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PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3

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Page 1: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

PHYSICS 231

INTRODUCTORY PHYSICS I

PHYSICS 231

INTRODUCTORY PHYSICS I

Lecture 3

Page 2: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

• HW 2 due: Wednesday Jan 23 @ 3:59 am

• (MLK Jr. Day on Jan 21)

• Note: related reading for each lecture listed on Calendar page at PHY 231 website

AnnouncementAnnouncement

Page 3: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Main points of last lecture

• Acceleration defined:

• Equations with constantAcceleration:

(x, v0, vf, a, t)

• Acceleration of freefall:

a =vf −vit

basic equations:

1) v =v0 +at

2) x=12(v0 +v)t

3) x=v0t+12at2

4) x=vft−12at2

5) ax=vf2

2−v02

2

a → (−g) = −9.81m/s2

Page 4: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 2.9a

A man throws a brick upward from the top of a building. (Assume the coordinate system is defined with positive defined as upward)

At what point is the acceleration zero?

A C

D

A C

D

B

E

a) Ab) Bc) Cd) De) None of the above

Page 5: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 2.9b

A man throws a brick upward from the top of a building. (Assume the coordinate system is defined with positive defined as upward)

At what point is the velocity zero?

A C

D

A C

D

B

E

a) Ab) Bc) Cd) De) None of the above

Page 6: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

CHAPTER 3

Two-Dimensional Motion Two-Dimensional Motion and Vectorsand Vectors

Two-Dimensional Motion Two-Dimensional Motion and Vectorsand Vectors

Page 7: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Scalars and Vectors

• Scalars: Magnitude only

• Examples: time, distance, speed,…

• Vectors: Magnitude and Direction

• Examples: displacement, velocity, acceleration,…

Page 8: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Representations:Representations:

x

y

(x, y)

(x, y)

(r, )

Vectors in 2 Dimensions

Vector distinguished byarrow overhead: A

Cartesian Polar

Page 9: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Vector Addition/Subtraction

• 2nd vector begins at end of first vector

• Order doesn’t matter

Vector addition

Vector subtraction

A – B can be interpreted as A+(-B)

• Order does matter

Page 10: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Vector Components

Cartesian components are projections along the x- and y-axes

Ax =Acosθ

Ay = Asinθ

Going backwards,

A = Ax2 + Ay

2 and =tan−1AyAx

Page 11: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.1a

The magnitude of (A-B) is :

a) <0b) =0c) >0

Page 12: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.1b

The x-component of (A-B) is:

a) <0b) =0c) >0

Page 13: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.1c

The y-component of (A-B) > 0

a) <0b) =0c) >0

Page 14: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.2

Some hikers walk due east from the trail head for 5 miles. Then the trail turns sharply to the southwest, and they continue for 2 more miles until they reach a waterfalls. What is the magnitude and direction of the displacement from the start of the trail to the waterfalls?

3.85 miles, at -21.5 degrees

5 mi

2 mi

Page 15: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

2-dim Motion: Velocity

Graphically,

v = r / t

It is a vector(rate of change of position)

Trajectory

Page 16: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Multiplying/Dividing Vectors by Scalars

• Example: v = r / t

• Vector multiplied by scalar is a vector: B = 2A

• Magnitude changes proportionately: |B| = 2|A|

• Direction is unchanged: B = A

B

A

Page 17: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

2-d Motion with constant acceleration

• X- and Y-motion are independent

• Two separate 1-d problems: x, vx, ax

y, vy, ay

• Connected by time t

• Important special case: Projectile motion• ax=0 • ay=-g

Page 18: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Projectile Motion

• X-direction: (ax=0)

• Y-direction: (ay=-g)

Note: we ignore• air resistance• rotation of earth

vx = constant

Δx = vxt

vy, f = vy,0 − gt

Δy = 12 (vy,0 + vy, f )t

Δy = vy,0t − 12 gt 2

Δy = vy, f t + 12 gt 2

−gΔy =vy, f

2

2−

vy,02

2

Page 19: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Projectile Motion

Acceleration is constant

Page 20: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Pop and Drop Demo

The Ballistic Cart Demo

Page 21: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Finding Trajectory, y(x)

1. Write down x(t)

2. Write down y(t)

3. Invert x(t) to find t(x)

4. Insert t(x) into y(t) to get y(x)

Trajectory is parabolic

x =v0,xt

y =v0,yt−12gt2

t =x/ v0,x

y =v0,yv0,x

x−12

gv0,x2 x2

Page 22: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.3

An airplane drops food to two starving hunters. The plane is flying at an altitude of 100 m and with a velocity of 40.0 m/s.

How far ahead of the hunters should the plane release the food?

X181 m

h

v0

Page 23: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.4a

h

D

v0

The Y-component of v at A is :a) <0b) 0c) >0

Page 24: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.4b

h

D

v0

a) <0b) 0c) >0

The Y-component of v at B is

Page 25: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.4c

h

D

v0

a) <0b) 0c) >0

The Y-component of v at C is:

Page 26: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.4d

h

D

v0

a) Ab) Bc) Cd) Equal at all points

The speed is greatest at:

Page 27: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.4e

h

D

v0

a) Ab) Bc) Cd) Equal at all points

The X-component of v is greatest at:

Page 28: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.4f

h

D

v0

a) Ab) Bc) Cd) Equal at all points

The magnitude of the acceleration is greatest at:

Page 29: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Range Formula

• Good for when yf = yi

x =vi,xt

y=vi,yt−12gt2 =0

t=2vi,yg

x=2vi,xvi,y

g=2vi

2 cos sing

x=vi2

gsin2

Page 30: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Range Formula

• Maximum for =45R =vi2

gsin2

Page 31: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.5a

100 m

A softball leaves a bat with an initial velocity of 31.33 m/s. What is the maximum distance one could expect the ball to travel?

Page 32: PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 3. HW 2 due: Wednesday Jan 23 @ 3:59 am (MLK Jr. Day on Jan 21) Note: related reading for each lecture listed

Example 3.6

68 m

A cannon hurls a projectile which hits a target located on a cliff D=500 m away in the horizontal direction. The cannon is pointed 50 degrees above the horizontal and the muzzle velocity is 75 m/s. Find the height h of the cliff?

h

D

v0