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    for Engineers & Scientists

    Ohanian & Markert

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    Preliminary Concepts

    Physicsthe study of matter (and/or energy?)

    Scientific notation: Earth Radius: 6.4 x 106 m

    Earth Sun distance: 1.5 x 1011 m

    Speed of light: 3.0 x 108 m

    Diameter of atom: 1.0 x 10-10 m

    Diameter of proton: 2.0 x 10-15 m

    When working with scientific figures, round the result

    in order to match the least precise figure. What to measure? Position, time and mass (well leave

    electric charges & temperature for later) Idealparticles

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    Position & Time

    Coordinates: needed in order to specify theposition of a particle Establish the origin point

    Grid lines: rectangular coordinates

    Two-dimensional grids; three-dimensional grids; n-dimensional grids

    In order to describe motion, we need the positionof the particle, and the time at which it had that

    position Coordinate grid + array of synchronized timing

    devices reference frame (position + time)

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    Units are needed

    in order to record measurements of

    position, time, and mass.

    The Metric system of units (also called the

    International System of Units):

    Length: the meter

    Time: the second

    Mass: the kilogram

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    Multiples and submultiples

    Kilo 103

    Mega 106

    Giga

    109

    Tera 1012

    Peta 1015

    Exa 1018

    Zetta 1021

    mili 10-3

    micro 10-6

    nano 10

    -9

    pico 10-12

    femto 10-15

    atto 10-18

    zepto 10-21

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    The Unit of Length

    Originally, the standard METER was a platinum-iridium alloy bar, kept in France. The distancebetween scratch marks located near both ends ofthe bar, was defined as a meter.

    It was chosen so that it would be the 1/107 partof the quarter of the polar circunference of theEarth.

    Nowadays, the length of the meter is defined in

    terms of the speed of light; it is the lengthtraveled by a light wave in vacuum in a timeinterval of 1 / 299,792,458 of a second.

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    Other prefixes and unit systems Angstrom = 1 x 10-10 m (Anders Jonas Angstrom, Sweden,

    1814-1874) 1 Astronomical Unit = 1.496 x 1011 m (distance from the

    Earth to the Sun)

    1 parsec (pc) = distance at which 1AU subtends an angle ofone second of an arc (about 3.26 light years, prove it)

    1 light-year = distance that light travels in a year British system of units:

    Foot = 0.3048 meters

    Mile = 5,280 feet = 1,609.38 m

    Nautical Mile = 1.151 miles or 1852 m Yard = 3 feet = 0.9144 m

    Inch = 1/12 feet = 2.54 cm

    Mil = 0.001 inch

    http://commons.wikimedia.org/wiki/File:A%C3%85ngstr%C3%B6m.jpg
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    Needing help with the parsec numbers?

    Parsec: distance

    corresponding to a

    parallax of one

    second

    Parallax:

    Displacement or

    difference in the

    apparent position

    of an object viewed

    along two different

    lines of sight

    http://en.wikipedia.org/wiki/File:Stellarparallax_parsec1.svg
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    The Unit of Time

    The SECOND was originally defined as

    1 / (60x60x24) or 1/86,400 of a mean solar

    day (one complete rotation of the Earth)

    Nowadays, the second is defined as the time

    needed for 9,192 million vibrations of a

    cesium atom (Cesium clocks are really cool!)

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    Time Intervals

    Age of the Universe 4.0 x 1017 s

    Age of the Solar System 1.4 x 1017 s

    Age of oldest fossil

    1.1 x 1017

    s Age of human species 7.9 x 1012 s

    From Sun to Earth 5.0 x 102 s

    From Moon to Earth 1.3 x 100 s Sound wave 3.8 x 10-3 s

    http://en.wikipedia.org/wiki/File:Metric_seal.svg
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    The Unit of Mass

    The KILOGRAM standard is a cylinder of an alloycomposed of platinum and iridium, kept in France.

    Up until now, we still dont have an atomic standard formass.

