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Physics I Lecture03-Motion in one dimension-I η°‘η΄‹ζΏ± εœ‹η«‹δΊ€ι€šε€§ε­Έ 理學陒 電子物理系

Physics I Lecture03-Motion in one dimension-I

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Physics ILecture03-Motion in one dimension-Iη°‘η΄‹ζΏ±εœ‹η«‹δΊ€ι€šε€§ε­Έη†ε­Έι™’ι›»ε­η‰©η†η³»

CONTENTS

1. Position, Velocity and Speed

2. Instantaneous Velocity and Speed

3. Motion with Constant Velocity

4. Acceleration

5. Motion Diagram

6. Motion with Constant Acceleration

7. Freely Falling Object

8. Kinmatic Equations & Calculus

1. POSITION, VELOCITY AND SPEED

Scalar: real number π‘₯, Vector: real number with direction

π‘₯ Ƹ𝑖, where the number is just the length of the vector

Position – a vector to note the direction and distance from the origin

0 1 2 3 4βˆ’1βˆ’2βˆ’3

ොπ‘₯

3ොπ‘₯ or 3 ΖΈπ‘–βˆ’1.2ොπ‘₯ or βˆ’ 1.2 Ƹ𝑖

Displacement – a vector, variation of the position

Notation - βˆ† Τ¦π‘₯ = Τ¦π‘₯𝑓 βˆ’ Τ¦π‘₯𝑖, where Τ¦π‘₯𝑖and Τ¦π‘₯𝑓 are initial and final position

βˆ† Τ¦π‘₯ = Τ¦π‘₯𝑓 βˆ’ Τ¦π‘₯𝑖 = 4.2 Ƹ𝑖 βˆ’ 10 Ƹ𝑖 = βˆ’5.8 Ƹ𝑖

Example: The initial position of an object is Τ¦π‘₯𝑖 = 10 Ƹ𝑖 and its final position is Τ¦π‘₯𝑓 = 4.2 Ƹ𝑖.

What is the displacement?

1. POSITION, VELOCITY AND SPEED

Distance – a scalar corresponding to the displacement

Notation - βˆ† Τ¦π‘₯ = Τ¦π‘₯𝑓 βˆ’ Τ¦π‘₯𝑖

βˆ† Τ¦π‘₯ = Τ¦π‘₯𝑓 βˆ’ Τ¦π‘₯𝑖 = 4.2 Ƹ𝑖 βˆ’ 10 Ƹ𝑖 = βˆ’5.8 Ƹ𝑖 = 5.8

average Velocity – a vector, The displacement divides by the period of time.

Notation - Τ¦π‘£π‘Žπ‘£π‘” =Τ¦π‘₯π‘“βˆ’ Τ¦π‘₯𝑖

βˆ†π‘‘

average Speed – a scalar, different from the average velocity.

Notation - π‘£π‘Žπ‘£π‘” =π‘‘π‘œπ‘‘π‘Žπ‘™ π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’ π‘‘π‘Ÿπ‘Žπ‘£π‘’π‘™π‘’π‘‘

βˆ†π‘‘

Example: The initial position of an object is Τ¦π‘₯𝑖 = 10 Ƹ𝑖 and its final position is Τ¦π‘₯𝑓 = 4.2 Ƹ𝑖.

What is the distance of its movement?

1. POSITION, VELOCITY AND SPEED

0 10 20 30 40βˆ’10βˆ’20βˆ’30

ොπ‘₯

0 𝑠10 𝑠20 𝑠30 𝑠40 𝑠50 𝑠

-40

-30

-20

-10

0

10

20

30

40

50

0 10 20 30 40 50 60

x (

m)

time (s)

t x

0 25

10 40

20 30

30 0

40 -20

50 -30

average velocity between t=0 and t=50:

Τ¦π‘£π‘Žπ‘£π‘” =Τ¦π‘₯ 50 βˆ’ Τ¦π‘₯ 0

50=

βˆ’30 ΖΈπ‘–βˆ’25 Ƹ𝑖

50= βˆ’

55

50Ƹ𝑖 (m/s)

average speed between t=0 and t=50:

π‘£π‘Žπ‘£π‘” =40βˆ’25 +(40βˆ’(βˆ’30))

