49
Chapter 2: One-Dimensional Motion Motion at fixed velocity Definition of average velocity Motion with fixed acceleration Graphical representations

Chapter 2: One-Dimensional Motion

Embed Size (px)

DESCRIPTION

Chapter 2: One-Dimensional Motion. Motion at fixed velocity Definition of average velocity Motion with fixed acceleration Graphical representations. Displacement vs. position. Position: x (relative to origin) Displacement: D x = x f -x i. Average velocity. Average velocity. - PowerPoint PPT Presentation

Citation preview

Page 1: Chapter 2: One-Dimensional Motion

Chapter 2: One-Dimensional Motion

•Motion at fixed velocity•Definition of average velocity•Motion with fixed acceleration•Graphical representations

Page 2: Chapter 2: One-Dimensional Motion

Displacement vs. position

Position: x (relative to origin)Displacement: x = xf-xi

Page 3: Chapter 2: One-Dimensional Motion

basic formula

v =xt

=xf −xi

t

Average velocity

Average velocity

•Can be positive or negative•Depends only on initial/final positions•e.g., if you return to original position, average velocity is zero

Page 4: Chapter 2: One-Dimensional Motion

basic formula

v =xt

=xf −xit

Instantaneous velocity

Let time interval approach zero

•Defined for every instance in time•Equals average velocity if v = constant•SPEED is absolute value of velocity

Page 5: Chapter 2: One-Dimensional Motion

Graphical Representation of Average Velocity

Between A and D , v is slope of blue line

Page 6: Chapter 2: One-Dimensional Motion

Graphical Representation of Instantaneous Velocity

v(t=3.0) is slope of tangent (green line)

Page 7: Chapter 2: One-Dimensional Motion

Example 2.1

Carol starts at a position x(t=0) = 1.5 m.At t=2.0 s, Carol’s position is x(t=2 s)=4.5 mAt t=4.0 s, Carol’s position is x(t=4 s)=-2.5 m

a) What is Carol’s average velocity between t=0 and t=2 s?b) What is Carol’s average velocity between t=2 and t=4 s?c) What is Carol’s average velocity between t=0 and t=4 s?

a) 1.5 m/sb) -3.5 m/sc) -1.0 m/s

Page 8: Chapter 2: One-Dimensional Motion

Example 2.2

On a mission to rid Spartan Stadium of vermin, an archer shoots an arrow across the stadium at an unlucky rat 200 meters away. The archer hears the squeal 2.2 seconds later. What was the velocity of the arrow? The speed of sound is 330 m/s.

Page 9: Chapter 2: One-Dimensional Motion

Example 2.2: Visualize the problem!

Page 10: Chapter 2: One-Dimensional Motion

Example 2.2

On a mission to rid Spartan Stadium of vermin, an archer shoots an arrow across the stadium at an unlucky rat 200 meters away. The archer hears the squeal 2.2 seconds later. What was the velocity of the arrow? The speed of sound is 330 m/s.

V = 125 m/s

Page 11: Chapter 2: One-Dimensional Motion

Example 2.3a

The instantaneous velocityis zero at ___

A) aB) b & dC) c & e

Page 12: Chapter 2: One-Dimensional Motion

Example 2.3b

The instantaneous velocity is negative at _____

A) aB) bC) cD) dE) e

Page 13: Chapter 2: One-Dimensional Motion

Example 2.3c

The average velocity is zero in the interval _____ A) a-c

B) b-dC) c-dD) c-eE) d-e

Page 14: Chapter 2: One-Dimensional Motion

Example 2.3d

The average velocity is negative in the interval(s)_________

A) a-b B) a-cC) c-eD) d-e

Page 15: Chapter 2: One-Dimensional Motion

SPEED

• Speed is |v| and is always positive• Average speed is sum over |x| elements divided by elapsed time

Page 16: Chapter 2: One-Dimensional Motion

Example 2.4

2

4

6

8

2 4 6 8 10 1200A

B

C

D

E

a) What is the average velocity between B and E?

b) What is the average speed between B and E?

a) 0.2 m/sb) 1.2 m/s

t (s)

x (m)