    Avogadros number: 6.02214 x 1023 atoms (ormolecules) per mole, and the atomic mass of achemical element

    Common Atomic Masses: 12grams for Carbon, 1g for

    Hydrogen, 16g for Oxygen Atomic mass unit: 1 u = Mass of a Carbon-12 atom / 12

    1 u = 1.66 x 10-27 Kg

    http://en.wikipedia.org/wiki/File:Metric_seal.svghttp://en.wikipedia.org/wiki/File:Metric_seal.svghttp://commons.wikimedia.org/wiki/File:Avogadro_Amedeo.jpg
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    Other Units

    1 avoirdupois pound = 0.45359 Kg

    1 ounce = 1/16 pound = 28.35 g

    1 Metric Ton = 103 Kg

    1 Ton (1,000 lb) = 907 Kg

    1 troy pound = 0.82286 avoirdupois pound

    1 troy pound = 12 troy ounces

    1 troy ounce = ( 192 / 175 ) * avoirdupoisounce

    http://commons.wikimedia.org/wiki/File:Avogadro_Amedeo.jpg
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    Derived Units

    Base units: the meter, the second, and the

    kilogram

    Derived units are constructed by a

    combination of the base units.

    Area (meters squared); volume (meters

    cubed)

    Density (Kg / meters3)

    Speed (meters / seg)

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    Warm-up Exercises

    Conversion of Units

    Always check unit consistency

    Ratios of two quantities with identical dimension

    or units will have no dimensions at all; they arecalled dimensionless quantities.

    Basic trigonometrical functions of the righttriangle; law of sines; law of cosines

    Basic algebra: equation systems, quadraticequations

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    Lets solve

    Page 22, Nos. 13 15

    Page 23

    Nos. 26 & 27

    Nos. 36 38

    Page 25, Nos. 68 & 69

    And for homework: Group 1 odd numbers between 70 & 84

    Group 2 even numbers between 69 & 83

    i

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    Just in case.

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    Chapter 3: Vectors

    Displacement of a particle: a change of itsposition

    The arrow drawn from an initial point P1 to a

    final point P2 is called the displacement vector. A displacement vector is defined by its length

    and direction.

    Velocity, acceleration, and force are vectors.

    Length, time, mass, temperature, and energyare scalars.

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    Operations involving vectors Vector addition: two displacements carried out in

    succession, result in a net displacement, which isregarded as the vector sum of the individualdisplacements.

    The sum of two vectors is called the resultantof thesevectors. Visual technique: triangle or parallelogram.

    The Commutative Law applies to vector addition The magnitude of the resultant of two vectors Is

    usually less than the sum of the magnitudes of thevectors.

    The negative of a given vector A is a vector of thesame magnitude, but opposite direction.

    The subtraction of two vectors A and B is defined asthe sum of A andB.

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    Lets go 3-D

    In space, the vector is the diagonal

    of the box formed.

    The position vector and other vectors are expressed interms of unit vectors: i (used for the x axis) j (used for the y axis)

    k (used for the z axis)

    The magnitude of the unit vectors is (of course) 1.

    Vectors expressed in terms of unit vectors: A = 2i + 3j 2k

    A = (2 ; 3 ; -2)

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    The Position Vector

    Any point in a plane can be specified by tworectangular coordinatesxand y, and thedisplacement vector from the origin to the point.

    The displacement vector joining the origin to anygiven point is called theposition vector.

    x and y are the components of the positionvector, and they will be represented with Ax andAy.

    The addition or subtraction of two vectors can beperformed by adding or subtracting theircomponents.

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    Vector Multiplication

    Dot Product: also called the scalar product, is theproduct of the magnitudes of the two vectors andthe cosine of the angle between them.

    Notation: A . B = |A|*|B|*Cos(A,B)

    When will it be positive, negative or cero?

    A . B = AxBx + AyBy + AzBz+

    The dot product of a vector and a unit vector, will

    give the first vectors component in thatdirection.

    Dot product is commutative

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    Cross Product

    Also called the vector product, because the result ofthis multiplication is another vector.

