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Lecuter #ch#12.2

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Dynamics
Thermodynamics–I
Dr. Ihab Alsurakji
Chapter 12
Kinematics of a Particle
Objectives
o To introduce the concepts of position, displacement, velocity, and acceleration.
o To study particle motion along a straight line.
Areas of Mechanics
Areas of Mechanics
Introduction
• Scalars (e.g.)
• Vectors (e.g.)
– distance
– speed
– mass
– temperature
– pure numbers
– time
– pressure
– area, volume
– charge
– energy
– displacement
– velocity
– acceleration
– force
– weight (force)
– momentum
Vectors
• Can be represented by an arrow (called the “vector”)
• Length of the vector represents the magnitude of the quantity
• Symbols for vectors:
- (e.g. force) 𝐹Ԧ ,or F (bold type)
Distance and Displacement
Distance is a scalar quantity that refers to "how
much ground an object has covered" during its
motion.
Displacement is a vector quantity that refers to
"how far out of place an object is"; it is the
object's overall change in position.
7 m = Distance
5 m = Displacement
Distance and Displacement
Distance
Displacement
➒ Total length of path travelled ➒ Direct distance
➒ Must be greater than (or ➒ Shortest distance between
equal to) magnitude of
two points
displacement
➒ Distance between start and
➒ Only equal if path is straight
finish points
➒ Symbol “d “
➒ Can describe with only one
direction
➒ Symbol “s”
𝑠 = π‘₯π‘“π‘–π‘›π‘Žπ‘™ − π‘₯π‘–π‘›π‘–π‘‘π‘–π‘Žπ‘™
7 m = Distance
5 m = Displacement
Average Speed and Average Velocity
π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’ 𝑑
π΄π‘£π‘’π‘Ÿπ‘Žπ‘”π‘’ 𝑆𝑝𝑒𝑒𝑑 =
=
π‘‘π‘–π‘šπ‘’
𝑑
π‘‘π‘–π‘ π‘π‘™π‘Žπ‘π‘’π‘šπ‘’π‘›π‘‘ 𝑠
π΄π‘£π‘’π‘Ÿπ‘Žπ‘”π‘’ π‘‰π‘’π‘™π‘œπ‘π‘–π‘‘π‘¦ =
=
π‘‘π‘–π‘šπ‘’
𝑑
𝑠 βˆ†π‘₯ π‘₯ − π‘₯π‘œ
𝑣= =
=
𝑑
𝑑
𝑑
Section 12.2 : Rectilinear Kinematics
❖Rectilinear : Straight line motion
❖Kinematics : Study the geometry of the motion dealing with s, v, a.
❖Rectilinear Kinematics : To identify at any given instant, the particle’s
position, velocity, and acceleration.
All objects such as rockets, projectiles, or vehicles will be considered as
particles “has negligible size and shape”
Particles : has mass but negligible size and shape
Velocity & Speed
βœ“ Speed : Distance per unit time
βœ“ Average speed :
𝑆𝑇 𝑑 (Always positive scalar )
𝑣𝑠𝑝 π‘Žπ‘£π‘” =
=
βˆ†π‘‘ 𝑑
βœ“ Velocity: displacement per unit time
βœ“ Average velocity :
βˆ†π‘ 
π‘£π‘Žπ‘£π‘” =
βˆ†π‘‘
𝑑𝑠
βœ“ Instantaneous velocity :
𝑣=
𝑑𝑑
Acceleration
βœ“ Acceleration : The rate of change in velocity (π‘šΤ𝑠 2 )
βˆ†π‘½ = 𝑉 ′ − 𝑉
βœ“ Average Acceleration:
βˆ†π‘½
π’‚π‘Žπ‘£π‘” =
βˆ†π‘‘
βœ“ Instantaneous acceleration :
βˆ†π‘£ 𝑑𝑣 𝑑 2 𝑠
𝒂 = lim
=
= 2
βˆ†π‘‘→0 βˆ†π‘‘
𝑑𝑑 𝑑𝑑
• If 𝑉 ′ > 𝑉 “Acceleration”
• If 𝑉 ′ < 𝑉 “Deceleration”
Relation involving s, v, and a
βœ“ Position “s”
𝑑𝑠
𝒗=
𝑑𝑑
𝑑𝑠
→ 𝑑𝑑 = 𝒗
𝑑𝑠 𝑑𝑣
=
𝒗
𝒂
βœ“ Velocity “v”
βœ“ Acceleration “a”
𝑑𝑣
𝒂=
𝑑𝑑
𝑑𝑣
→ 𝑑𝑑 =
𝒂
𝒂𝑑𝑠 = 𝒗𝑑𝑣
For Constant Acceleration
π’Ž
𝒇𝒕
𝒂 = 𝒂𝒄 = −πŸ—. πŸ–πŸ 𝟐 = πŸ‘πŸ. 𝟐 𝟐
𝒔
𝒔
Constant Acceleration
v
t
 dv =  a dt
c
vo
o
s
t
 ds =  v dt
so
yields
v = vo + act
yields
s = s o + v ot + (1/2)a ct 2
o
v
s
vo
so
 v dv =  a c ds yields
v2 = (vo )2 + 2ac(s - so)
Velocity as a Function of Time
𝑑𝑣
𝒂π‘ͺ =
𝑑𝑑
𝑑𝑣 = 𝒂π‘ͺ 𝑑𝑑
𝑣
𝑣 = π‘£π‘œ + 𝒂π‘ͺ 𝑑
𝑑
ΰΆ± 𝑑𝑣 = ΰΆ± 𝒂π‘ͺ 𝑑𝑑
𝑣𝑂
0
so and vo are the initial position and velocity at t = 0.