Page 17: Chapter 2: One-Dimensional Motion

Acceleration

The rate of change of the velocity

Average acceleration: measured over finite time interval

Instantaneous acceleration: measured over infinitesimal interval, t -

> 0

a =vf −vit

Page 18: Chapter 2: One-Dimensional Motion

Accelerometer Demo

Page 19: Chapter 2: One-Dimensional Motion

Graphical Description of Acceleration

Acceleration is slope oftangent line in v vs. t graph

Page 20: Chapter 2: One-Dimensional Motion

Graphical Description of Acceleration

a > 0

a < 0

a is positive/negativewhen v vs. t is

rising/fallingor when x vs t curves

upwards/downwards

Page 21: Chapter 2: One-Dimensional Motion

Example 2.5a

a

b

cd

e

At which point(s) does the position equal zero?A) a onlyB) a and dC) b onlyD) b & d

Page 22: Chapter 2: One-Dimensional Motion

Example 2.5b

a

b

cd

e

At which point(s) does the velocity equal zero?A) aB) b onlyC) c onlyD) b & dE) a & d

Page 23: Chapter 2: One-Dimensional Motion

Example 2.5c

a

b

cd

e

At which point is the velocity negative?A) aB) bC) cD) dE) e

Page 24: Chapter 2: One-Dimensional Motion

Example 2.5d

a

b

cd

e

At which segment(s) is the acceleration negative?

A) a-cB) c-dC) c-eD) d-e

Page 25: Chapter 2: One-Dimensional Motion

Example 2.5e

a

b

cd

e

At which point(s) does the acceleration equal zero?

A) none of the belowB) bC) cD) dE) e

Page 26: Chapter 2: One-Dimensional Motion

Constant Acceleration

• a vs. t is a constant• v vs t is a straight line• x vs t is a parabola

Eq.s of Motion

v f =v0 +at

x=12(v0 +vf )t

Page 27: Chapter 2: One-Dimensional Motion

Solving Problems with Eq.s of Motion

5 variables: x, t, v0, vf, a

2 equations: v f =v0 +at

x=12(v0 +vf )t

3 variables must be given so that2 equations can solve for 2 unknowns

Page 28: Chapter 2: One-Dimensional Motion

Example 2.6

Crash Houlihan speeds down the intersate, when she slams on the brakes and slides into a concrete barrier. The police measure skid marks to be 60 m long, and from a tape recording, know that she was breaking from 3.5 seconds. Furthermore, they know that her Mercedes would decelerate at 5.5 m/s2 while skidding. What was Crash’s speed when she hit the barrier?

7.52 m/s

Page 29: Chapter 2: One-Dimensional Motion

Other Forms of Eq.s of Motion

x =v0 + (v0 + at)

2t

x = v0t +1

2at2

Substitute to eliminate vf

v f =v0 +at

x=12(v0 +vf )t

Page 30: Chapter 2: One-Dimensional Motion

Other Forms of Eq.s of Motion

x =(v f − at) + v f

2t

x = v f t −1

2at2

Substitute to eliminate v0

v f =v0 +at

x=12(v0 +vf )t

Page 31: Chapter 2: One-Dimensional Motion

Other Forms of Eq.s of Motion

x =(v0 + v f )

2

(v f − v0 )

a

ax=vf2

2−v02

2

Substitute to eliminate t

v f =v0 +at

x=12(v0 +vf )t

Page 32: Chapter 2: One-Dimensional Motion

Final List of 1-d Equations

Which one should I use?Each Eq. has 4 of the 5 variables: x, t, v0, v & aAsk yourself “Which variable am I not given and not interested in?” If that variable is t, use Eq. (5).

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

Page 33: Chapter 2: One-Dimensional Motion

Example 2.6 (Revisited)

Crash Houlihan speeds down the intersate, when she slams on the brakes and slides into a concrete barrier. The police measure skid marks to be 60 m long, and from a tape recording, know that she was breaking from 3.5 seconds. Furthermore, they know that her Mercedes would decelerate at 5.5 m/s2 while skidding. What was Crash’s speed when she hit the barrier?