    A x B produces another vector: Perpendicular to A and B

    With a magnitude equal to the product of the magnitudesof the two vectors times the sine of the angle betweenthem

    For the direction of the resulting vector, use the right-hand rule

    A x B = - B x A

    i x i = 0; j x j = 0; k x k = 0

    i x j = k ; j x k = i ; k x i = j

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    Now, we exercise

    Page 88; Section 3.2: 12 to 15

    Page 89; Section 3.3: 30 to 36

    Page 90; Section 3.4: 47 to 65

    Homework: Review problems (pg 91)

    Group 1: 66, 68, 70, 74, 76

    Group 2: 67, 69, 71, 73, 75

    For everyone: 72, 77, 78

    END OF SESSION 1 (I wonder if were onschedule or not?)

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    Motion along a straight line We will assume that the straight line coincides

    with the x axis. Therefore, the x coordinate is afunction of time x=f(t).

    Average velocity is defined as the change ofposition divided by the time interval

    If we use a x vs t graph, the definition ofaverage velocity is the same as the slopebetween the two points (t1, x1) and (t2,x2)

    Are average speedand average velocitythe

    same? Discuss. Can the average velocity be negative? If so, how

    do we interpret this result?

    Velocity unit: meters / seg

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    Chapter 2: Motion

    Mechanics: the branch of Physics that studiesbodies in motion. Two major divisions: Kinematics (position, velocity, and acceleration)

    Dynamics (force)

    As a first approach, we will study translationalmotion of a particle (leaving rotational andinternal motions for later).

    Average speed = total distance traveled / timetaken

    Motion and speed are relative to the frame ofreference with respect to which it is calculated.

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    Instantaneous velocity

    Defined from a graphical point of view as theslope of the tangent that touches the plot at aspecific time.

    Can the average velocity be equal to theinstantaneous velocity? Discuss.

    Using a mathematical approach:v = lim (Dx/Dt)

    Dt0

    And that takes us to the calculus definition:v = dx / dt

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    Acceleration

    The average acceleration is defined as the change ofvelocity divided by the change of timea = (v2 v1) / (t2 t1)

    Units : meters / seg2

    If a vehicle is speeding up while moving in the negativedirection, what happens to its acceleration? And if itsslowing down?

    Instantaneous acceleration is equal to the slope of the

    tangent drawn on the plot of velocity vs. time. It is also the first derivative of the velocity, hence:

    a = (d/dt)(dx/dt) = d2x/dt2

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    Motion with constant acceleration

    Constant acceleration implies a constant slope in theplot of velocity vs. time (feel free to graph this)

    From the previous graph, we can determine that theacceleration (slope) is:

    a = (Vf V0)/t; therefore

    Vf= V0 + at (Eq. 1)

    The average velocity, at a constant acceleration, is theaverage of two values: initial and final velocity:

    v = (Vf+ V0)/2; or

    v = V0 + at/2

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    More motion (at constant acceleration)

    The new position x will be equal to the initial positionx0 plus the product of the average velocity multipliedby time:

    x = x0 + vt; therefore,

    x = x0 + v0t + at2

    /2 (Eq. 2) If we isolate t from Eq. 1 and replace it in Eq. 2, we will

    find a direct relationship between position and velocity(go ahead, find it):

    (x x0) = (vf2 v0

    2) /2a (Eq. 3)

    In free fall, the acceleration is a constant usuallydenoted by g, and it is equal to 9.81 m/s2

    Standard gs, terminal velocity

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    Exercises, exercises, exercises

    Solve the challenging ones for: Speed (pg 58)

    Average velocity (pg 60)

    Acceleration (pg 61)

    Motion with constant acceleration (pg 62)

    Acceleration of free fall (pg 64)

    Integration of equations of motion (pg 65)

    Ah, homework! Review problems (pg 66) Group 1: odd numbers between 110 and 120

    Group 2: even numbers between 111 and 119 PLUS119

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    Ch. 4: Motion in 2D and 3D

    Two-dimensional motion consists of two one-dimensional motions occurring simultaneously.

    To describe translational motion of a particle in aplane, we will use an x coordinate and a y coordinate.

    Average and instantaneous velocity for the x and ycomponents are defined as seen in Chapter 2. Andapplying Pythagoras, we can obtain the instantaneousspeed.

