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Chapter 3 Vectors and Two-Dimensional Motion. Vector Notation When handwritten, use an arrow: When handwritten, use an arrow: When printed, will be in.

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Presentation on theme: "Chapter 3 Vectors and Two-Dimensional Motion. Vector Notation When handwritten, use an arrow: When handwritten, use an arrow: When printed, will be in."— Presentation transcript:

1 Chapter 3 Vectors and Two-Dimensional Motion

2 Vector Notation When handwritten, use an arrow: When handwritten, use an arrow: When printed, will be in bold print: A When printed, will be in bold print: A When dealing with just the magnitude of a vector in print, an italic letter will be used: A When dealing with just the magnitude of a vector in print, an italic letter will be used: A

3 Properties of Vectors Equality of Two Vectors Equality of Two Vectors Two vectors are equal if they have the same magnitude and the same direction Two vectors are equal if they have the same magnitude and the same direction Movement of vectors in a diagram Movement of vectors in a diagram Any vector can be moved parallel to itself without being affected Any vector can be moved parallel to itself without being affected

4 More Properties of Vectors Negative Vectors Negative Vectors Two vectors are negative if they have the same magnitude but are 180° apart (opposite directions) Two vectors are negative if they have the same magnitude but are 180° apart (opposite directions) A = -B A = -B Resultant Vector Resultant Vector The resultant vector is the sum of a given set of vectors The resultant vector is the sum of a given set of vectors

5 Adding Vectors When adding vectors, their directions must be taken into account When adding vectors, their directions must be taken into account Units must be the same Units must be the same Graphical Methods Graphical Methods Use scale drawings Use scale drawings Algebraic Methods Algebraic Methods More convenient More convenient

6 Adding Vectors Graphically (Triangle or Polygon Method) Choose a scale Choose a scale Draw the first vector with the appropriate length and in the direction specified, with respect to a coordinate system Draw the first vector with the appropriate length and in the direction specified, with respect to a coordinate system Draw the next vector with the appropriate length and in the direction specified, with respect to a coordinate system whose origin is the end of vector A and parallel to the coordinate system used for A Draw the next vector with the appropriate length and in the direction specified, with respect to a coordinate system whose origin is the end of vector A and parallel to the coordinate system used for A

7 Graphically Adding Vectors, cont. Continue drawing the vectors “tip-to-tail” Continue drawing the vectors “tip-to-tail” The resultant is drawn from the origin of A to the end of the last vector The resultant is drawn from the origin of A to the end of the last vector Measure the length of R and its angle Measure the length of R and its angle Use the scale factor to convert length to actual magnitude Use the scale factor to convert length to actual magnitude

8 Graphically Adding Vectors, cont. When you have many vectors, just keep repeating the process until all are included When you have many vectors, just keep repeating the process until all are included The resultant is still drawn from the origin of the first vector to the end of the last vector The resultant is still drawn from the origin of the first vector to the end of the last vector

9 Alternative Graphical Method When you have only two vectors, you may use the Parallelogram Method When you have only two vectors, you may use the Parallelogram Method All vectors, including the resultant, are drawn from a common origin All vectors, including the resultant, are drawn from a common origin The remaining sides of the parallelogram are sketched to determine the diagonal, R The remaining sides of the parallelogram are sketched to determine the diagonal, R

10 Notes about Vector Addition Vectors obey the Commutative Law of Addition Vectors obey the Commutative Law of Addition The order in which the vectors are added doesn’t affect the result The order in which the vectors are added doesn’t affect the result

11 Vector Subtraction Special case of vector addition Special case of vector addition If A – B, then use A+(-B) If A – B, then use A+(-B) Continue with standard vector addition procedure Continue with standard vector addition procedure

12 Multiplying or Dividing a Vector by a Scalar The result of the multiplication or division is a vector The result of the multiplication or division is a vector The magnitude of the vector is multiplied or divided by the scalar The magnitude of the vector is multiplied or divided by the scalar If the scalar is positive, the direction of the result is the same as of the original vector If the scalar is positive, the direction of the result is the same as of the original vector If the scalar is negative, the direction of the result is opposite that of the original vector If the scalar is negative, the direction of the result is opposite that of the original vector

13 Components of a Vector A component is a part A component is a part It is useful to use rectangular components It is useful to use rectangular components These are the projections of the vector along the x- and y-axes These are the projections of the vector along the x- and y-axes

14 Components of a Vector, cont. The x-component of a vector is the projection along the x-axis The x-component of a vector is the projection along the x-axis The y-component of a vector is the projection along the y-axis The y-component of a vector is the projection along the y-axis Then, Then,

15 More About Components of a Vector The previous equations are valid only if θ is measured with respect to the x-axis The previous equations are valid only if θ is measured with respect to the x-axis The components can be positive or negative and will have the same units as the original vector The components can be positive or negative and will have the same units as the original vector The components are the legs of the right triangle whose hypotenuse is A The components are the legs of the right triangle whose hypotenuse is A May still have to find θ with respect to the positive x-axis May still have to find θ with respect to the positive x-axis

