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University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul http://zitompul.wordpress.com 2013

University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul 2013

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Page 1: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

University Physics: Mechanics

Ch4. TWO- AND THREE-DIMENSIONAL MOTION

Lecture 4

Dr.-Ing. Erwin Sitompulhttp://zitompul.wordpress.com

2013

Page 2: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/2Erwin Sitompul University Physics: Mechanics

Solution of Homework 3: The Beetles

Starting point

1st run, 0.5 m

2nd run, 0.8 m

1st r

un, 1

.6 m

2nd run, ?

New location

30

40

Page 3: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/3Erwin Sitompul University Physics: Mechanics

Thus, the second run of the green beetle corresponds to the vector

Solution of Homework 3: The Beetles

New location

Starting point

A

B

CD

30

40

ˆ ˆ ˆ0.5i (0.8cos30 i 0.8sin 30 j)A B

ˆ ˆ1.19i 0.4 j

ˆ ˆ1.6cos50 i 1.6sin 50 jC

ˆ ˆ1.03i 1.23j

A B C D

D A B C

ˆ ˆ ˆ ˆ(1.19i 0.4 j) (1.03i 1.23j) ˆ ˆ0.16i 0.83j

ˆ ˆ0.16i 0.83j m.D ��������������

Page 4: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/4Erwin Sitompul University Physics: Mechanics

Solution of Homework 3: The Beetles

(a) The magnitude of the second run?

(b) The direction of the second run?

ˆ ˆ0.16i 0.83j mD

2 2(0.16) ( 0.83)D

0.85 m

1 0.83tan

0.16

79.09

N

E

S

W

D→

79.09

0.85 m

The direction of the second run is 79.09° south of due east or 10.91° east of due south.

Page 5: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/5Erwin Sitompul University Physics: Mechanics

Moving in Two and Three Dimensions In this chapter we extends the material of the preceding

chapters to two and three dimensions. Position, velocity, and acceleration are again used, but they

are now a little more complex because of the extra dimensions.

Page 6: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/6Erwin Sitompul University Physics: Mechanics

Position and Displacement One general way of locating a particle is with a position

vector r,ˆ ˆ ˆi j kr x y z

The coefficients x, z, and y give the particle’s location along the coordinate axes and relative to the origin.

The following figure shows a particle with position vectorˆ ˆ ˆ( 3 m)i (2 m) j (5 m)kr

In rectangular coordinates, the position is given by (–3 m, 2 m, 5 m).

Page 7: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/7Erwin Sitompul University Physics: Mechanics

Position and Displacement As a particle moves, its position vector changes in a way that

the vector always extends from the origin to the particle. If the position vector changes from r1 to r2, then the particle’s

displacement delta is:

2 1r r r

2 2 2 1 1 1ˆ ˆ ˆ ˆ ˆ ˆ( i j k) ( i j k)r x y z x y z

2 1 2 1 2 1ˆ ˆ ˆ( )i ( )j ( )kr x x y y z z

ˆ ˆ ˆi j kr x y z

→ →

Page 8: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/8Erwin Sitompul University Physics: Mechanics

Average Velocity and Instantaneous Velocity If a particle moves through a displacement Δr in a time

interval Δt, then its average velocity vavg is:

displacement

average velocitytime interval

avg

rv

t

The equation above can be rewritten in vector components as:

avg

ˆ ˆ ˆi j kx y zv

t

ˆ ˆ ˆi j kx y z

t t t

Page 9: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/9Erwin Sitompul University Physics: Mechanics

The particle’s instantaneous velocity v is the velocity of the particle at some instant.

The direction of instantaneous velocity of a particle is always tangent to the particle’s path at the particle’s position.

Average Velocity and Instantaneous Velocity

drv

dt

Page 10: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/10Erwin Sitompul University Physics: Mechanics

Average Velocity and Instantaneous Velocity Writing the last equation in unit-vector form:

This equation can be simplified by rewriting it as:ˆ ˆ ˆi j kx y zv v v v

where the scalar components of v are:

,x

dxv

dt ,y

dyv

dt z

dzv

dt

The next figure shows a velocity vector v and its scalar x and y components. Note that v is tangent to the particle’s path at the particle’s position.