Position as a Function of Time
𝑑𝑠
𝑣=
= π‘£π‘œ + 𝒂π‘ͺ 𝑑
𝑑𝑑
𝑠
𝑑
ΰΆ± 𝑑𝑠 = ΰΆ± π‘£π‘œ + 𝒂π‘ͺ 𝑑 𝑑𝑑
𝑠𝑂
0
𝟏
𝟐
𝑠 = π‘ π‘œ + π‘£π‘œ 𝑑 + 𝒂π‘ͺ 𝒕
𝟐
so and vo are the initial position and velocity at t = 0.
Velocity as a Function of Position
𝒗𝑑𝑣 = 𝒂𝒄 𝑑𝑠
𝑣
𝑠
ΰΆ± 𝒗𝑑𝑣 = ΰΆ± 𝒂𝒄 𝑑𝑠
𝑣𝑂
𝑠𝑂
1 2 1 2
𝑣 − π‘£π‘œ = π‘Žπ‘ 𝑠 − π‘ π‘œ
2
2
2
2
𝑣 = π‘£π‘œ + 2π‘Žπ‘ 𝑠 − π‘ π‘œ
so and vo are the initial position and velocity at t = 0.
Example # 1
A particle moves along a straight line such that its position is defined by
𝑠 = 𝑑 3 − 3𝑑 2 + 2 m
Determine the velocity of the particle when t = 4 s.
Ans. v = 24 m/s.
Example # 2
A motorcyclist travels along a straight road at a speed of 27 m/s. When the
brakes are applied, the motorcycle decelerates at a rate of -6t m/s2. The distance
the motorcycle travels before it stops.
Ans. s = 54 m
Example # 3
A car moves in a straight line such that for a short time its velocity is defined by
v = 3𝑑 2 + 2𝑑
ft/s, where t is in seconds. Determine its position and
acceleration when t = 3 s. When t = 0, s = o.
Ans.
s = 36 m
a= 20 m/s2
Example # 4
A car starts from rest and moves along a straight line with an acceleration of a =
(3𝑠 −1/3 ) m/s2. where s is in meters. Determine the car’s acceleration when t = 4
sec.
Ans.
a= 1.06 m/s2
Example # 5
Ball A is released from rest at a height of 12m at the same
time that ball B is thrown upward, 1.5m from the ground.
The balls pass one another at a height of 6m. Find the speed
at which ball B was thrown upward.
Ans.
t= 1.106 sec
v= 9.5 m/s
Example # 6
Ali and Omar are standing at the top of a cliff of height “H”. Both throw a ball
with initial speed π‘£π‘œ , Ali straight down and Omar straight up. The speed of the
balls when they hit the ground are 𝑣𝐴𝐿 and 𝑣𝑂𝑀 respectively. Which of the
following is true:
a) 𝑣𝐴𝐿 < 𝑣𝑂𝑀
b) 𝑣𝐴𝐿 = 𝑣𝑂𝑀
c) 𝑣𝐴𝐿 > 𝑣𝑂𝑀
Summary
Time dependent Acceleration
Constant Acceleration
𝑠(𝑑)
𝑑𝑠
𝑣=
𝑑𝑑
𝑣 = π‘£π‘œ + π‘ŽπΆ 𝑑
1
𝑠 = π‘ π‘œ + π‘£π‘œ 𝑑 + π‘ŽπΆ 𝑑 2
2
𝑑𝑣 𝑑 2 𝑠
π‘Ž=
= 2
𝑑𝑑 𝑑𝑑
𝑣 2 = π‘£π‘œ2 + 2π‘Žπ‘ 𝑠 − π‘ π‘œ
π‘Žπ‘‘π‘  = 𝑣𝑑𝑣
This applies to a freely falling object:
a = g = 9.81 m/sec2 = 32.2 ft/sec2
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