Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time...

22
Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9

Transcript of Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time...

Page 1: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

• Non-constant Force – spring intro. continued• Constant force – gravitation (near Earth)• Time estimates for collisions

Section 2.7-2.9

Page 2: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Q 2.2 bThree carts are moving on three tracks. Which cart(s) experience a net force to the left? A. Green Cart which moves to the left at constant speed. B. Red Cart which moves to the left, gradually speeding up.C. Blue Cart which moves to the left, gradually slowing down.D. Both Green and Red cartsE. Both Blue and Red cartsF. Both Green and Blue carts

Dp = F Dt

Page 3: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Smoothly-Varying Force: Spring

LskskF ssspˆ

Page 4: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Q 2.5 cA spring is 12 cm (0.12 m) long when relaxed. Its stiffness is 30 N/m. You stretch the spring so its length is now 20 cm (0.20 m). What is the magnitude of the force you exert on the spring?a) 0.24 Nb) 0.24 Nmc) 2.4 Nd) 2.4 Nme) 24 Nf) 24 Nm

Page 5: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Experiment: Observe Motion

Compute: Simulate Motion (with force and momentum visualized)

Analytical: (for a later chapter) build and solve ‘equations of motion.’

while t < tmax:

ttt

tm

prr

tFpp

rLrkF

object

objectobjectobject

objectnetobjectobject

eqobjectsobjectnet

ˆ*

Three ways to Explore

Page 6: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

2.6 Constant Force –near-Earth gravitation

Page 7: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

A ball is initially on the ground, and you kick it with initial velocity < 3,7,0> m/s. At this speed air resistance is negligible. Assume the usual coordinate system. Which component(s) of the ball's momentum will change in the next half second (after the ball’s left your foot)?

a) px

b) py

c) pz

d) px & py

e) py & pz

f) pz & px

g) px, py, & pz

Page 8: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

The initial momentum of the ball was < 1.5, 3.5, 0 > kg*m/s. The final momentum of the ball is < 1.5, 1.05, 0 > kg*m/s. Therefore...

1 2 3

4 5 6

Q2.6.c: Which graph correctly shows py for the ball during this 0.5 s?

Page 9: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

You throw a ball so that just after it leaves your hand at location it has velocity . Now that it has left your hand, (and we’re neglecting air resistance) the net force all the time is . What are the velocity and position of the ball after time Dt?

0,, iii yxr

0,, yixii vvv

00 ,,. mgFF gEnet

system: Ball (b)y

x0,, ii yxr

i

0,, yixii vvv

0,,0. gmgmF gE

0airF

?fr

?fv

Apply the Momentum Principle

Page 10: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

tgvvyvvx

tgvv

yiyfxixf

if

:ˆ:ˆ

system: Ball (b)y

x0,, ii yxr

i

0,, yixii vvv

0,,0. mgF gE

0airF

?fr

?fv

Apply the Momentum Principle

Apply Position Update

Page 11: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

tgvvyvvx

tgvv

yiyfxixf

if

:ˆ:ˆ

system: Ball (b)y

x0,, ii yxr

i

0,, yixii vvv

0,,0. mgF gE

0airF

?fr

?fv

Apply the Momentum Principle

Apply Position Update 221 tgtvrr iif

221 tgtvyyytvxxx iyifixif :ˆ:ˆ

Page 12: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

v x (ho

rizon

tal)

tgvvyvvx

tgvv

yiyfxixf

if

:ˆ:ˆ

system: Ball (b)y

x0,, ii yxr

i

0,, yixii vvv

0,,0. mgF gE

0airF

?fr

?fv

Apply the Momentum Principle

Apply Position Update 221 tgtvrr iif

tvxx ixif

Graphical Representations

t (time)x (h

orizo

ntal

)

221 tgtvyyytvxxx iyifixif :ˆ:ˆ

221 tgtvyy iyif

Y (vertical)

t (time)

vY (vertical)

xixf vv tgvv yiyf

Page 13: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Example: If you throw a ball horizontally off of a 10-m high cliff at 5 m/s, how far from the base of the cliff will it hit the ground? How fast will it be going when it hits?

tgvvyvvx

tgvv

yiyfxixf

if

:ˆ:ˆ

system: Ball (b)y

x0,, ii yxr

i

0,, yixii vvv

0,,0. mgF gE

0airF

?fr

?fv

Apply the Momentum Principle

Apply Position Update 221 tgtvrr iif

221 tgtvyyytvxxx iyifixif :ˆ:ˆ

Page 14: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.
Page 15: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

tgvvyvvx

tgvv

yiyfxixf

if

:ˆ:ˆ

system: Ball (b)y

x0,, ii yxr

i

0,, yixii vvv

0,,0. mgF gE

0airF

?fr

?fv

Apply the Momentum Principle

Apply Position Update 221 tgtvrr iif

221 tgtvyyytvxxx iyifixif :ˆ:ˆ

Example: At the start of a football game, the kickoff has an initial speed of 22 m/s at 40° above horizontal.

a) How long does the ball stay in the air?

b) How far away does the ball hit the ground?

c) What is the maximum height that the ball reaches?

Page 16: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.
Page 17: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Exercise: You have probably seen a basketball player throw the ball to a teammate at the other end of the court, 30 m away.

a) Estimate a reasonable initial angle for such a throw, and then determine the corresponding initial speed.

b) For your chosen angle, how long does it take for the ball to go the length of the court?

c) What is the highest point along the trajectory, relative to the thrower’s hand?

tgvvyvvx

tgvv

yiyfxixf

if

:ˆ:ˆ

system: Ball (b)y

x0,, ii yxr

i

0,, yixii vvv

0,,0. mgF gE

0airF

?fr

?fv

Apply the Momentum Principle

Apply Position Update 221 tgtvrr iif

221 tgtvyyytvxxx iyifixif :ˆ:ˆ

Page 18: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.
Page 19: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Example of Estimating collision forceSay a 2200 kg truck, going 25m/s, hits a brick wall and comes to a dead stop. In the process, the truck’s hood crumples back 0.8 m. Estimate the magnitude of the average force of the collision.

smvi /25

kgmt 2200

POW!

?. wtaveF

mr 8.0

0fv t

vmF

t

vvmF

t

pF

itwtavg

if

twtavg

wtavg

.

.

.

0

avgv

rt

?t

22iif

avg

vvvv

0

iv

rt

2

r

vmF itwtavg

2

2

.

NF

m

smkgF

wtavg

wtavg

6.

2

2

.

101.1

8.02

/252200

Page 20: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

A 5-kg lead ball is dropped from rest at a height of 10 m. The ball leaves a 5 cm deep dent in the ground.a) How fast is the ball traveling just before hitting the ground?

b) What is the approximate force exerted by the ground on the ball while it is stopping?

Page 21: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.
Page 22: Non-constant Force – spring intro. continued Constant force – gravitation (near Earth) Time estimates for collisions Section 2.7-2.9.

Fri. 2.6 – .8 Constant Force, time estimates, Models RE 2.c

Mon. Tues

3.1 – .5, .14-.15 Fundamental Forces, Gravitation

RE 3.aEP 2, HW2: Ch 2 Pr’s 40, 57, 63, 67 & CP