Physics. Session Kinematics - 4 Session Opener X Y O X Y O X Y O X Y O Who is moving ? Who is at rest ? Everything is relative.

Slides:



Advertisements
Similar presentations
Motion in Two Dimensions
Advertisements

Physics. Session Kinematics - 3 Session Objectives Problems ? Free fall under gravity.
Vectors and Two Dimensional Motion
2009 Physics 2111 Fundamentals of Physics Chapter 3 1 Fundamentals of Physics Chapter 3 Motion in 2 &3 Dimensions 1.Moving in 2 &3 Dimensions 2.Position.
Relative Velocity.
Chapter 5 Projectile motion. 1. Recall: a projectile is an object only acted upon by gravity.
Chapter 2 MOTION IN TWO DIMENSIONS
Motion in Two Dimensions
Solutions to 1st Major 111.
Lecture III Curvilinear Motion.
Chapter 5 Projectile motion
Free Fall & Vectors in Physics
Vectors and Scalars AP Physics C.
What about this??? Which one is false?. Aim & Throw where????
SPH4U – Grade 12 Physics Unit 3
Physics. Session Kinematics - 2 Session Opener REST ! or MOTION.
Vectors and Scalars AP Physics B. Scalar A SCALAR is ANY quantity in physics that has MAGNITUDE, but NOT a direction associated with it. Magnitude – A.
Vectors Vector: a quantity that has both magnitude (size) and direction Examples: displacement, velocity, acceleration Scalar: a quantity that has no.
Problems Ch(1-3).
What is motion? Motion is the change in the position of an object. To describe the motion of an object we use terms like: Distance, displacement, speed,
Lecture 4: More kinematics. Displacement and change in displacement Position vector points from the origin to a location. The displacement vector points.
A River Problem A crocodile is lurking beside the Platte River. It spots an unsuspecting juggler on the bank of the river exactly opposite.
Chapter 3 Acceleration and Newton’s Second Law of Motion.
Motion in a Plane We set up a reference frame.
Forces in Two Dimensions
Problems Ch(1-3).
AP Physics.  Think of a curve being traced out over time, sometimes doubling back on itself or crossing itself. Such a curve cannot be described by a.
Ch. 3 Vectors & Projectile Motion. Scalar Quantity Described by magnitude only – Quantity Examples: time, amount, speed, pressure, temperature.
2-Dimensional Kinematics Unit 2 Presentation 2. Projectile Problems  Projectile Motion: The two- dimensional (x and y) motion of an object through space.
College Physics, 7th Edition
Two-Dimensional Motion and VectorsSection 1 Preview Section 1 Introduction to VectorsIntroduction to Vectors Section 2 Vector OperationsVector Operations.
One Dimensional Kinematics: Problem Solving Kinematics in Two-Dimensions: Law of Addition of Velocities Projectile Motion 8.01 W02D1.
Vectors. Vectors and Scalars A vector has magnitude as well as direction. Some vector quantities: displacement, velocity, force, momentum A scalar has.
Physics. Session Kinematics - 1 Session Opener You fly from Delhi to Mumbai New Delhi Mumbai Hyderabad Then you fly from Mumbai to Hyderabad Does it.
Chapter 4 Motion in Two Dimensions. Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail.
MOTION RELATIVE TO ROTATING AXES
Chapter 4 Motion in two and three dimensions. Two principles for 2D and 3D motions: Two principles for 2D and 3D motions: 1) The principle of independence.
Physics. Session Kinematics - 5 Session Opener How far can this cannon fire the shot? Courtesy :
Kinematics in Two Dimensions
Chapter 4 Two-Dimensional Kinematics. Units of Chapter 4 Motion in Two Dimensions Projectile Motion: Basic Equations Zero Launch Angle General Launch.
Chapter 4 MOTION IN TWO DIMENSIONS. Two dimensions One dimension Position O x M x x y M Path of particle O x y.
KINEMATICS OF PARTICLES
3.1 & 3.2 Vectors & Scalars. Biblical Reference The Lord will grant that the enemies who rise up against you will be defeated before you. They will come.
Lecture 3:. Freely Falling Objects Free fall from rest: Free fall is the motion of an object subject only to the influence of gravity. The acceleration.
Lecture 6: Vectors & Motion in 2 Dimensions (part II)
Warm-Up 09/02/10 Vera is speeding down the interstate at 45.0 m/s when she sees an accident in the middle of the road. By the time Vera slams on the breaks,
Advanced Physics Chapter 3 Kinematics in Two Dimensions; Vectors.
Module 1.1 – Displacement and Velocity Vectors
R. Field 1/22/2013 University of Florida PHY 2053Page 1 2-d Motion: Constant Acceleration Kinematic Equations of Motion (Vector Form) The velocity vector.
University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 6 Dr.-Ing. Erwin Sitompul
VECTORS. BIG IDEA: Horizontal and vertical motions of an object are independent of one another.
Chapter 3 Kinematics in More Dimensions; Vectors.
Chapter 3: Two-Dimensional Motion and Vectors
CONTENTS  Scalars and Vectors.  Bearings & Compass headings.  Drawing Vectors.  Vector addition & subtraction.  Relative velocity.  Change in.
Motion in Two and Three Dimensions Chapter 4. Position and Displacement A position vector locates a particle in space o Extends from a reference point.
PHY 151: Lecture Position, Velocity, and Acceleration Vectors
Kinematics in Two Dimensions Vectors
Motion in Two Dimensions
Physics 1: Mechanics Đào Ngọc Hạnh Tâm
Chapter 3: Motion in Two and Three Dimensions
Chapter 3: Motion in Two and Three Dimensions
Relative Motion © Brendan Doheny, Applied Maths Facilitator,
Motion in Two Dimensions
a is always perpendicular to vx a is always perpendicular to vy
Last Time: Vectors Introduction to Two-Dimensional Motion Today:
Physics C Relative Motion
Motion in Two Dimensions
A scalar is only a magnitude with appropriate units.
Chapter 3 Vectors Questions 3-1 Vectors and Scalars
Vectors.
Presentation transcript:

Physics

Session Kinematics - 4

Session Opener X Y O X Y O X Y O X Y O Who is moving ? Who is at rest ? Everything is relative

Session Objective 1.Two dimensional motion with constant acceleration 2.Relative displacement 3.Relative velocity 4.River and Boat problem 5.Rain and Man problem

2 D Equations of motion

have different directions Motion is curvilinear. Both x and y components separately satisfy the equations

Till now we have discussed motion w.r.t. only a single frame of reference. The position, velocity and acceleration of a particle depends on the frame chosen. Relative Velocity

Consider position of a point P w.r.t. two frames of reference A & B : A B P Here Differentiating the equation w.r.t. time : Where, is velocity of pt. P w.r.t A And so on … Important equation-(1)

Class Exercise - 1 Which one of the following represent(s) the displacement-time graph of two objects A and B moving with zero relative speed? (a) (b) (c) (d)

Solution Displacement of A w.r.t. B remains constant with time. Hence answer is a, b

Relative Velocity If the two frames A & B are fixed w.r.t to each other we get : & Note: To avoid non inertial frames we assume no relative acceleration between the frames A & B, hence on further differentiating the velocity equation we get : as

Relative Velocity in 1D As there is 1 axis of motion there are two possible cases : From the equation we derived above we have : Here, g=ground or 1) The particles move in same direction : 12

Relative Velocity in 1D 2) The particles move in opposite directions : Thus relative velocity is higher when velocities are in opposite directions 12

Class Exercise - 4 V BA = 10 m/s at t = 0; a A = 2 m/s 2 ; a B = 3 m / s 2. Find the relative displacement of B with respect to A after t = 2 s. Solution:

Class Exercise - 5 An elevator whose floor to ceiling distance is 2.50 m, starts ascending with a constant acceleration of 1.25 m/s s after the start, a bolt begins to fall from the ceiling of the elevator. Calculate (i) free fall time of the bolt, (ii) displacement and distance covered by the bolt during the free fall in the reference frame fixed to the shaft of the elevator. g = 10 ms –2.

