Comprehensive Study Guide: Motion and Acceleration

Kinematic Variables and Systematic Problem-Solving Routine

  • Fundamental Kinematic Variables and Standard SI Units:

    • Initial position: xix_i, measured in meters (m\text{m}
    • Final position: xfx_f, measured in meters (m\text{m}
    • Displacement: Δx=xf−xi\Delta x = x_f - x_i, defined as the net change in position, measured in meters (m\text{m}
    • Initial velocity: viv_i, measured in meters per second (m/s\text{m/s}
    • Final velocity: vfv_f, measured in meters per second (m/s\text{m/s}
    • Acceleration: aa, measured in meters per second squared (m/s2\text{m/s}^2
    • Elapsed time: tt or Δt\Delta t, measured in seconds (s\text{s}
  • Step-by-Step Problem-Solving Routine:

    • Step 1: Establish a positive reference direction and ensure signs remain consistent throughout all calculations.
    • Step 2: Explicitly list all known physical quantities and identify the target unknown variable.
    • Step 3: Convert all given measurements to standard SI units (m\text{m}, s\text{s}, m/s\text{m/s}, m/s2\text{m/s}^2) before performing calculations.
    • Step 4: Select a kinematic equation that connects the known parameters directly to the unknown quantity.
    • Step 5: Substitute values, perform numerical calculations, append appropriate physical units, and verify that the sign and magnitude make physical sense.

Speed and Velocity

  • Core Concepts and Distinctions:

    • Speed: Describes how rapidly distance is covered over time. Speed is a scalar quantity possessing magnitude only, with no directional component.
    • Average Speed Formula:average speed=total distancetotal time\text{average speed} = \frac{\text{total distance}}{\text{total time}}
    • Velocity: Describes both the speed and directional orientation of motion. Velocity is a vector quantity possessing both magnitude and direction.
    • Average Velocity Formula: Defined as displacement divided by the elapsed time interval:     vavg=ΔxΔt=xf−xiΔtv_{\text{avg}} = \frac{\Delta x}{\Delta t} = \frac{x_f - x_i}{\Delta t}
    • Standard SI Unit: Both speed and velocity are expressed in meters per second (m/s\text{m/s}).
  • Worked Examples and Practice:

    • Worked Example 1 (Average Speed Calculation):
    • Problem Statement: A car travels 200 m200\,\text{m} in 2.0 s2.0\,\text{s}. Calculate its average speed.
    • Known Values: distance=200 m\text{distance} = 200\,\text{m}, time=2.0 s\text{time} = 2.0\,\text{s}
    • Substitution: average speed=200 m2.0 s\text{average speed} = \frac{200\,\text{m}}{2.0\,\text{s}}
    • Calculation: average speed=100 m/s\text{average speed} = 100\,\text{m/s}
    • Final Answer: 100 m/s100\,\text{m/s}
    • Worked Example 2 (Average Velocity Calculation):
    • Problem Statement: A car moves 200 m200\,\text{m} east in 2.0 s2.0\,\text{s}. Calculate its average velocity.
    • Known Values: Δx=+200 m east\Delta x = +200\,\text{m}\text{ east}, Δt=2.0 s\Delta t = 2.0\,\text{s}
    • Substitution: vavg=+200 m2.0 sv_{\text{avg}} = \frac{+200\,\text{m}}{2.0\,\text{s}}
    • Calculation and Physical Interpretation: The positive sign directly represents the designated eastward direction.
    • Final Answer: +100 m/s east+100\,\text{m/s}\text{ east}
    • Question 1 (Grizzly Bear Average Speed with Unit Conversion):
    • Problem Statement: A grizzly bear runs 1870 m1870\,\text{m} in 2.0 min2.0\,\text{min}. What is its average speed in m/s\text{m/s}?
    • Unit Conversion: 2.0 min×60 s/min=120 s2.0\,\text{min} \times 60\,\text{s/min} = 120\,\text{s}
    • Substitution: average speed=1870 m120 s\text{average speed} = \frac{1870\,\text{m}}{120\,\text{s}}
    • Calculation: average speed=15.58 m/s\text{average speed} = 15.58\,\text{m/s}
    • Final Answer: 15.6 m/s15.6\,\text{m/s}

