Two-Dimensional Analysis: Projectile and Uniform Circular Motion Study Guide

Fundamentals of Two-Dimensional Analysis

  • The study of two-dimensional analysis focuses on two primary types of movement: Projectile Motion and Circular Motion.

  • The central objective is to analyze projectile motion by relating horizontal and vertical components. This analysis allows for the determination of critical quantities, including:

    • Range

    • Maximum height

    • Time of flight

    • Velocity

Projectile Motion Dynamics and Key Terminology

  • Projectile motion is defined as the curved path an object follows when it is thrown into the air, specifically moving under the influence of the force of gravity.

  • Key parameters of a projectile's flight include:

    • Range (RR): This is the horizontal distance covered by the object during its entire flight.

    • Height (HH): This is the vertical distance measured from the ground to the object's highest point.

    • Highest Point Characteristics: As the projectile follows its curved path, it reaches an apex where its vertical velocity (VyV_y) is exactly equal to zero (00).

    • Launch Angle (θ\theta): The specific angle at which the projectile is launched significantly affects its trajectory.

Components of Initial Velocity

  • To analyze the motion, the initial velocity (ViV_i) must be resolved into its horizontal (xx) and vertical (yy) components:

    • For the x-component: Vx=Vi×cos(θ)V_x = V_i \times \text{cos}(\theta)

    • For the y-component: Vy=Vi×sin(θ)V_y = V_i \times \text{sin}(\theta)

  • The magnitude of the resultant velocity vector is given by: v=sqr(Vx2+Vy2)v = \text{sqr}(V_x^2 + V_y^2) [Note: Represented as v=sqr(v12+v22)v = \text{sqr}(v1^2 + v2^2) in some notations].

  • The angle of the trajectory can be found using the inverse tangent function: θ=tan−1(VyVx)\theta = \text{tan}^{-1}(\frac{V_y}{V_x})

Sample Problem: Component Resolution (Sipa)

  • Scenario: A sipa is kicked at a 30∘30^\circ angle with an initial velocity of 6 m/s6\,m/s.

  • Given Values:

    • Initial Velocity (ViV_i) = 6 m/s6\,m/s

    • Angle (θ\theta) = 30∘30^\circ

  • Calculations for x-component (VxV_x):

    • Vx=Vi×cos(θ)V_x = V_i \times \text{cos}(\theta)

    • Vx=6 m/s×cos(30∘)V_x = 6\,m/s \times \text{cos}(30^\circ)

    • Vx=6 m/s×0.8660V_x = 6\,m/s \times 0.8660

    • Vx=5.2 m/sV_x = 5.2\,m/s

  • Calculations for y-component (VyV_y):

    • Vy=Vi×sin(θ)V_y = V_i \times \text{sin}(\theta)

    • Vy=6 m/s×sin(30∘)V_y = 6\,m/s \times \text{sin}(30^\circ)

    • Vy=6 m/s×0.5V_y = 6\,m/s \times 0.5

    • Vy=3 m/sV_y = 3\,m/s

Trajectory Calculations: Height, Range, and Time

  • Specific formulas are utilized to determine the physical properties of a projectile's path:

    • Total Time (TT): The duration of the flight is calculated as: T=2Vi×sin(θ)gT = \frac{2V_i \times \text{sin}(\theta)}{g}

    • Maximum Height (HH): The peak vertical distance is calculated as: H=(Vi×sin(θ))22gH = \frac{(V_i \times \text{sin}(\theta))^2}{2g}

    • Range (RR): The total horizontal distance is calculated as: R=Vi2×sin(2θ)gR = \frac{V_i^2 \times \text{sin}(2\theta)}{g}

Sample Problem: Takraw Ball Analysis

  • Scenario: A takraw ball has an initial velocity of 5 m/s5\,m/s and is projected at an angle of 15∘15^\circ. The goal is to find the maximum height, total time, and range as it lands.