50=

85

50(m/s)

1. POSITION, VELOCITY AND SPEED

Displacement: βˆ† Τ¦π‘₯ = Τ¦π‘₯𝑓 βˆ’ Τ¦π‘₯𝑖 = 2 βˆ’ 12 Ƹ𝑖 = βˆ’10 Ƹ𝑖 (m)

Distance: βˆ† Τ¦π‘₯ = βˆ’10 Ƹ𝑖 = 10 (n)

average Velocity: Τ¦π‘£π‘Žπ‘£π‘” = ΰ΅—βˆ† Τ¦π‘₯βˆ†π‘‘ =

βˆ’10 Ƹ𝑖

4βˆ’1= βˆ’

10

3Ƹ𝑖 (m/s)

Example: A particle is moving along the x-axis. Its initial position is Τ¦π‘₯𝑖 = 12 Ƹ𝑖 (m) at

time 𝑑𝑖 = 1 (s) and its final position is Τ¦π‘₯𝑓 = 2 Ƹ𝑖 (m) at time 𝑑𝑓 = 4 (s). Find out its

displacement and average velocity during the time interval.

2. INSTANTANEOUS VELOCITY AND SPEED

Velocity – a vector, The infinitesimal displacement divides by the

infinitesimal period of time.

Notation - Ԧ𝑣 = limβˆ†π‘‘β†’0

Τ¦π‘₯π‘“βˆ’ Τ¦π‘₯𝑖

βˆ†π‘‘= lim

βˆ†π‘‘β†’0

π‘₯ 𝑑𝑓 βˆ’π‘₯ 𝑑𝑖

βˆ†π‘‘ΖΈπ‘– = lim

βˆ†π‘‘β†’0

π‘₯ 𝑑+βˆ†π‘‘ βˆ’π‘₯ 𝑑

βˆ†π‘‘ΖΈπ‘–

Speed – a scalar, The norm of the average velocity.

Notation - 𝑣 = Ԧ𝑣 =𝑑π‘₯ 𝑑

𝑑𝑑Ƹ𝑖 =

𝑑π‘₯ 𝑑

𝑑𝑑

=𝑑π‘₯ 𝑑

𝑑𝑑Ƹ𝑖

http://588ku.com/image/qicheyibiaoban.html

2. INSTANTANEOUS VELOCITY AND SPEED

The velocity: Ԧ𝑣 𝑑 = limβˆ†π‘‘β†’0

Τ¦π‘₯ 𝑑+βˆ†π‘‘ βˆ’ Τ¦π‘₯ 𝑑

βˆ†π‘‘

= limβˆ†π‘‘β†’0

3 𝑑+βˆ†π‘‘ 2+2 𝑑+βˆ†π‘‘ βˆ’ 3𝑑2+2𝑑

βˆ†π‘‘ΖΈπ‘– = 6𝑑 + 2 Ƹ𝑖 (m/s)

The average velocity: Τ¦π‘£π‘Žπ‘£π‘” 𝑑 =Τ¦π‘₯ 3 βˆ’ Τ¦π‘₯ 1

3βˆ’1=

33βˆ’5

2Ƹ𝑖 = 14 Ƹ𝑖 (m/s)

Compared with Ԧ𝑣 1 = 8 Ƹ𝑖 (m/s), Ԧ𝑣 2 = 14 Ƹ𝑖 (m/s),

Ԧ𝑣 3 = 20 Ƹ𝑖 (m/s)

Example: The position of an object moving on the x-axis varies in time according to

the equation Τ¦π‘₯ 𝑑 = 3𝑑2 + 2𝑑 Ƹ𝑖, where π‘₯ is in meters and 𝑑 is in seconds. (a) Find the

velocity as a function of time. (b) Find the average velocity in the intervals between

𝑑 = 1 and 𝑑 = 3 s.

3. MOTION WITH CONSTANT VELOCITY

Object in constant velocity motion, its instantaneous velocity is Ԧ𝑣 𝑑 = 𝑣0 Ƹ𝑖. As you

know the velocity, you can find out its position as a function of time by integration with a specified constant of Τ¦π‘₯ 𝑑 = 0 = Τ¦π‘₯ 0 = Τ¦π‘₯0.