Solution Let us consider the line of motion of elevator and bolt as the Y-axis and the floor’s initial position (when the bolt starts falling) as origin. (i)At the moment when the bolt starts falling, speed of the elevator and the bolt = 0 + at = 0 + 1(1.25) = 1.25 m/s Let t’ be the time after which the bolt strikes the floor. The y-coordinate of the bolt and floor at time t’ are respectively (As the bolt is freely falling, its acceleration is –g)

Solution As the bolt strikes the floor at time t’, y b = y f  t’ – gt ’2 = t’ + (1.25)t’ 2 (b) S b = vt’ + at ’2

Solution The bolt goes up from P to Q and then goes down from Q to R.  Distance covered = 2(PQ) + QR

River & boat problem in 1D Note upstream flow will take place only if : 1) Boat flows downstream (with the flow) 2) Boat flows upstream (against the flow) Here, b=boat, r=river, g=ground

Relative Velocity in 2D The basic equation of relative velocity are the same. Here vectors are used for describing directional aspects of motion.

Class Exercise - 3 There are two reference frames XY with the origin O and X’Y’ with the origin O’. The velocity of an object as observed from O is m/s. The velocity of an object as observed from O’ is m/s. Find the velocity of O’ as observed from O. Solution:

Class Exercise - 10 Three persons are located at the vertices of an equilateral triangle whose sides equal a. They all start moving simultaneously with velocity v constant in magnitude with the first person heading continuously for the second, the second for the third and the third for the first. They will meet after time

Solution Hence answer is (a) For the motions of B and Cx rel = a

The motion of a boat or a man across a river 1)Motion through the shortest distance from A to B: h A BC In the above case the man’s velocity w.r.t the river has two components 1)perpendicular to the flow 2)against the flow

The motion of a boat or a man across a river Shortest Distance = AB From fig. we get velocity of man along AB. Here, m=man r=river g=ground Velocity component: 1)Perpendicular to flow 2) against flow

The motion of a boat or a man across a river 2) Motion taking the shortest time to go across the river The man will take least time to reach the other side of the river when the value of his velocity component perpendicular to the flow of river is maximum. From 1 & 2 it is clear that this happens when : h 1 2

Class Exercise - 7 The velocity of a river is 3 km/hr. The velocity of a man with respect to the river is 5 km/hr. Find the time taken by the man to reach the opposite bank if the path that he takes to swim across makes an angle of 60° with the horizontal. (Width of the river = 1.5 km) Solution: V mr = 5 km/hr V rg = 3 km/hr

Class Exercise - 8 In the above question, if the man reaches the opposite bank of the river at a distance x directly from the opposite point on the river, then x will be equal to (a)1.6 km(b) 1.75 km (c) 1.9 km(d) 2.1 km Solution: x = (V rg + V mr cos60°) × t x = 1.9 km Hence answer is (c).

Class Exercise - 9 Two ships are 10 km apart on a line running south to north. The one farther north is steaming west at 20 km/hr. The other is moving north at 20 km/hr. What is their distance of the closest approach and how long do they take to reach it? Solution: Suppose the two ships are at X and Y moving with velocities u and v respectively (each 20 km/hr) If A is an observer and B is moving towards X, then the closest approach of B to A is AN.

Solution (The perpendicular drawn from A to BX) The velocity of Y relative to X =  = 45º From DQPR, the ship Y will move along a direction QR relative to the ship X, where QR is at 45º to PQ, the north-south direction, when the relative velocity is considered, the ship X is at rest.

Solution The distance of the closest approach PN = PQ sin45º = (10 km) = km The distance QN = PQ cos45º = km

To cross along AB with respect to ground: If V mr = 5 m/s as shown and V rg = 4 m/s due east then what should be the velocity of man with respect to ground and the time taken to cross the river if d =30m? h A BC N E S W Man crossing a river - shortest path

Here, m=man r=river g=ground Shortest time For shortest time the velocity of man with respect to river should be parallel to AB. A h CB Man crossing a river - shortest path

Class Exercise - 6 A man standing on a road has to hold his umbrella at 30° vertical to keep the rain away. He throws the umbrella and starts running at 10 km/hr. He finds that raindrops are hitting his head vertically. Find the speed of rain-drops with respect to (i) the road, (ii) the moving man. Solution: Let v 1 = Velocity of rain with respect to the ground, v 2 = Velocity of the man running on the ground = 10 km/hr,

Solution v 3 = Velocity of rain with respect to the moving man directed vertically. Resolving v 1 along the X- and Y-axes, or v 1 = 2v 2 = 20 km/hr

Thank you