Average Acceleration

  • Definitions and Mathematical Formulation:

    • Acceleration: The rate of change of velocity with respect to time. An object experiences acceleration when it speeds up, slows down, or alters its direction of travel.
    • Direction and Sign: Acceleration is a vector quantity; its algebraic sign (+ or −+\text{ or } -) depends strictly on the established coordinate direction.
    • Average Acceleration Formula:aavg=ΔvΔt=vf−viΔta_{\text{avg}} = \frac{\Delta v}{\Delta t} = \frac{v_f - v_i}{\Delta t}
    • Standard SI Unit: Meters per second squared (m/s2\text{m/s}^2).
  • Worked Examples and Practice Applications:

    • Worked Example 3 (Car Accelerating from Rest):
    • Problem Statement: A car starts from rest and reaches +10.0 m/s+10.0\,\text{m/s} in 8.0 s8.0\,\text{s}. Calculate its average acceleration.
    • Known Values: vi=0 m/sv_i = 0\,\text{m/s}, vf=+10.0 m/sv_f = +10.0\,\text{m/s}, Δt=8.0 s\Delta t = 8.0\,\text{s}
    • Substitution: a=(+10.0 m/s)−(0 m/s)8.0 sa = \frac{(+10.0\,\text{m/s}) - (0\,\text{m/s})}{8.0\,\text{s}}
    • Calculation: a=+1.25 m/s2a = +1.25\,\text{m/s}^2
    • Final Answer: +1.25 m/s2+1.25\,\text{m/s}^2
    • Question 1 (Runner Accelerating in Positive Direction):
    • Problem Statement: A runner increases velocity from +2.0 m/s+2.0\,\text{m/s} to +10.0 m/s+10.0\,\text{m/s} in the positive direction over 3.0 s3.0\,\text{s}. Find the average acceleration.
    • Method: Apply a=vf−viΔta = \frac{v_f - v_i}{\Delta t}
    • Calculation: a=(+10.0)−(+2.0)3.0=8.03.0=+2.67 m/s2a = \frac{(+10.0) - (+2.0)}{3.0} = \frac{8.0}{3.0} = +2.67\,\text{m/s}^2
    • Final Answer: +2.67 m/s2+2.67\,\text{m/s}^2
    • Question 2 (Vehicle Decelerating to a Stop):
    • Problem Statement: A driver applies the brakes for 5.0 s5.0\,\text{s}, slowing the car from +30.0 m/s+30.0\,\text{m/s} to rest. Determine the average acceleration.
    • Method: Apply a=vf−viΔta = \frac{v_f - v_i}{\Delta t}
    • Calculation: a=0−30.05.0=−30.05.0=−6.0 m/s2a = \frac{0 - 30.0}{5.0} = \frac{-30.0}{5.0} = -6.0\,\text{m/s}^2
    • Final Answer: −6.0 m/s2-6.0\,\text{m/s}^2
    • Question 3 (Bicyclist Decreasing Speed):
    • Problem Statement: A bicyclist decreases speed from 23 m/s23\,\text{m/s} to 13 m/s13\,\text{m/s} over 5.0 s5.0\,\text{s}. Calculate the bicyclist's acceleration.
    • Method: Apply a=vf−viΔta = \frac{v_f - v_i}{\Delta t}
    • Calculation: a=13−235.0=−105.0=−2 m/s2a = \frac{13 - 23}{5.0} = \frac{-10}{5.0} = -2\,\text{m/s}^2
    • Final Answer: −2 m/s2-2\,\text{m/s}^2
    • Question 4 (Car Increasing Speed):
    • Problem Statement: A car accelerates from 11 m/s11\,\text{m/s} to 25 m/s25\,\text{m/s} over 7.0 s7.0\,\text{s}. What is the acceleration of the car?
    • Method: Apply a=vf−viΔta = \frac{v_f - v_i}{\Delta t}
    • Calculation: a=25−117.0=147.0=2 m/s2a = \frac{25 - 11}{7.0} = \frac{14}{7.0} = 2\,\text{m/s}^2
    • Final Answer: 2 m/s22\,\text{m/s}^2