Ԧ𝑣 𝑑 = 𝑣0 Ƹ𝑖

𝑑 Τ¦π‘₯ 𝑑

𝑑𝑑= Ԧ𝑣 𝑑 = 𝑣0 Ƹ𝑖 𝑑 Τ¦π‘₯ 𝑑 = 𝑣0𝑑𝑑 Ƹ𝑖

ࢱ𝑑 Τ¦π‘₯ 𝑑 = ࢱ𝑣0𝑑𝑑 Ƹ𝑖 ΰΆ±Τ¦π‘₯0

Τ¦π‘₯ 𝑑

𝑑 Τ¦π‘₯ 𝑑′ = ΰΆ±0

𝑑

𝑣0𝑑 𝑑′ Ƹ𝑖

Τ¦π‘₯ 𝑑 = Τ¦π‘₯0 + 𝑣0𝑑 Ƹ𝑖

Τ¦π‘₯ 𝑑 βˆ’ Τ¦π‘₯0𝑑 βˆ’ 0

= Τ¦π‘£π‘Žπ‘£π‘” = 𝑣0 Ƹ𝑖 Τ¦π‘₯ 𝑑 βˆ’ Τ¦π‘₯0 = 𝑣0𝑑 Ƹ𝑖 Τ¦π‘₯ 𝑑 = Τ¦π‘₯0 + 𝑣0𝑑 Ƹ𝑖

3. MOTION WITH CONSTANT VELOCITY

𝑑 Τ¦π‘₯ 𝑑

𝑑𝑑= Ԧ𝑣 𝑑 = 5.0 Ƹ𝑖

ΰΆ±10 Ƹ𝑖

Τ¦π‘₯ 𝑑

𝑑 Τ¦π‘₯ = Ƹ𝑖 ΰΆ±2.0

𝑑

5.0𝑑𝑑

Τ¦π‘₯ 𝑑 = 10 + 5.0 𝑑 βˆ’ 2.0 Ƹ𝑖 = 5.0𝑑 Ƹ𝑖 (m)

Τ¦π‘₯ 10 = 50 Ƹ𝑖 (m)

Example: A particle moves with a constant velocity Ԧ𝑣 𝑑 = 5.0 Ƹ𝑖 (m/s).

The position is Τ¦π‘₯ 2.0 = 10 Ƹ𝑖 (m) at 𝑑 = 2.0 (s).

(a) Please find the position as a function of time.

(b) Please find its position at 𝑑 = 10 (s).

4. ACCELERATION

average Acceleration – a vector, The velocity variation

divides by the period of time.

Notation - Τ¦π‘Žπ‘Žπ‘£π‘” =π‘£π‘“βˆ’π‘£π‘–

βˆ†π‘‘

Acceleration – a vector, The infinitesimal velocity variation divides by

the infinitesimal period of time.

Notation - Τ¦π‘Ž = limβˆ†π‘‘β†’0

π‘£π‘“βˆ’π‘£π‘–

βˆ†π‘‘= lim

βˆ†π‘‘β†’0

𝑣 𝑑𝑓 βˆ’π‘£ 𝑑𝑖

βˆ†π‘‘= lim

βˆ†π‘‘β†’0

𝑣 𝑑+βˆ†π‘‘ βˆ’π‘£ 𝑑

βˆ†π‘‘

Derivation - Τ¦π‘Ž =𝑑𝑣 𝑑

𝑑𝑑=

𝑑2 Τ¦π‘₯ 𝑑

𝑑𝑑2

Ԧ𝑣 𝑑 = 3𝑑2 βˆ’ 27 Ƹ𝑖 (m/s)

Τ¦π‘Ž 𝑑 = 6𝑑 Ƹ𝑖 (m/s2)

Example: A particle moves according to the expression Τ¦π‘₯ 𝑑 = 4 βˆ’ 27𝑑 + 𝑑3 Ƹ𝑖, where π‘₯ is in

meters and 𝑑 is in seconds. Please find its velocity and acceleration as a function of time.