    Apply the same strategy to define average accelerationand instantaneous acceleration.

    Remember: velocity and acceleration are vectors, andcan be separated into their x and y components.

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    Projectile Motion

    The only acceleration experienced by a bodythat has been launched, is gravity (verticalacceleration).

    Therefore, the x component of acceleration isZERO, and the y component of acceleration is-g (-9.81 m/s2).

    So we have linear uniform motion for the xaxis, and motion with constant accelerationfor the y axis.

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    Uniform Circular Motion

    Defined as motion with constant speed along acircular path

    The velocity vector at any instant is tangent to the

    path (or to the circle). All the velocity vectors have same magnitude but

    different direction; therefore, circular motion isaccelerated motion.

    The acceleration vector points inward along theradius, toward the center of the circle (centripetalacceleration). Why?

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    Exercises

    They begin on page 121, as usual practice the

    exercises with an asterisk (they should be the

    most challenging ones).

    And finally, homework:

    Review problems, page 127: everyone solves

    exercises 102 to 105.

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    Chapter 5: Newtons Laws of Motion

    Dynamics: the study of forces and their effects

    on the motion of bodies

    Under ideal frictionless conditions, a body in

    motion will continue to move forever

    Newtons First Law establishes: In the

    absence of a net external force, a body at rest

    remains at rest, and a body in motion

    continues to move at constant velocity. Inertia: the tendency of a body to continue in

    its initial state of motion

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    Considerations for the Law of Inertia

    The Law of Inertia is not valid in all reference

    frames; specifically, in a reference frame that

    has an accelerated motion relative to another.

    The reference frames in which the 1st Law is

    valid, are called inertialreference frames.

    The velocity of the particle is relative to the

    reference frame; acceleration is absolute(regardless of the reference frame)

    d

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    Newtons 2nd Law

    Force: any push or pull exerted on a body;

    such a push (or pull) has magnitude and

    direction

    As Sir Isaac would have said: An external

    force acting on a body, gives it an acceleration

    that is in the direction of the force and has a

    magnitude directly proportional to the

    magnitude of the force and inverselyproportional to the mass of the body

    a = F / m and therefore, F = ma

    h d l

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    Weight, Contact Force and Normal Force

    Mass is an intrinsic property of the body; weight

    is an extrinsic property of a body (measuring thepull of gravity on it, and gravity depends on

    location).

    Gravity requires no perceptible medium for its

    transmission. Common forces require contact.

    Contact force: the push that the surface of a body

    exerts on the other adjacent surface. If the two

    bodies are solid: Friction force: sliding surfaces

    Normal or compression force: perpendicular press

    between surfaces

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    Mass and Force

    Mass is a measure of the resistance that the body

    offers to changes in its velocity.

    Force: a vector applied to a specific mass, that

    generates acceleration

    In the International Unit system, the unit of force isthe Newton (the force that will give a mass of 1 Kg an

    acceleration of 1 m/s2

    In the British system, the unit of force is the pound-

    force (lbf), and its equal to 4.482 N.

    Weight is a force, proportional to the mass of the

    body being weighed.

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    Newtons 3rd Law

    Quoting Sir Isaac: Whenever a body exerts a

    force on another body, the latter exerts a force

    of equal magnitude and opposite direction on

    the former.

    Action-reaction forces need not to be normal

    to the surface

    Not all two forces of equal magnitudes andopposite directions are an action-reaction pair.

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    Final relevant concepts

    Free-body diagram: the body is presented free

    from its surrounding environment, and the

    environment is reduced to the forces it exerts over

    the body. Tension: the force with which a cable pulls on what is

    attached to it. The direction of the tension is along

    the cable.

    The transmission of the magnitude of the tension

    without change occurs even if the cable is led around

    pulleys

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    Exercises (as usual)

    The Problems section begins on page 162.

    You should practice the exercises marked with

    the asterisks (the challenging ones).

    1st part of homework for week No. 2: Review

    problems for everyone! (starting on page 168)

    Exercises 78 to 81

    Exercises 91 to 94

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    I wonder if were still running late