Kinematic Equations for Constant Acceleration

  • Kinematics Principles and Equation Selection:

    • Kinematics describes motion purely mathematically without considering the forces causing that motion.
    • When acceleration is uniform (constant), four primary algebraic relations link displacement, velocity, acceleration, and time.
    • Selection Criteria:
    • Velocity as a function of time: vf=vi+atv_f = v_i + a t (applied when time is known or sought, and displacement is omitted).
    • Displacement via average velocity: xf=xi+12(vi+vf)tx_f = x_i + \frac{1}{2}(v_i + v_f) t (applied when initial and final velocities are known and acceleration is omitted).
    • Position as a function of time and acceleration: xf=xi+vit+12at2x_f = x_i + v_i t + \frac{1}{2} a t^2 (applied when time, initial velocity, and acceleration are known).
    • Velocity as a function of displacement: vf2=vi2+2a(xf−xi)v_f^2 = v_i^2 + 2 a (x_f - x_i) or vf2=vi2+2aΔxv_f^2 = v_i^2 + 2 a \Delta x (applied when time is absent from the problem statement).
  • Comprehensive Worked Problems:

    • Worked Example 4 (Two-Part Acceleration Analysis):
    • Problem Statement: An object starts from rest at xi=0 mx_i = 0\,\text{m} and accelerates at +1.25 m/s2+1.25\,\text{m/s}^2. (a) Determine its position after 6.0 s6.0\,\text{s}. (b) Determine its velocity when it reaches position xf=+20.0 mx_f = +20.0\,\text{m}.
    • Known Values: xi=0 mx_i = 0\,\text{m}, vi=0 m/sv_i = 0\,\text{m/s}, a=+1.25 m/s2a = +1.25\,\text{m/s}^2, t=6.0 st = 6.0\,\text{s}
    • Part (a) Position Calculation: Using xf=xi+vit+12at2x_f = x_i + v_i t + \frac{1}{2} a t^2:       xf=0+0(6.0)+12(1.25)(6.0)2=22.5 mx_f = 0 + 0(6.0) + \frac{1}{2}(1.25)(6.0)^2 = 22.5\,\text{m}
    • Part (b) Velocity Calculation: Using vf2=vi2+2a(xf−xi)v_f^2 = v_i^2 + 2 a (x_f - x_i):       vf2=02+2(1.25)(20.0−0)=50.0 m2/s2v_f^2 = 0^2 + 2(1.25)(20.0 - 0) = 50.0\,\text{m}^2/\text{s}^2vf=50.0=+7.07 m/sv_f = \sqrt{50.0} = +7.07\,\text{m/s}
    • Final Answers: (a) +22.5 m+22.5\,\text{m}, (b) +7.07 m/s+7.07\,\text{m/s}
    • Question 1 (Runner Starting from Rest):
    • Problem Statement: A runner starts from rest at xi=0 mx_i = 0\,\text{m} and accelerates at +2.0 m/s2+2.0\,\text{m/s}^2 for 5.0 s5.0\,\text{s}. Find the runner's position after 5.0 s5.0\,\text{s}.
    • Method: Use xf=xi+vit+12at2x_f = x_i + v_i t + \frac{1}{2} a t^2
    • Calculation: xf=0+0(5.0)+12(2.0)(5.0)2=25 mx_f = 0 + 0(5.0) + \frac{1}{2}(2.0)(5.0)^2 = 25\,\text{m}
    • Final Answer: +25 m+25\,\text{m}
    • Question 2 (Cyclist Speeding Up Over a Set Distance):
