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Transcript of In this chapter we will study 4.1 The Position, Velocity and Acceleration vectors 4.3Projectile...
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Chapter 4Motion in Two Dimensions
In this chapter we will study
4.1The Position, Velocity and Acceleration vectors
4.3 Projectile Motion
4.4 Uniform Circular Motion
4.5 Tangential and Radial Acceleration
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Displacement Vector1 2For a particle that changes position vector from to we define the displacement
vector as follows:
r r
r
2 1.r r r
1 2The position vectors and are written in terms of components asr r
1 1 1 1ˆ ˆ ˆi j kr x y z
2 2 2 2
ˆ ˆ ˆi j kr x y z
2 1 2 1 2 1ˆ ˆ ˆ ˆ ˆ ˆi j k i j kr x x y y z z x y z
2 1x x x 2 1y y y
2 1z z z
The displacement r can then be written as
ˆ ˆ ˆ3i 2 j 5kr m
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Average and Instantaneous Velocity
Following the same approach as in Chapter 2 we define the average velocity as
displacementaverage velocity =
time interval
avg
ˆ ˆ ˆ ˆ ˆ ˆi j k i j kr x y z x y zv
t t t t t
We define the instantaneous velocity (or more simply the velocity) as the limit:
lim
0
r drv
t dtt
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Average and Instantaneous Acceleration The average acceleration is defined as:
change in velocityaverage acceleration =
time interval2 1
avg
v v va
t t
We define the instantaneous acceleration as the limit:
ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆ ˆlim i j k i j k i j k
0
yx zx y z x y z
dvdv dvv dv da v v v a a a
t dt dt dt dt dtt
The three acceleration components are given by the equations
xx
dva
dt
yy
dva
dt z
z
dva
dt dv
adt
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PROJECTILE MOTION
Sadia KhanPHYS 101
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In this lecture we will study1 Projectile Motion
2 Some important Terms
3 Horizontal “Velocity” Component
4 Vertical “Velocity” Component
5 Horizontally Launched Projectiles
6 Vertically Launched Projectiles
7 Time of Flight
8 Horizontal Range
9 Vertical Height
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A particle moves in a vertical plane with some initial velocity but its acceleration is always the free-fall acceleration g, which is downward. Such a particle is called a projectile and its motion is called projectile motion.
WHAT IS PROJECTILE MOTION?
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SOME IMPORTANT TERMS
Point of projection: The point from where the object is projected.
Angle of projection: The angle made by the projectile at point of projection.
Time of flight: Time taken by the projectile to remain in air.
Point of landing: The point at which projectile strikes.
Range: Maximum horizontal distance covered by the projectile.
Height: Maximum vertical distance reached by the projectile.
Trajectory: Path followed by the projectile.
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PROJECTILES MOVE IN TWO DIMENSIONS
Since a projectile moves in 2-dimensions, therefore its velocity has two components just like a resultant vector.
Horizontal and Vertical
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HORIZONTAL “VELOCITY” COMPONENT
It NEVER changes, covers equal displacements in equal time periods. This means the initial horizontal velocity equals the final horizontal velocity.
In other words, the horizontal velocity is CONSTANT. BUT WHY?
Gravity DOES NOT work horizontally to increase or decrease the velocity.
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VERTICAL “VELOCITY” COMPONENT
It changes (due to gravity), does NOT cover equal displacements in equal time periods.
Both the MAGNITUDE and DIRECTION change.
As the projectile moves up the MAGNITUDE DECREASES and its direction is UPWARD.
As it moves down the MAGNITUDE INCREASES and the direction is DOWNWARD.
Component Magnitude Direction
Horizontal Constant Constant
Vertical Changes Changes
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HORIZONTALLY LAUNCHED PROJECTILES
Projectiles which have NO upward trajectory and NO initial VERTICAL velocity.
𝒗 𝒚 𝒊=𝟎
𝒗 𝒙𝒊=𝒗 𝒙 𝒇=𝒄 𝒐𝒏𝒔𝒕𝒂𝒏𝒕
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Launching a Cannon ball
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VERTICALLY LAUNCHED PROJECTILES
Horizontal Velocity is constant
Vertical Velocity decreases on the way upward
Vertical Velocity increases on the way down,
NO Vertical Velocity at the top of the trajectory.
Component Magnitude Direction
Horizontal Constant Constant
Vertical Decreases up, Increases down Changes
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VERTICALLY LAUNCHED PROJECTILES
Since the projectile was launched at a angle, the velocity MUST be broken into components!!!
vo
vxi
vyi
q
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PROJECTILE MOTION EQUATIONS
𝐑𝐞𝐜𝐚𝐥𝐥Horizontal (x) Motion
a = ____ Vertical (y) Motion
a = ____
xv
xd
0 g
Constant
tvx
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Time for upward motion + Time for downward motion
T = t1 + t2
TIME OF FLIGHT:
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HORIZONTAL RANGE:
=
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The maximum value of R can be calculated by the following equation. This result makes sense because the maximum value of Sin2θ = 1, which occurs when 2θ = 90°.
HORIZONTAL MAXIMUM RANGE
Therefore, R is maximum when θ = 45°
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MAXIMUM HEIGHT
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Example:A long jumper leaves the ground at an angle of 20.0° above the horizontal and at a speed of 11.0 m/s.How far does he jump in the horizontal direction?
7.94 m
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Example:A long jumper leaves the ground at an angle of 20.0° above the horizontal and at a speed of 11.0 m/s.What is the maximum height reached?
0.722 m
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Quantity Formulae
Horizontal velocity component
Vertical velocity component
Range of Projectile
Height
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Uniform Circular Motion
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Tangential and Radial AccelerationThe tangential acceleration component causes a change in the speed v of the particle. This component is parallel to the instantaneous velocity, and its magnitude is given by
The radial acceleration component arises from a change in direction of the velocity vector and is given by