Study Notes on Vector Quantities and Their Applications

Chapter Four: Vector Quantities & Their Applications

Key Ideas

  • Vectors: Quantities that possess both magnitude and direction. Examples include forces and displacements.

    • A vector is represented by an arrow:

    • Direction: The direction of the vector is indicated by the direction the arrow points.

    • Magnitude: The length of the arrow is proportional to the vector's magnitude.

  • Vector Addition: The process of combining vector quantities.

    • The result of vector addition is termed the resultant vector.

    • Vectors can be added:

    • Geometrically: By drawing to scale.

    • Mathematically: Using algebra and trigonometry.

  • Resolution of Vectors: The process of breaking down a single vector into its components.

    • Simplifies problems involving two-dimensional motion, static equilibrium, and motion on inclined planes.

Key Objectives

At the conclusion of this chapter you will be able to:

  • Define the terms scalar and vector, and list scalar and vector quantities.

  • Represent a vector quantity by an arrow drawn to scale.

  • Relate the direction of a vector to compass directions.

  • Define the term resultant vector.

  • Add vector quantities both graphically and algebraically.

  • Relate vector subtraction to vector addition.

  • Define vector resolution and resolve a vector into its x- and y-components (limited to two-dimensional analysis).

  • Add vector quantities by combining their x- and y-components.

  • Define the term static equilibrium.

  • Solve static equilibrium problems.

  • Identify and calculate the parallel and perpendicular components of an object’s weight when on an inclined plane.

  • Solve problems involving motion on inclined planes and in two dimensions.

4.1 Introduction

  • Scalar Quantities: Quantities described solely by their magnitudes (size) such as mass, time, and temperature.

  • Vector Quantities: Must include direction in their description (e.g., velocity, acceleration, and force).

4.2 Displacement and Representation of Vector Quantities

  • Displacement: Defined as a directed change in the position of an object. - Example: An indication of 30 meters [east] indicates a displacement.

  • Vectors can be represented by arrows, where:

    • Arrow length represents magnitude.

    • Direction points from the tail to the tip.

    • Example scalings are provided:

    • 1 cm of arrow length represents 20 meters.

4.3 Vector Addition

  • Concept: Determines the net effect of two or more vectors acting on an object.

    • Example: An airplane traveling at 300 m/s [east] enters a jet stream with a velocity of 100 m/s [north].

    • Resultant calculation performed by placing vectors head to tail:

    OA (3.0 m [E])+B (4.0 m [E])=R (7.0 m [E])OA \text{ (3.0 m [E])} + B \text{ (4.0 m [E])} = R \text{ (7.0 m [E])}

  • When vectors are in opposite directions, their magnitudes are subtracted:

    • Example: A bird flies 3.0 km [N] then 4.0 km [S], yielding a resultant of:

      R=1.0km[S]R = 1.0 km [S]

  • Vectors at right angles:

    • Can be added via the Pythagorean theorem:

      R2=P2+J2R^2 = P^2 + J^2

4.4 Vector Subtraction

  • Definition: Subtraction considered as a special case of addition:

    • AB=A+(B)A - B = A + (-B).

    • The negative vector is equal in magnitude but opposite in direction.

4.5 Vector Resolution

  • Definition: The process of breaking down a single vector into its perpendicular components along specified axes (typically x and y).

    • This simplifies the analysis of vector interactions in two or three dimensions.

    • A vector AA can be resolved into:

      • x-component: Ax=Acos(angle)A_x = A \cos(\text{angle})

      • y-component: Ay=Asin(angle)A_y = A \sin(\text{angle})

        where the angle is the angle the vector makes with the positive x-axis.

4.6 Adding Vectors by Components

  • Method:

    1. Resolve each vector into its x and y components.

    2. Algebraically sum all the x-components to find the resultant x-component (Rx=sum of AxR_x = \text{sum of } A_x).

    3. Algebraically sum all the y-components to find the resultant y-component (Ry=sum of AyR_y = \text{sum of } A_y).

    4. Calculate the magnitude of the resultant vector using the Pythagorean theorem: R=Rx2+Ry2R = \sqrt{R_x^2 + R_y^2}.

    5. Determine the direction of the resultant vector using trigonometry: angle=arctan(Ry/Rx)\text{angle} = \arctan(R_y/R_x). The quadrant of the resultant must be considered based on the signs of RxR_x and RyR_y.

4.7 Static Equilibrium

  • Definition: A state where an object is at rest and the net force acting on it is zero.

    • This implies that the object is not accelerating (a=0a=0).

  • Conditions for Static Equilibrium:

    • The sum of all force components in the x-direction must be zero: sum of Fx=0\text{sum of } F_x = 0.

    • The sum of all force components in the y-direction must be zero: sum of Fy=0\text{sum of } F_y = 0.

  • Problem Solving: Typically involves resolving all forces into components and applying these equilibrium conditions to solve for unknown forces.

4.8 Motion on Inclined Planes

  • Analysis: Problems involving objects on inclined planes are simplified by resolving forces into components parallel and perpendicular to the incline.

  • Weight Components: An object's weight (Fg)(Fg) acting vertically downwards is resolved into:

    • Parallel component: The component of weight acting down the incline: W=Fgsin(angle)W_{||}=Fg\sin(\text{angle})

    • Perpendicular component: The component of weight normal to the incline: W=Fgcos(angle)W_{\perp}=Fg\cos(\text{angle})

      where the angle is the angle of inclination of the plane with the horizontal.

  • Forces to Consider: Normal force, friction, and any applied forces, in addition to the components of weight.

4.9 Two-Dimensional Motion

  • Concept: Motion that occurs in a plane, such as projectile motion or circular motion. The x and y components of motion are generally independent but occur simultaneously.

  • Independence of Components:

    • Horizontal motion (x-direction) is often characterized by constant velocity (assuming no air resistance).

    • Vertical motion (y-direction) is characterized by constant acceleration due to gravity (g=9.8 m/s2g = 9.8 \text{ m/s}^2 downwards).

  • Kinematic Equations: Applied separately to the x and y components. For example:

    • x=v0xt+12axt2x = v_{0x}t + \frac{1}{2}a_xt^2

    • y=v0yt+12ayt2y = v_{0y}t + \frac{1}{2}a_yt^2

  • Projectile Motion: A common example where an object is launched into the air and follows a parabolic trajectory under the influence of gravity only.