  • Given Values:

    • Vi=5 m/sV_i = 5\,m/s

    • θ=15∘\theta = 15^\circ

    • g=9.8 m/s2g = 9.8\,m/s^2

  • Calculation of Maximum Height (HH):

    • H=(5 m/s×sin(15∘))22×9.8 m/s2H = \frac{(5\,m/s \times \text{sin}(15^\circ))^2}{2 \times 9.8\,m/s^2}

    • H=0.09 mH = 0.09\,m

  • Calculation of Range (RR):

    • R=(5 m/s)2×sin(2×15∘)9.8 m/s2R = \frac{(5\,m/s)^2 \times \text{sin}(2 \times 15^\circ)}{9.8\,m/s^2}

    • R=1.28 mR = 1.28\,m

  • Calculation of Total Time (TT):

    • T=2×(5 m/s)×sin(15∘)9.8 m/s2T = \frac{2 \times (5\,m/s) \times \text{sin}(15^\circ)}{9.8\,m/s^2}

    • T=0.26 sT = 0.26\,s

Activity: Solving for Sipa Flight

  • The exercise involves finding the maximum height, total time, and range for a sipa kicked at an initial velocity of 5 m/s5\,m/s.

  • Different angles are assigned based on the student's category:

    • For Male Students: 30∘30^\circ and 50∘50^\circ

    • For Female Students: 40∘40^\circ and 60∘60^\circ

Uniform Circular Motion (UCM)

  • Uniform Circular Motion is a type of motion that allows an object to follow a circular path while maintaining a constant speed.

  • Common Examples of UCM:

    • Carousel

    • Centrifuge

    • Microwave

    • Washing machine

    • Machine dryer

Dynamics of Circular Motion

  • Changing Direction: As an object moves in a circle, it is constantly changing its direction. Even though the speed remains constant, the velocity changes because velocity is a vector quantity (having both magnitude and direction).

  • Tangential Velocity: At all instances, the object is moving tangent to the circle. The velocity vector is directed tangent to the circle at every point.

  • Perpendicular Relationship: The directions of acceleration and velocity are perpendicular to each other while the speed remains constant.

  • Related Terms:

    • Period (TT): The amount of time needed to complete one full rotation.

    • Frequency (ff): The number of rotations completed per unit of time.

Centripetal Force and Acceleration

  • Centripetal Force (FcF_c): This is the net force acting upon an object in circular motion, directed toward the center of the circle. It is what allows the object to accelerate in a circular path.

  • Centripetal Acceleration (aca_c): This is the acceleration of a body traversing a circular path. It is caused by the constant change in direction of the velocity vector.

    • Direction: Directed radially toward the center of the circle.

    • Magnitude formula: ac=v2ra_c = \frac{v^2}{r}

    • Units: Measured in meters per second squared (m/s2m/s^2).

  • Centripetal Force Formula: Based on Newton's Second Law (F=maF = ma), the centripetal force is calculated as:

    • Fc=m×acF_c = m \times a_c

    • Units:

      • mass (mm) is measured in kilograms (kgkg).

      • force (FcF_c) is measured in Newtons (NN).

      • acceleration (aca_c) is measured in m/s2m/s^2.

Sample Problem: Carousel Analysis

  • Scenario: Shiela is riding in a carousel moving at a constant speed of 7.0 m/s7.0\,m/s with a radius of 1.3 m1.3\,m.

  • Part A: Centripetal Acceleration:

    • Given:

      • v=7.0 m/sv = 7.0\,m/s

      • r=1.3 mr = 1.3\,m

    • Formula: ac=v2ra_c = \frac{v^2}{r}

    • Solution:

      • ac=(7.0 m/s)21.3 ma_c = \frac{(7.0\,m/s)^2}{1.3\,m}

      • ac=49.0 m2/s21.3 ma_c = \frac{49.0\,m^2/s^2}{1.3\,m}

      • ac=37.69 m/s2a_c = 37.69\,m/s^2

  • Part B: Centripetal Force:

    • Requirement: Find the force if the mass of the carousel (or system component) is 26 kgs26\,kgs.

    • Given:

      • m=26 kgsm = 26\,kgs

      • ac=37.69 m/s2a_c = 37.69\,m/s^2

    • Formula: Fc=m×acF_c = m \times a_c

    • Solution:

      • Fc=26 kg×37.69 m/s2F_c = 26\,kg \times 37.69\,m/s^2

      • Fc=979.94 kg⋅m/s2F_c = 979.94\,kg \cdot m/s^2 or 979.94 N979.94\,N

  • Calculation Note: Always round off results to the nearest hundredths.