ˆ ˆ ˆ( i j k)d

v x y zdt

ˆ ˆ ˆi j k

dx dy dz

dt dt dt

Page 11: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/11Erwin Sitompul University Physics: Mechanics

The figure below shows a circular path taken by a particle. If the instantaneous velocity of the particle at a certain time is v = 2i – 2j m/s, through which quadrant is the particle currently moving when it is traveling(a) clockwise(b) counterclockwise

(a) clockwise (b) counterclockwise

Firstquadrant

Thirdquadrant

vy

vx

–2

2

ˆ ˆ2 2 m sv i j

Average Velocity and Instantaneous Velocity

^ ^→

Page 12: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/12Erwin Sitompul University Physics: Mechanics

When a particle’s velocity changes from v1 to v2 in a time interval Δt, its average acceleration aavg during Δt is:

change in velocityaverage

acceleration time interval

2 1avg

v va

t

v

t

If we shrink Δt to zero, then aavg approaches the instantaneous acceleration a ; that is:

dva

dt

ˆ ˆ ˆ( i j k)x y z

dv v v

dt ˆ ˆ ˆi j kyx z

dvdv dv

dt dt dt

Average and Instantaneous Acceleration→ →

Page 13: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/13Erwin Sitompul University Physics: Mechanics

We can rewrite the last equation asˆ ˆ ˆi j kx y za a a a

where the scalar components of a are:

,xx

dva

dt ,yy

dva

dt z

z

dva

dt

Acceleration of a particle does not have to point along the path of the particle

Average and Instantaneous Acceleration

Page 14: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/14Erwin Sitompul University Physics: Mechanics

A particle with velocity v0 = –2i + 4j m/s at t = 0 undergoes a constant acceleration a of magnitude a = 3 m/s2 at an angle 130° from the positive direction of the x axis. What is the particle’s velocity v at t = 5 s?

Solution:0x x xv v a t 0y y yv v a t

0 2 m sxv 0 4 m syv 3 cos130xa 3 sin130ya

21.928 m s 22.298 m s

2 ( 1.928)(5)xv 11.64 m s

4 (2.298)(5)yv 15.49 m s

Thus, the particle’s velocity at t = 5 s is

ˆ ˆ11.64i 15.49j m s.v

Average and Instantaneous Acceleration^→

^→

At t = 5 s,

Page 15: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/15Erwin Sitompul University Physics: Mechanics

Homework 4: The PlaneA plane flies 483 km west from city A to city B in 45 min and then 966 km south from city B to city C in 1.5 h. From the total trip of the plane, determine:(a) the magnitude of its displacement;(b) the direction of its displacement;(c) the magnitude of its average velocity;(d) the direction of its average velocity;(e) its average speed.

Page 16: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/16Erwin Sitompul University Physics: Mechanics

Homework 4A: The TurtleA turtle starts moving from its original position with the speed 10 cm/s in the direction 25° north of due east for 1 minute. Afterwards, it continues to move south for 2 m in 8 s. From the total movement of the turtle, determine:(a) the magnitude of its displacement;(b) the direction of its displacement;(c) the magnitude of its average velocity;(d) the direction of its average velocity;(e) its average speed.

Page 17: University Physics: Mechanics Ch4. TWO- AND THREE-DIMENSIONAL MOTION Lecture 4 Dr.-Ing. Erwin Sitompul  2013

4/17Erwin Sitompul University Physics: Mechanics

Homework 4B: Shopping Trip1. A shopper at a supermarket follows the path indicated by vectors S, H, O,

and P in the figure. Given that the vectors have magnitudes S = 51 ft, H = 45 ft, O = 35 ft, and P = 13 ft. For all his movement, the shopper requires 8.5 min. Find:

→ → →

(a) the magnitude of his displacement;(b) the direction of his displacement;(c) the magnitude of his average velocity;(d) the direction of his average velocity;(e) his average speed.

2. Compute A + B + C and express the result in magnitude-angle notation (polar coordinate).

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