4. ACCELERATION

https://www.pdhpe.net/the-body-in-motion/how-do-biomechanical-principles-influence-movement/motion/acceleration/

Τ¦π‘Ž =𝑑 Ԧ𝑣 𝑑

𝑑𝑑=𝑑2 Τ¦π‘₯ 𝑑

𝑑𝑑2

CONTENTS

1. Position, Velocity and Speed

2. Instantaneous Velocity and Speed

3. Motion with Constant Velocity

4. Acceleration

5. Motion Diagram

6. Motion with Constant Acceleration

7. Freely Falling Object

8. Kinmatic Equations & Calculus

5. MOTION DIAGRAM

car at rest

car in motion with constant velocity

car in motion with constant acceleration

car in motion with constant deceleration

https://giphy.com/gifs/dog-cartoons-UKm1AF0UrCkb6

6. MOTION WITH CONSTANT ACCELERATIONObject in constant acceleration motion, its instantaneous acceleration is Τ¦π‘Ž 𝑑 = π‘Ž0 Ƹ𝑖. As you know the acceleration, you can find out its velocity and position as a function of time

by integration with two specified constants of

Τ¦π‘₯ 𝑑 = 0 = Τ¦π‘₯ 0 = Τ¦π‘₯0 and Ԧ𝑣 𝑑 = 0 = Ԧ𝑣 0 = Ԧ𝑣0 = 𝑣0 Ƹ𝑖.

Τ¦π‘Ž 𝑑 = π‘Ž0 Ƹ𝑖 = Τ¦π‘Žπ‘Žπ‘£π‘” =Ԧ𝑣 𝑑 βˆ’ Ԧ𝑣0𝑑 βˆ’ 0

Ԧ𝑣 𝑑 βˆ’ Ԧ𝑣0 = π‘Ž0𝑑 Ƹ𝑖

Ԧ𝑣 𝑑 = Ԧ𝑣0 + π‘Ž0𝑑 Ƹ𝑖 = 𝑣0 Ƹ𝑖 + π‘Ž0𝑑 Ƹ𝑖

𝑑𝑣 𝑑

𝑑𝑑= π‘Ž0 Ƹ𝑖 𝑑 Ԧ𝑣 = π‘Ž0 Ƹ𝑖𝑑𝑑 ΰΆ±

𝑣0

𝑣 𝑑

𝑑 Ԧ𝑣 = ΰΆ±0

𝑑

π‘Ž0 Ƹ𝑖𝑑𝑑′

Ԧ𝑣 𝑣0

𝑣 𝑑= π‘Ž0 Ƹ𝑖 𝑑

β€²0𝑑 Ԧ𝑣 𝑑 βˆ’ Ԧ𝑣0 = π‘Ž0𝑑 Ƹ𝑖 Ԧ𝑣 𝑑 = Ԧ𝑣0 + π‘Ž0𝑑 Ƹ𝑖

6. MOTION WITH CONSTANT ACCELERATIONObject in constant acceleration motion, its instantaneous acceleration

is Τ¦π‘Ž 𝑑 = π‘Ž0 Ƹ𝑖. As you know the acceleration, you can find out its velocity

and position as a function of time by integration with two specified

constants of Τ¦π‘₯ 𝑑 = 0 = Τ¦π‘₯ 0 = Τ¦π‘₯0 and Ԧ𝑣 𝑑 = 0 = Ԧ𝑣 0 = Ԧ𝑣0 = 𝑣0 Ƹ𝑖.

Ԧ𝑣 𝑑 = 𝑣0 Ƹ𝑖 + π‘Ž0𝑑 Ƹ𝑖

t

v

𝑑0

𝑣 𝑑 = 𝑣0 + π‘Ž0𝑑

𝑣0

𝑣0 + π‘Ž0𝑑0

Ԧ𝑣 0 = 𝑣0 Ƹ𝑖, Ԧ𝑣 𝑑0 = 𝑣0 Ƹ𝑖 + π‘Ž0𝑑0 Ƹ𝑖

The area in v-t graph:

π‘₯ 𝑑0 βˆ’ π‘₯ 0 =𝑣0 + 𝑣0 + π‘Ž0𝑑0

2𝑑0 = 𝑣0𝑑0 +

π‘Ž0𝑑02

2

π‘₯ 𝑑 = π‘₯0 + 𝑣0𝑑 +π‘Ž0𝑑

2

2

Τ¦π‘₯ 𝑑 = Τ¦π‘₯0 + 𝑣0𝑑 Ƹ𝑖 +π‘Ž0𝑑

2

2Ƹ𝑖

6. MOTION WITH CONSTANT ACCELERATIONObject in constant acceleration motion, its instantaneous acceleration

is Τ¦π‘Ž 𝑑 = π‘Ž0 Ƹ𝑖. As you know the acceleration, you can find out its velocity

and position as a function of time by integration with two specified

constants of Τ¦π‘₯ 𝑑 = 0 = Τ¦π‘₯ 0 = Τ¦π‘₯0 and Ԧ𝑣 𝑑 = 0 = Ԧ𝑣 0 = Ԧ𝑣0 = 𝑣0 Ƹ𝑖.

𝑑 Τ¦π‘₯

𝑑𝑑= Ԧ𝑣 𝑑 = 𝑣0 Ƹ𝑖 + π‘Ž0𝑑 Ƹ𝑖 𝑑 Τ¦π‘₯ = 𝑣0 + π‘Ž0𝑑 𝑑𝑑 Ƹ𝑖

ΰΆ±Τ¦π‘₯0

Τ¦π‘₯ 𝑑

𝑑 Τ¦π‘₯ = ΰΆ±0

𝑑

𝑣0 + π‘Ž0𝑑 𝑑𝑑 Ƹ𝑖

Τ¦π‘₯ 𝑑 = Τ¦π‘₯0 + 𝑣0𝑑 Ƹ𝑖 +π‘Ž0𝑑

2

2Ƹ𝑖

6. MOTION WITH CONSTANT ACCELERATION

Three Equations:Τ¦π‘₯ = Τ¦π‘₯0 + 𝑣0𝑑 Ƹ𝑖 +

π‘Ž0𝑑2

2Ƹ𝑖

Ԧ𝑣 = 𝑣0 Ƹ𝑖 + π‘Ž0𝑑 Ƹ𝑖 1st equation

2nd equation

Ԧ𝑣 βˆ’ 𝑣0 Ƹ𝑖 = π‘Ž0𝑑 Ƹ𝑖

Τ¦π‘₯ βˆ’ Τ¦π‘₯0 = 𝑣0𝑑 Ƹ𝑖 +π‘Ž0𝑑 Ƹ𝑖

2𝑑 Τ¦π‘₯ βˆ’ Τ¦π‘₯0 π‘Ž0 Ƹ𝑖 = 𝑣0 Ƹ𝑖 βˆ™ π‘Ž0𝑑 Ƹ𝑖 +

π‘Ž0𝑑 Ƹ𝑖

2βˆ™ π‘Ž0𝑑 Ƹ𝑖

βˆ† Τ¦π‘₯ βˆ™ Τ¦π‘Ž = 𝑣0 Ƹ𝑖 βˆ™ 𝑣 Ƹ𝑖 βˆ’ 𝑣0 Ƹ𝑖 +1

2𝑣 Ƹ𝑖 βˆ’ 𝑣0 Ƹ𝑖 βˆ™ 𝑣 Ƹ𝑖 βˆ’ 𝑣0 Ƹ𝑖

𝑣2 = 𝑣02 + 2 Τ¦π‘Ž βˆ™ βˆ† Τ¦π‘₯ 3rd equation

𝑣2 = 𝑣02 + 2π‘Žπ‘ 

6. MOTION WITH CONSTANT ACCELERATION

𝑣𝑖 = 108π‘˜π‘š

β„ŽΓ—

1000π‘š

1π‘˜π‘šΓ—

1β„Ž

3600𝑠= 30 (m/s)

𝑣𝑓 = 72π‘˜π‘š

β„ŽΓ—

1000π‘š

1π‘˜π‘šΓ—

1β„Ž

3600𝑠= 20 (m/s)

𝑠 =100 (m)

pick up the right equation: 𝑣𝑓2 = 𝑣0

2 + 2π‘Žπ‘ 

400 = 900 + 2π‘Ž Γ— 100 π‘Ž = βˆ’2.5 (m/s2)

pick up the right equation: 𝑣𝑓 = 𝑣0 + π‘Žπ‘‘

20 = 30 βˆ’ 2.5 Γ— 𝑑 𝑑 = 4 (s)

Example: You start to brake your car from a speed of 108 to 72 km/h when spotting a police car.