7.52 m/s

Page 34: Chapter 2: One-Dimensional Motion

Example 2.7aA drag racer starts her car from rest and accelerates at 10.0 m/s2 for the entire distance of a 400 m (1/4 mi) race.How much time was required to finish the race?

a) v =v0 +at

b) x=12(v0 +v)t

c) x=v0t+12at2

d) x=vft−12at2

e) ax=vf2

2−v02

2

Page 35: Chapter 2: One-Dimensional Motion

Example 2.7bA drag racer starts her car from rest and accelerates at 10.0 m/s2 for the entire distance of a 400 m (1/4 mi) race.What was her final speed?

a) v =v0 +at

b) x=12(v0 +v)t

c) x=v0t+12at2

d) x=vft−12at2

e) ax=vf2

2−v02

2

Page 36: Chapter 2: One-Dimensional Motion

Example 2.7cA drag racer starts her car from rest and finishes a race in 3.5 seconds with a constant acceleration for the entire distance of a 400 m (1/4 mi) race.What was her final speed?

a) v =v0 +at

b) x=12(v0 +v)t

c) x=v0t+12at2

d) x=vft−12at2

e) ax=vf2

2−v02

2

Page 37: Chapter 2: One-Dimensional Motion

Free Fall

• Objects under the influence of gravity (no resistance) fall with constant downward acceleration (if near Earth’s surface).

g = 9.81 m/s2

• Use the usual equations with a --> -g

Page 38: Chapter 2: One-Dimensional Motion

•Father was a musician, experimented with music•Initially was a professor teaching pre-meds•Developed telescope ~ 1610:

Milky Way = starsMoons of JupiterPhases of Venus…

•Measured g•Quantified mechanics•In 1632, published Dialogue concerning the two greatest world systems•Was found guilty of heresy

Galileo

Page 39: Chapter 2: One-Dimensional Motion

Example 2.8a

A man drops a brick off the top of a 50-m building. The brick has zero initial velocity.

a) How much time is required for the brick to hit the ground?

b) What is the velocity of thebrick when it hits the ground?

A B

c

a) 3.19 sb) -31.3 m/s

Page 40: Chapter 2: One-Dimensional Motion

Example 2.8b

A man throws a brick upward from the top of a 50 m building. The brick has an initial upward velocity of 20 m/s.

a) How high above the building does the brick get before it falls?

b) How much time does the brick spend going upwards?

c) What is the velocity of the brick when it passes the man going downwards?

d) What is the velocity of the brick when it hits the ground?

e) At what time does the brick hit the ground?

A B

c

Page 41: Chapter 2: One-Dimensional Motion

Example 2.8b

A man throws a brick upward from the top of a 50 m building. The brick has an initial upward velocity of 20 m/s.

a) How high above the building does the brick get before it falls?

b) How much time does the brick spend going upwards?

c) What is the velocity of the brick when it passes the man going downwards?

d) What is the velocity of the brick when it hits the ground?

e) At what time does the brick hit the ground?

a) 20.4 mb) 2.04 sc) -20 m/sd) -37.2 m/se) 5.83 s

Page 42: Chapter 2: One-Dimensional Motion

Example 2.9a

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

At ‘A’ the acceleration is positive

A C

D

A C

D

B

E

a) Trueb) False

Page 43: Chapter 2: One-Dimensional Motion

Example 2.9b

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

At ‘B’ the velocity is zero

A C

D

A C

D

B

E

a) Trueb) False

Page 44: Chapter 2: One-Dimensional Motion

Example 2.9c

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

At ‘B’ the acceleration is zero

A C

D

A C

D

B

E

a) Trueb) False

Page 45: Chapter 2: One-Dimensional Motion

Example 2.9d

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

At ‘C’ the velocity is negative

A C

D

A C

D

B

E

a) Trueb) False

Page 46: Chapter 2: One-Dimensional Motion

Example 2.9e

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

At ‘C’ the acceleration is negative

A C

D

A C

D

B

E

a) Trueb) False

Page 47: Chapter 2: One-Dimensional Motion

Example 2.9f

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

The speed at ‘C’ and at ‘A’ are equal

A C

D

A C

D

B

E

a) Trueb) False

Page 48: Chapter 2: One-Dimensional Motion

Example 2.9g

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

The velocity at ‘C’ and at ‘A’ are equal

A C

D

A C

D

B

E

a) Trueb) False

Page 49: Chapter 2: One-Dimensional Motion

Example 2.9h

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

The speed is greatest at ‘E’

A C

D

A C

D

B

E

a) Trueb) False