    • Problem Statement: A cyclist accelerates at +1.50 m/s2+1.50\,\text{m/s}^2 over a distance of 10.0 m10.0\,\text{m}. If the cyclist's initial velocity is +10.0 m/s+10.0\,\text{m/s}, determine the final velocity.
    • Method: Time is omitted; use vf2=vi2+2aΔxv_f^2 = v_i^2 + 2 a \Delta x
    • Calculation: vf2=(10.0)2+2(1.50)(10.0)=100+30.0=130v_f^2 = (10.0)^2 + 2(1.50)(10.0) = 100 + 30.0 = 130
    • Square Root Evaluation: vf=130=11.4 m/sv_f = \sqrt{130} = 11.4\,\text{m/s}
    • Final Answer: +11.4 m/s+11.4\,\text{m/s}
    • Question 3 (Runner Decelerating Over a Set Distance):
    • Problem Statement: A runner slows down with a constant acceleration of −1.0 m/s2-1.0\,\text{m/s}^2 over a distance of 5.0 m5.0\,\text{m}. Given an initial velocity of +10.0 m/s+10.0\,\text{m/s}, find the final velocity.
    • Method: Use vf2=vi2+2aΔxv_f^2 = v_i^2 + 2 a \Delta x
    • Calculation: vf2=(10.0)2+2(−1.0)(5.0)=100−10.0=90v_f^2 = (10.0)^2 + 2(-1.0)(5.0) = 100 - 10.0 = 90
    • Square Root Evaluation: vf=90=9.49 m/sv_f = \sqrt{90} = 9.49\,\text{m/s}
    • Final Answer: +9.5 m/s+9.5\,\text{m/s}
    • Question 4 (Bicyclist Accelerating from Rest):
    • Problem Statement: A bicyclist starts from rest and accelerates at 5.50 m/s25.50\,\text{m/s}^2 for 12.0 s12.0\,\text{s}. Find the bicyclist's position at 12.0 s12.0\,\text{s}.
    • Method: Use xf=vit+12at2x_f = v_i t + \frac{1}{2} a t^2
    • Calculation: xf=0(12.0)+12(5.50)(12.0)2=12(5.50)(144)=396 mx_f = 0(12.0) + \frac{1}{2}(5.50)(12.0)^2 = \frac{1}{2}(5.50)(144) = 396\,\text{m}
    • Final Answer: 396 m396\,\text{m}
    • Question 5 (Cheetah Accelerating from Rest):
    • Problem Statement: A cheetah starts from rest and accelerates at 10.0 m/s210.0\,\text{m/s}^2 for 3.0 s3.0\,\text{s}. Find its position after 3.0 s3.0\,\text{s}.
    • Method: Use xf=vit+12at2x_f = v_i t + \frac{1}{2} a t^2
    • Calculation: xf=0(3.0)+12(10.0)(3.0)2=12(10.0)(9.0)=45 mx_f = 0(3.0) + \frac{1}{2}(10.0)(3.0)^2 = \frac{1}{2}(10.0)(9.0) = 45\,\text{m}
    • Final Answer: 45 m45\,\text{m}
    • Question 6 (Dropped Watermelon Velocity Prior to Impact):
    • Problem Statement: A watermelon is dropped from rest from a roof 15.0 m15.0\,\text{m} above the ground. Ignoring air resistance, calculate its velocity immediately prior to ground impact.
    • Coordinate Convention: Select downward as positive: vi=0v_i = 0, a=+9.81 m/s2a = +9.81\,\text{m/s}^2, Δx=+15.0 m\Delta x = +15.0\,\text{m}
    • Method: Use vf2=vi2+2aΔxv_f^2 = v_i^2 + 2 a \Delta x
    • Calculation: vf=2(9.81)(15.0)=294.3=17.2 m/sv_f = \sqrt{2(9.81)(15.0)} = \sqrt{294.3} = 17.2\,\text{m/s}
    • Final Answer: 17.2 m/s downward17.2\,\text{m/s}\text{ downward}

