Mechanics Lecture 2, Slide 1 Vectors and 2d-Kinematics Continued Comments on Homework Summary of...

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Mechanics Lecture 2, Slide 1 Vectors and 2d-Kinematics Continued Comments on Homework Summary of Vectors and 2-d Kinematics Homework Solutions

Transcript of Mechanics Lecture 2, Slide 1 Vectors and 2d-Kinematics Continued Comments on Homework Summary of...

Mechanics Lecture 2, Slide 1

Vectors and 2d-KinematicsContinued

Comments on Homework Summary of Vectors and 2-d Kinematics Homework Solutions

Homework Results Vectors and 2-d kinematics

Mechanics Lecture 1, Slide 2

Average=87%No attempt = 14

Awesome Job!

See Me or TAs

Homework 1 results

Mechanics Lecture 1, Slide 3

Average=62.5%

Among those who made an attemptAverage=74.7%

Great Suggestions for Success

Mechanics Lecture 1, Slide 4

Questions/Suggestions

Mechanics Lecture 1, Slide 5

22

2

r

MG

mr

MmG

m

Fag

r

MmGF

m

FamaF

g

g

2

26

2421311

2 /8.91037.6

1097.51067.6 sm

m

kgskgm

R

MGg earth

Each component can be treated separately. Remember that they are component of a vector

Kinematic equations for displacement,velocity and acceleration are the source for the derived equations .

For this situation the horizontal component of the velocity remains constant. The vertical component of velocity changes due to the gravitational acceleration.

Mechanics Lecture 2, Slide 6

Vectors and 2d-kinematics – Main Points

Mechanics Lecture 2, Slide 7

Vectors and 2d-kinematics – Main Points

Vectors and 2d-kinematics Fundamental Equations

Mechanics Lecture 2, Slide 8

Source of Projectile Trajectory Equations

Mechanics Lecture 1, Slide 9

Horizontal Vertical Boring

Ballistic Projectile Motion Quantities

Mechanics Lecture 2, Slide 14

Initial velocityspeed,angle

Maximum Height of trajectory, h=ymax

Range of trajectory, D

Height of trajectory at arbitrary x,t

“Hang Time”Time of Flight, tf

Derived Projectile Trajectory Equations

Mechanics Lecture 1, Slide 15

2

000 cos2

1

cossin)(

v

xg

v

xvxy

200 2

1)( gttvyty y

Height of trajectory as f(x), y(x)

Height of trajectory as f(t) , y(t)

g

vD

2sin20

g

v

g

vt y

f

sin2200

g

vyh

2

sin220

0

Range of trajectory

Time of Flight (“Hang Time”)

Maximum height

Homework Solutions-Baseball

Mechanics Lecture 1, Slide 16

Homework Solutions-Baseball

Mechanics Lecture 1, Slide 17

Homework Hints- Baseball Stadium Wall

Mechanics Lecture 1, Slide 18

Homework Hints – Stadium Wall

Mechanics Lecture 1, Slide 19

Calculate time to reach wall using vx:

cos// 00 vxvxt wallwallwall x

Calculate y position at time to reach wall:

200

20000

200

cos/2

1tan

cos/2

1cos/sin

2

1

vxgxyy

vxgvxvyy

tgtvyy

wallwallwall

wallwallwall

wallwallwall y

Homework Solutions-Baseball Stadium

Mechanics Lecture 1, Slide 20

200

20000

200

00

cos/2

1tan

cos/2

1cos/sin

2

1

cos//

vxgxyy

vxgvxvyy

tgtvyy

vxvxt

wallwallwall

wallwallwall

wallwallwall

wallwallwall

y

x

ftftftfty

sftftsftftfty

vxgxyy

ysftgftx

wall

wall

wallwallwall

37.15124.24761.3953

)8192.0/176/565)/1.16()7002)(.565(3

cos/2

1tan

0;/2.32;35;565

22

200

020

Homework Hints-Catch

Mechanics Lecture 1, Slide 21

Homework Hints-Catch

Mechanics Lecture 1, Slide 22

cos00 vvx

sin00 vvx

g

vy

g

vyy y

2

sin

2

)( 20

0

20

0max

g

v

g

vvtvx

g

vt

tvtgtgtv

tgtvyyyy

yx

x

y

yy

y

ff

f

ffff

ffff

sincos22

22

1;