The traveled distance is 100 m. Assume that the car is in constant acceleration motion, please

calculate its acceleration and the time required for the decrease in speed.

6. MOTION WITH CONSTANT ACCELERATION

𝑣𝑖 = 3 Γ— 104 (m/s)

𝑣𝑓 = 5 Γ— 106 (m/s)

𝑠 = 2 (cm) = 21π‘š

100π‘π‘š= 0.02 (m)

pick up the right equation: 𝑣𝑓2 = 𝑣0

2 + 2π‘Žπ‘ 

2.5 Γ— 1013 = 9 Γ— 108 + 2π‘Ž Γ— 0.02 π‘Ž β‰… 2.5 Γ—1013

0.04= 6.25 Γ— 1014 (m/s2)

pick up the right equation: 𝑣𝑓 = 𝑣0 + π‘Žπ‘‘

5 Γ— 106 = 3 Γ— 104 + 6.25 Γ— 1014 Γ— 𝑑 𝑑 β‰… 8 Γ— 10βˆ’9 (s)

Example: An electron in the cathode-ray tube of a television set enters a region in which it

accelerates uniformly in a straight line from a speed of 3 Γ— 104 m/s to a speed of 5 Γ— 106 m/s in

a distance of 2 cm. How long is the electron in constant acceleration?

6. MOTION WITH CONSTANT ACCELERATION

45 Γ— 2 + 45𝑑 =5

2𝑑2

Example: A mortorcycle traveling at a constant speed of 45 m/s passes a trooper on a car hidden

behind a billboard. 2 second after the speeding mortorcycle passes the billboard, the trooper sets

out from the billboard to catch the mortorcycle, accelerating at a constant rate of 5.00 m/s2.

How long does it take her to overtake the mortorcycle?

t

v𝑣 𝑑 = π‘Ž0𝑑 , π‘Ž0=5

v=45

t=2

https://giphy.com/gifs/drive-fast-adrenaline-14hVD0HODUPY08

7. FREELY FALLING OBJECT

𝑑 = 0𝑑 = 1

𝑑 = 2

𝑑 = 3

𝑑 = 4

t y(t) (m) vy(t) (m/s) a(t) (m/s2)

0 0 0 -9.8

1 -4.9 -9.8 -9.8

2 -19.6 -19.6 -9.8

3 -44.1 -29.4 -9.8

4 -78.4 -39.2 -9.8

-100 -9.8

https://media.giphy.com/media/cXqQCO1bWp5tK/giphy.mp4

7. FREELY FALLING OBJECT

t y(t) (m) vy(t) (m/s) a(t) (m/s2)

0 -19.6 19.6 -9.8

1 -4.9 9.8 -9.8

2 0 0 -9.8

3 -4.9 -9.8 -9.8

4 -19.6 -19.6 -9.8

5 -44.1 -29.4 -9.8

6 -78.4 -39.2 -9.8

-100 -9.8

8. KINEMATIC EQUATIONS & CALCULUS

𝑑

𝑣 𝑑

𝑑1 𝑑2 𝑑3 𝑑4 𝑑5 𝑑6 𝑑7 𝑑8

βˆ†π‘‘2 βˆ†π‘‘4

𝑣 𝑑6

π‘₯ = limβˆ†π‘‘π‘›β†’0

𝑛=1

π‘š

𝑣 𝑑𝑛 βˆ†π‘‘π‘›

π‘₯ π‘‘π‘š βˆ’ π‘₯ 0 = ΰΆ±0

π‘‘π‘š

𝑣 𝑑 𝑑𝑑

ACKNOWLEDGEMENT

εœ‹η«‹δΊ€ι€šε€§ε­Έη†ε­Έι™’

θ‡ͺδΈ»ζ„›ε­ΈηΏ’θ¨ˆη•«

γ€η§‘ζŠ€ιƒ¨θ£œεŠ©γ€‘