Free Fall and Gravitational Acceleration

  • Free Fall Dynamics and Conditions:

    • Definition: Free fall occurs when the gravitational force is the sole significant influence acting upon a body (aerodynamic drag and air resistance are negligible).
    • Universal Gravitational Acceleration: Near Earth's surface, all bodies experience identical gravitational acceleration regardless of mass, geometry, or composition:     g=9.81 m/s2 downwardg = 9.81\,\text{m/s}^2\text{ downward}
    • Kinematics at Apex: At the highest point of an upward trajectory, instantaneous vertical velocity equals zero (v=0 m/sv = 0\,\text{m/s}). However, acceleration remains non-zero and continues acting downward (a=−9.81 m/s2a = -9.81\,\text{m/s}^2).
    • Application of Equations: Constant-acceleration kinematic equations apply directly by replacing the general acceleration aa with the signed value of gravitational acceleration (+9.81 m/s2+9.81\,\text{m/s}^2 or −9.81 m/s2-9.81\,\text{m/s}^2 depending on chosen directional signs).
  • Worked Examples and Vertical Trajectory Analysis:

    • Worked Example 5 (Time to Attain Maximum Height):
    • Problem Statement: A toy rocket is launched vertically upward at +25.0 m/s+25.0\,\text{m/s}. Determine the time required to reach its highest point.
    • Known Values: vi=+25.0 m/sv_i = +25.0\,\text{m/s}, vf=0 m/sv_f = 0\,\text{m/s}, a=−9.81 m/s2a = -9.81\,\text{m/s}^2
    • Governing Equation: vf=vi+atv_f = v_i + a t
    • Derivation: 0=25.0+(−9.81)t  ⟹  9.81t=25.00 = 25.0 + (-9.81)t \implies 9.81 t = 25.0
    • Calculation: t=25.09.81=2.55 st = \frac{25.0}{9.81} = 2.55\,\text{s}
    • Final Answer: 2.55 s2.55\,\text{s}
    • Worked Example 6 (Maximum Height Attained):
    • Problem Statement: Using the rocket from Worked Example 5 reaching apex at t=2.55 st = 2.55\,\text{s}, calculate its maximum altitude above the launch point.
    • Known Values: xi=0 mx_i = 0\,\text{m}, vi=+25.0 m/sv_i = +25.0\,\text{m/s}, a=−9.81 m/s2a = -9.81\,\text{m/s}^2, t=2.55 st = 2.55\,\text{s}
    • Governing Equation: xf=xi+vit+12at2x_f = x_i + v_i t + \frac{1}{2} a t^2
    • Substitution: xf=0+(25.0)(2.55)+12(−9.81)(2.55)2x_f = 0 + (25.0)(2.55) + \frac{1}{2}(-9.81)(2.55)^2
    • Calculation: xf=63.75−31.895=63.8−31.9=+31.9 mx_f = 63.75 - 31.895 = 63.8 - 31.9 = +31.9\,\text{m}
    • Final Answer: +31.9 m+31.9\,\text{m}
    • Practice Set A, Question 1 (Thrown Ball Height After Fixed Duration):
    • Problem Statement: A ball is thrown straight upward with an initial velocity of 10.0 m/s10.0\,\text{m/s}. Determine its height after 2.0 s2.0\,\text{s}.