2

10

2

1;

200

0

0

022

0

2000

0

Homework Hints-Catch

Mechanics Lecture 1, Slide 23

20000

0000

0

max1

0

max

/2

1/

cos;sin

)(cos;

)(cos

xjuliejuliejulie vxgvxvyy

vvvv

v

yyv

v

yyv

xy

xy

max2

0max0

20

20

20

max00max2

0

2

cossin

cos;2sin

yyvyygv

vvv

yyvvyygv

Homework Solutions-Catch

Mechanics Lecture 1, Slide 24

20000

0000

0

max1

0

max

/2

1/

cos;sin

)(cos;

)(cos

xjuliejuliejulie vxgvxvyy

vvvv

v

yyv

v

yyv

xy

xy

max2

0max0

20

20

20

max00max2

0

2

cossin

cos;2sin

yyvyygv

vvv

yyvvyygv

Homework Solutions-Catch

Mechanics Lecture 1, Slide 25

smsmvvx

/92.13)35)(cos/17(cos00

smsmvvy

/75.9)5736)(./17(sin00

m

sm

smm

g

vy

g

vyy y 34.6

)/81.9(2

/75.95.1

2

sin

2

)(2

220

0

20

0max

smyyvyygv /92.192 max2

0max0

mg

vvtvx yx

x ff 67.272 00

0

Homework Solutions-Catch

Mechanics Lecture 1, Slide 26

mmmmy

smmsmsmmsmmy

vxgvxvyy

julie

julie

xjuliejuliejulie xy

40.599.1290.165.1

)/17(/67.27)/81.9(2

1)/17(/67.27)/38.10(5.1

/2

1/

22

20000

smsmvv

smsm

y/38.10/92.195215.0sin

5215.0)8534.0(1sin

41.318534.0cos;8534.0/92.19//17cos

00

2

01

Homework Hints-Catch 2

Mechanics Lecture 1, Slide 27

Homework Hints-Catch 2

Mechanics Lecture 1, Slide 28

cos0vvx vVx is constant !

g

vgvtgvttv y

yy ffy

0

00

2)(

g

vt

tvtgtgtv

y

yy

f

ffff

0

022

0

22

1;

2

10

Kinetic energy should be same as when ball was thrown. Y-component of velocity would be downward.

Homework Hints-Catch 2

Mechanics Lecture 1, Slide 29

g

vvtvx yx

x ff

00

0

2

julie

julie

t

xv

x0

Same conditions as before

max2

0max0 2 yyvyygv

20000 /2

1/ xjuliejuliejulie vxgvxvyy

xy

Homework Hints – Soccer Kick & Cannonball

Mechanics Lecture 1, Slide 30

Homework Hints – Soccer Kick & Cannonball

Mechanics Lecture 1, Slide 31

20

200 yx

vvv

x

y

v

v

0

01tan

g

vyy y

2

)( 20

0max

g

vD

2sin2

0

g

vvtvx yx

x ff

00

0

2

Homework Hints – Soccer Kick & Cannonball

Mechanics Lecture 1, Slide 32

)()(

)(;)(

220

00

givenyxgiven

givenxgivengiveny

ttvvttv

vttvtgvttvxy

200 2

1givengivengiven tgtvytty

y

Homework Solutions-Catch

Mechanics Lecture 1, Slide 33

Homework Hints-Catch

Mechanics Lecture 1, Slide 34

cos00 vvx

sin00 vvx

g

vy

g

vyy y

2

sin

2

)( 20

0

20

0max

g

v

g

vvtvx

g

vt

tvtgtgtv

tgtvyyyy

yx

x

y

yy

y

ff

f

ffff

ffff

sincos22

22

1;

2

10

2

1;

200

0

0

022

0

2000

0

Homework Hints-Catch 2

Mechanics Lecture 1, Slide 35

Homework Solutions-Catch 2

Mechanics Lecture 1, Slide 36

smsmvvx /92.13)35)(cos/17(cos0 vVx is constant !

smssmsmttv

vg

vgvtgvttv

fy

ffy y

y

yy

/75.9)9878.1)(/81.9(/75.9)(

2)(

2

0

0

00

ssm

sm

g

vt

tvtgtgtv

y

yy

f

ffff

988.1/81.9

)/75.9(222

1;

2

10

2

0

022

0

Kinetic energy should be same as when ball was thrown. Y-component of velocity would be downward.

