: Velocity of the object in Frame 1: Velocity of the object in Frame 2: Velocity of an object in two different reference frames 1 1d dt=v r2 2d dt=v r dr1dt=dRdt+dr2dt⇒v1=V +v2 V = dR / dtConcept Question: Relatively Inertial Reference Frames Suppose Frames 1 and 2 are relatively inertial reference frames. 1) An object that is at rest in Frame 2 is moving at a constant velocity in reference Frame 1. 2) An object that is accelerating in Frame 2 has the same acceleration in reference Frame 1. 3) An object that is moving at constant velocity in Frame 2 is accelerating in reference Frame 1. 4) An object that is accelerating in Frame 2 is moving at constant velocity in reference Frame 1. 5) Two of the above 6) None of the above Group Problem: Law of Addition of Velocities Suppose two cars, Car 1, and Car 2, are traveling along roads that are perpendicular to each other. Reference Frame A is at rest with respect to the ground. Reference Frame B is at rest with respect to Car 1. Choose unit vectors such that Car 1 is moving in the positive y-direction, and Car 2 is moving in the positive x-direction in reference Frame A. a) What is the vector description of the velocity of Car 2 in Reference Frame B? b) What is the magnitude of the velocity of Car 2 as observed in Reference Frame B? c) What angle does the velocity of Car 2 make with respect to the positive x-direction as observed in Reference Frame B?7 Law of Addition of Accerelations Suppose an object is moving; then, observers in different reference frames will measure different accelerations Acceleration of Frame 2 with respect to Frame 1: Acceleration of the object in Frame 1: Acceleration of the object in Frame 2: Acceleration of an object in two different reference frames a1= dv1dt2 2d dt=v r dv1dt=dVdt+dv2dt⇒a1=A +a2 A = dV / dtRelatively Inertial Reference Frames Two reference frames with the zero relative acceleration One moving object has different position vectors in different frames Law of addition of velocities Acceleration in either reference frame is the same 1 2= +r R r v1=V +v2d dt= =A V 0 V = dR dt a1=A +a2=a2Projectile Motion: Components of Acceleration Force: Newton’s Second Law: Acceleration: ay= − g ax= 029.8 m/sg = F = −mgˆj −mgˆj = ma a = − gˆj8 Demo: Relative Motion Gun A7 Video Link: http://tsgphysics.mit.edu/front/index.php?page=demo.php?letnum=A%207&show=0 Concept Q.: Which Hits First? A person simultaneously throws two objects in the air. The objects leave the person’s hands at different angles and travel along the parabolic trajectories indicated by A and B in the figure below. Which of the
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