    • Coordinate Convention: Establish upward as positive; a=−9.81 m/s2a = -9.81\,\text{m/s}^2
    • Method: Apply xf=vit+12at2x_f = v_i t + \frac{1}{2} a t^2
    • Calculation: xf=(10.0)(2.0)+12(−9.81)(2.0)2=20.0−19.62=+0.38 mx_f = (10.0)(2.0) + \frac{1}{2}(-9.81)(2.0)^2 = 20.0 - 19.62 = +0.38\,\text{m}
    • Final Answer: +0.38 m+0.38\,\text{m}
    • Practice Set A, Question 2 (Rocket Height After Fixed Duration):
    • Problem Statement: A toy rocket is launched straight upward at 35.0 m/s35.0\,\text{m/s}. Find its height after 3.0 s3.0\,\text{s}.
    • Coordinate Convention: Upward positive, a=−9.81 m/s2a = -9.81\,\text{m/s}^2
    • Method: Apply xf=vit+12at2x_f = v_i t + \frac{1}{2} a t^2
    • Calculation: xf=(35.0)(3.0)+12(−9.81)(3.0)2=105.0−44.145=60.855 mx_f = (35.0)(3.0) + \frac{1}{2}(-9.81)(3.0)^2 = 105.0 - 44.145 = 60.855\,\text{m}
    • Final Answer: +60.9 m+60.9\,\text{m}
    • Worked Example 7 (Velocity at a Specified Elevation):
    • Problem Statement: A toy rocket is launched vertically from the ground at +25.0 m/s+25.0\,\text{m/s}. Calculate its velocity when it is 30.0 m30.0\,\text{m} above the ground.
    • Known Values: xi=0 mx_i = 0\,\text{m}, xf=+30.0 mx_f = +30.0\,\text{m}, vi=+25.0 m/sv_i = +25.0\,\text{m/s}, a=−9.81 m/s2a = -9.81\,\text{m/s}^2
    • Governing Equation: vf2=vi2+2a(xf−xi)v_f^2 = v_i^2 + 2 a (x_f - x_i)
    • Substitution: vf2=(25.0)2+2(−9.81)(30.0)=625−588.6=36.4v_f^2 = (25.0)^2 + 2(-9.81)(30.0) = 625 - 588.6 = 36.4
    • Root Extraction and Sign Resolution: vf=±36.4=±6.03 m/sv_f = \pm \sqrt{36.4} = \pm 6.03\,\text{m/s}
    • Physical Distinction: The positive root represents ascending motion (+6.03 m/s+6.03\,\text{m/s}, upward); the negative root represents descending motion (−6.03 m/s-6.03\,\text{m/s}, downward).
    • Final Answer: +6.03 m/s+6.03\,\text{m/s}
    • Practice Set B, Question 4 (Rocket Velocity at Lower Elevation):
    • Problem Statement: A toy rocket is launched straight upward at 35.0 m/s35.0\,\text{m/s}. Determine its velocity when it reaches a height of 10.0 m10.0\,\text{m}.
    • Method: Use vf2=vi2+2aΔxv_f^2 = v_i^2 + 2 a \Delta x
    • Calculation: vf2=(35.0)2+2(−9.81)(10.0)=1225−196.2=1028.8v_f^2 = (35.0)^2 + 2(-9.81)(10.0) = 1225 - 196.2 = 1028.8
    • Root Extraction: vf=±1028.8=±32.1 m/sv_f = \pm \sqrt{1028.8} = \pm 32.1\,\text{m/s}
    • Final Answer: +32.1 m/s+32.1\,\text{m/s}

Cumulative Free Fall Review and Master Kinematic Reference

  • Cumulative Multi-Point Trajectory Analysis:

    • Problem Context: A ball is launched vertically upward from ground level (y0=0 my_0 = 0\,\text{m}) with an initial velocity vi=5.0 m/sv_i = 5.0\,\text{m/s}. Acceleration due to gravity is downward (a=−9.81 m/s2a = -9.81\,\text{m/s}^2). Its height is recorded at 0.1 s0.1\,\text{s}, 0.2 s0.2\,\text{s}, 0.5 s0.5\,\text{s}, 0.75 s0.75\,\text{s}, and 1.0 s1.0\,\text{s}.
    • Analytical Formula:y(t)=vit+12at2=5.0t−4.905t2y(t) = v_i t + \frac{1}{2} a t^2 = 5.0 t - 4.905 t^2
    • Calculated Altitudes:
    • At t=0.1 st = 0.1\,\text{s}: y(0.1)=5.0(0.1)−4.905(0.1)2=0.500−0.04905=0.45095 m≈0.451 my(0.1) = 5.0(0.1) - 4.905(0.1)^2 = 0.500 - 0.04905 = 0.45095\,\text{m} \approx 0.451\,\text{m}
    • At t=0.2 st = 0.2\,\text{s}: y(0.2)=5.0(0.2)−4.905(0.2)2=1.000−0.1962=0.8038 m≈0.804 my(0.2) = 5.0(0.2) - 4.905(0.2)^2 = 1.000 - 0.1962 = 0.8038\,\text{m} \approx 0.804\,\text{m}
    • At t=0.5 st = 0.5\,\text{s}: y(0.5)=5.0(0.5)−4.905(0.5)2=2.500−1.22625=1.27375 m≈1.274 my(0.5) = 5.0(0.5) - 4.905(0.5)^2 = 2.500 - 1.22625 = 1.27375\,\text{m} \approx 1.274\,\text{m}
    • At t=0.75 st = 0.75\,\text{s}: y(0.75)=5.0(0.75)−4.905(0.75)2=3.750−2.75906=0.99094 m≈0.991 my(0.75) = 5.0(0.75) - 4.905(0.75)^2 = 3.750 - 2.75906 = 0.99094\,\text{m} \approx 0.991\,\text{m}
    • At t=1.0 st = 1.0\,\text{s}: y(1.0)=5.0(1.0)−4.905(1.0)2=5.000−4.905=0.095 my(1.0) = 5.0(1.0) - 4.905(1.0)^2 = 5.000 - 4.905 = 0.095\,\text{m}
    • Height Comparison and Chronological Ordering:
    • Comparing calculated magnitudes: 0.095 m<0.451 m<0.804 m<0.991 m<1.274 m0.095\,\text{m} < 0.451\,\text{m} < 0.804\,\text{m} < 0.991\,\text{m} < 1.274\,\text{m}
    • Corresponding time values arranged from least height to greatest height: 1.0 s1.0\,\text{s}, 0.1 s0.1\,\text{s}, 0.2 s0.2\,\text{s}, 0.75 s0.75\,\text{s}, 0.5 s0.5\,\text{s}
  • Master Equation Reference and Application Matrix:

    • Average Speed:speed=distancetime\text{speed} = \frac{\text{distance}}{\text{time}}Condition: Scalar calculation of distance rate.
    • Average Velocity:vavg=ΔxΔtv_{\text{avg}} = \frac{\Delta x}{\Delta t}Condition: Vector displacement divided by elapsed time.
    • Average Acceleration:aavg=ΔvΔta_{\text{avg}} = \frac{\Delta v}{\Delta t}Condition: Rate of velocity change over an elapsed interval.
    • Velocity-Time Relation:vf=vi+atv_f = v_i + a tCondition: Connects velocity and time when position/displacement is omitted.
    • Position via Average Velocity:xf=xi+12(vi+vf)tx_f = x_i + \frac{1}{2}(v_i + v_f) tCondition: Position determined when both initial and final velocities are known.
    • Position-Time-Acceleration Relation:xf=xi+vit+12at2x_f = x_i + v_i t + \frac{1}{2} a t^2Condition: Connects position, elapsed time, and acceleration when final velocity is omitted.
    • Velocity-Displacement Relation:vf2=vi2+2aΔxv_f^2 = v_i^2 + 2 a \Delta xCondition: Connects velocities, acceleration, and displacement when time is omitted.
    • Earth Gravitational Acceleration Constant:g=9.81 m/s2 downwardg = 9.81\,\text{m/s}^2\text{ downward}Condition: Near-surface free fall ignoring atmospheric drag.