Homework Solutions-Catch 2

Mechanics Lecture 1, Slide 37

mg

vvtvx yx

x ff 67.272 00

0

smsm

m

t

xv

julie

julie

x/17

/628.1

67.270 Same conditions as before

smyyvyygv /92.192 max2

0max0

mmmmy

smmsmsmmsmmy

vxgvxvyy

julie

julie

xjuliejuliejulie xy

40.599.1290.165.1

)/17(/67.27)/81.9(2

1)/17(/67.27)/38.10(5.1

/2

1/

22

20000

Homework Hints – soccer kick

Mechanics Lecture 1, Slide 38

Homework Solutions– soccer kick

Mechanics Lecture 1, Slide 39

smsmsmvvvyx

/213.21/15/15 2220

200

01

0

01 451tantan

x

y

v

v

m

sm

smm

g

vyy y 47.11

)/81.9(2

/150

2

)(2

220

0max

m

sm

smsm

g

vvtvx yx

x ff 87.45)/81.9(

/15/15222

00

0

m

sm

smsm

g

vD 87.45

)/81.9(

/15/15)2sin(2

20

Homework Solutions – soccer kick

Mechanics Lecture 1, Slide 40

smstv

smsmstvstvstv

smssmsmsgvstv

yx

y y

/06.17)7.0(

)/13.8()/15()7.0()7.0()7.0(

/133.8)7.0)(/81.9(/157.0)7.0(

2222

20

mssmssmmsty

sgsvystyy

097.87.0/81.92

17.0/1507.0

7.02

17.07.0

22

200

Homework Solutions - Cannonball

Mechanics Lecture 1, Slide 41

Cannonball Solutions

Mechanics Lecture 1, Slide 42

smsmsmvvvyx

/566.43/23/37 2220

200

01

0

01 87.3137

23tantan

x

y

v

v

m

sm

smm

g

vyy y 96.26

)/81.9(2

/230

2

)(2

220

0max

m

sm

sm

g

vD 51.173

/81.9

)87.31(2sin/566.432sin2

022

0

Cannonball- Solutions

Mechanics Lecture 1, Slide 43

smstv

smsmstvstvstv

vstvsmssmsmsgvstv

yx

xy xy

/28.39)0.1(

)/19.13()/37()0.1()0.1()0.1(

)0.1(;/19.13)0.1)(/81.9(/230.1)0.1(

2222

02

0

mssmssmmsty

sgsvystyy

09.180.1/81.92

10.1/2300.1

0.12

10.10.1

22

200

Mechanics Lecture 2, Slide 44

Vectors and 2d-kinematics – Main Points

Mechanics Lecture 2, Slide 45

Time spend in the air depends on the maximum height

Maximum height depends on the initial vertical velocity

vtrain car

Trigonometric Identity for range equation

Mechanics Lecture 2, Slide 46

)2sin(2

1)sin()sin(

2

1cossin

)sin()sin(2

1cossin

222

1cossin

4cossin

422cossin

2cos

2sin

)()()()(

)()()()(

i

ee

i

ee

i

eeee

i

eeeeeeeeee

i

ee

ee

i

ee

iiii

iiii

iiiiiiiiiiii

ii

ii

http://mathworld.wolfram.com/Cosine.html http://mathworld.wolfram.com/Sine.html

Trigonometric Identities relating sum and products

Mechanics Lecture 2, Slide 47

List of trigonometric identities

cossin2sincoscossin)2sin(

sincoscossin)sin(

Hyperphysics-Trajectories

Mechanics Lecture 1, Slide 48

http://hyperphysics.phy-astr.gsu.edu/hbase/traj.html