Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

Embed Size (px)

Citation preview

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    1/9

    11/17/2011

    1

    Two-Dimensional

    Motion and Vectors

    Scalars and Vectors

    In Physics, quantities are described as eitherscalar quantities or vector

    quantities .

    A scalar quantityhas only a magnitude (numbers and units) but no

    direction.

    A vector quantityhas both a magnitude and a direction.

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    2/9

    11/17/2011

    2

    Which of the follow are vectors?

    distance

    displacement

    mass

    weight

    temperature

    velocity

    acceleration

    No

    Yes

    No

    Yes

    No

    Yes

    Yes

    Vectors...

    There are two common ways of indicating that

    something is a vector quantity:

    Boldface notation:AA

    Arrow notation:

    AA =

    AA

    AA

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    3/9

    11/17/2011

    3

    January 10, 2011 Physics 114A - Lecture 5 5/26

    The Components of a VectorThe Components of a VectorLength, angle, and components can be

    calculated from each other using trigonometry:

    cosxA A q= sinyA A q=

    2 2

    x yA A A= +

    1tan /y xA Aq

    -=

    January 10, 2011 Physics 114A - Lecture 5 6/26

    2D Cartesian and Polar Coordinate Representations2D Cartesian and Polar Coordinate Representations

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    4/9

    11/17/2011

    4

    Vector addition:

    The sum of two vectors is another vector.

    A = B + C

    B

    C A

    B

    C

    Vector subtraction:

    Vector subtraction can be defined in

    terms of addition.B - C

    B

    C

    B

    -C

    B - C

    = B + (-1)C

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    5/9

    11/17/2011

    5

    Unit Vectors:

    A Unit VectorUnit Vector is a vectorhaving length 1 and no units.

    It is used to specify adirection.

    Unit vector uu points in thedirection ofUU.

    Often denoted with ahat: uu =

    UU

    x

    y

    z

    ii

    jj

    kk

    l Useful examples are the cartesianunit vectors [ ii, j, k, j, k]

    point in the direction of thex, yand zaxes.

    R = rxi + ryj + rzk

    Vector addition using components:

    l Consider CC=AA + BB.

    (a) CC = (Axii+ Ayjj) + (Bxii+ Byjj) = (Ax+ Bx)ii+

    (Ay+ By)jj

    (b) CC = (Cxii+ Cyjj)

    l Comparing components of(a) and (b):

    Cx= Ax+ Bx

    Cy= Ay+ ByCC

    BxAA

    ByBB

    Ax

    Ay

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    6/9

    11/17/2011

    6

    l Vector A = {0,2,1}

    l Vector B = {3,0,2}

    l Vector C = {1,-4,2}

    What is the resultant vector, D, fromadding A+B+C?

    (a)(a) {{33,,--44,,22}} (b)(b) {{44,,--22,,55}} (c)(c) {{55,,--22,,44}}

    Example

    D = (AXi+ AYj+ AZk) + (BXi+ BYj+ BZk) + (CXi+ CYj+ CZk)

    = (AX + BX + CX)i+ (AY + BY+ CY)j+ (AZ + BZ + CZ)k

    = (0 + 3 + 1)i+ (2 + 0 - 4)j+ (1 + 2 + 2)k

    = {4,-2,5}

    January 10, 2011 Physics 114A - Lecture 5 12/26

    Multiplying VectorsMultiplying Vectors

    x y z

    x y z

    A A i A j A k

    B B i B j B k

    = + +

    = + +

    r

    r

    x x y y z z

    AB

    A B A B A B A B

    A B Cosq

    = + +

    =

    r r

    Dot Product (Scalar Product)

    Cross Product (Vector Product)

    ( )

    ( )

    ( )

    ( )

    y z z y

    z x x z

    x y y x

    AB

    x y z

    x y z

    A B A B A B i

    A B A B j

    A B A B k

    A B Sin a b

    i j k

    A A A

    B B B

    q

    = -

    + -

    + -

    =

    =

    r r

    (determinant)

    Given two vectors:

    Note that , ,

    and .

    A B A A B B

    A B B A

    ^ ^

    r r rr r

    r rr r

    AB is the magnitude of Btimes the projection of Aon B (or vice versa).

    Note that AB = BA

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    7/9

    11/17/2011

    7

    Describing Position in 3-Space A vector is used to establish the position of a particle of

    interest. The position vector, r, locates the particle at some

    point in time.

    January 11, 2011 Physics 114A - Lecture 6 14/2414/24

    The Displacement Vector

    r xx yy= +r

    2 1r r rD = -r r r

    2 1

    2 2 1 1 ( ) ( )

    r r r

    x x y y x x y y

    xx y y

    D = -

    = + - +

    = D + D

    r r r

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    8/9

    11/17/2011

    8

    Instantaneous Velocity in 3D

    V = lim (r / t) as t 0 = dr / dt 3 Components : Vx = dx / dt, etc

    Magnitude,

    |V| = SQRT( Vx2 + Vy

    2 + Vz2)

    Average Velocity in 3-D

    Vavg = (r2 r1)/(t2-t1)

    = r / t

    t is scalar so, V vector

    parallel to vector

  • 8/2/2019 Lecture-4 (Dr. M Fadhali).Ppt [Compatibility Mode]2slides

    9/9

    11/17/2011

    9

    Properties of VectorsProperties of Vectors

    January 10, 2011 Physics 114A - Lecture 5 18/26

    The Components of a VectorThe Components of a VectorWe can resolve vector into perpendicular components using

    two-dimensional coordinate systems:

    Polar Coordinates Cartesian Coordinates

    cos25.0 (1.50 m)(0.906) 1.36 mxr r= = =

    sin25.0 (1.50 m)(0.423) 0.634 my

    r r= = =

    2 2 2 2 2(1.36 m) (0.634 m) 2.25 m 1.50 mx yr r r= + = + = =

    [ ]1 1tan (0.634 m) / (1.36 m) tan (0.466) 25.0q - -= = =