16 Adding Vectors Algebraically Choose a coordinate system and sketch the vectors Choose a coordinate system and sketch the vectors Find the x- and y-components of all the vectors Find the x- and y-components of all the vectors Add all the x-components Add all the x-components This gives R x : This gives R x :

17 Adding Vectors Algebraically, cont. Add all the y-components Add all the y-components This gives R y : This gives R y : Use the Pythagorean Theorem to find the magnitude of the Resultant: Use the Pythagorean Theorem to find the magnitude of the Resultant: Use the inverse tangent function to find the direction of R: Use the inverse tangent function to find the direction of R:

18 Motion in Two Dimensions Using + or – signs is not always sufficient to fully describe motion in more than one dimension Using + or – signs is not always sufficient to fully describe motion in more than one dimension Vectors can be used to more fully describe motion Vectors can be used to more fully describe motion Still interested in displacement, velocity, and acceleration Still interested in displacement, velocity, and acceleration

19 Displacement The position of an object is described by its position vector, r The position of an object is described by its position vector, r The displacement of the object is defined as the change in its position The displacement of the object is defined as the change in its position Δr = r f - r i Δr = r f - r i

20 Velocity The average velocity is the ratio of the displacement to the time interval for the displacement The average velocity is the ratio of the displacement to the time interval for the displacement The instantaneous velocity is the limit of the average velocity as Δt approaches zero The instantaneous velocity is the limit of the average velocity as Δt approaches zero The direction of the instantaneous velocity is along a line that is tangent to the path of the particle and in the direction of motion The direction of the instantaneous velocity is along a line that is tangent to the path of the particle and in the direction of motion

21 Acceleration The average acceleration is defined as the rate at which the velocity changes The average acceleration is defined as the rate at which the velocity changes The instantaneous acceleration is the limit of the average acceleration as Δt approaches zero The instantaneous acceleration is the limit of the average acceleration as Δt approaches zero

22 Ways an Object Might Accelerate The magnitude of the velocity (the speed) can change The magnitude of the velocity (the speed) can change The direction of the velocity can change The direction of the velocity can change Even though the magnitude is constant Even though the magnitude is constant Both the magnitude and the direction can change Both the magnitude and the direction can change

23 Projectile Motion An object may move in both the x and y directions simultaneously An object may move in both the x and y directions simultaneously It moves in two dimensions It moves in two dimensions The form of two dimensional motion we will deal with is called projectile motion The form of two dimensional motion we will deal with is called projectile motion

24 Assumptions of Projectile Motion We may ignore air friction We may ignore air friction We may ignore the rotation of the earth We may ignore the rotation of the earth With these assumptions, an object in projectile motion will follow a parabolic path With these assumptions, an object in projectile motion will follow a parabolic path

25 Rules of Projectile Motion The x- and y-directions of motion can be treated independently The x- and y-directions of motion can be treated independently The x-direction is uniform motion The x-direction is uniform motion a x = 0 a x = 0 The y-direction is free fall The y-direction is free fall a y = -g a y = -g The initial velocity can be broken down into its x- and y-components The initial velocity can be broken down into its x- and y-components

26 Projectile Motion

27 Some Details About the Rules x-direction x-direction a x = 0 a x = 0 x = v xo t x = v xo t This is the only operative equation in the x- direction since there is uniform velocity in that direction This is the only operative equation in the x- direction since there is uniform velocity in that direction

28 More Details About the Rules y-direction y-direction free fall problem free fall problem a = -g a = -g take the positive direction as upward take the positive direction as upward uniformly accelerated motion, so the motion equations all hold uniformly accelerated motion, so the motion equations all hold

29 Velocity of the Projectile The velocity of the projectile at any point of its motion is the vector sum of its x and y components at that point The velocity of the projectile at any point of its motion is the vector sum of its x and y components at that point

30 Some Variations of Projectile Motion An object may be fired horizontally An object may be fired horizontally The initial velocity is all in the x-direction The initial velocity is all in the x-direction v o = v x and v y = 0 v o = v x and v y = 0 All the general rules of projectile motion apply All the general rules of projectile motion apply

31 Non-Symmetrical Projectile Motion Follow the general rules for projectile motion Follow the general rules for projectile motion Break the y-direction into parts Break the y-direction into parts up and down up and down symmetrical back to initial height and then the rest of the height symmetrical back to initial height and then the rest of the height

32 Relative Velocity It may be useful to use a moving frame of reference instead of a stationary one It may be useful to use a moving frame of reference instead of a stationary one It is important to specify the frame of reference, since the motion may be different in different frames of reference It is important to specify the frame of reference, since the motion may be different in different frames of reference There are no specific equations to learn to solve relative velocity problems There are no specific equations to learn to solve relative velocity problems

33 Solving Relative Velocity Problems The pattern of subscripts can be useful in solving relative velocity problems The pattern of subscripts can be useful in solving relative velocity problems Write an equation for the velocity of interest in terms of the velocities you know, matching the pattern of subscripts Write an equation for the velocity of interest in terms of the velocities you know, matching the pattern of subscripts


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