General Physics 1: Motion Descriptors and Uniformly Accelerated Linear Motion Notes

Introduction to Motion and Motion Descriptors

Motion is a fundamental concept in physics, specifically within the study of kinematics.

  • Definition of Motion: Motion is defined as the change of position of an object in a specific span of time relative to an observer. To identify if an object is moving, one must observe its position compared to a reference point over a duration of time.
  • Essential Components of Motion:
    • Position: The specific location of an object. To measure motion, we track the initial position (x0x_0) and the final position (xfx_f).
    • Time: The duration during which the change in position occurs (tt).

Detailed Motion Descriptors

There are six primary descriptors used to quantify and qualify the motion of an object.

Time

  • Definition: A quantity that describes when an event took place. It is a necessary parameter to observe changes in a specific space.
  • Symbol: tt
  • SI Unit: seconds (ss)

Distance and Displacement

Distance and displacement both measure how far an object has moved, but they differ in their nature as scalar or vector quantities.

  • Distance:

    • Definition: Describes the total length traveled by an object in motion. It accounts for the entire path taken.
    • Type of Quantity: Scalar (magnitude only).
    • Symbol: xx, yy, zz, or dd
    • SI Unit: meters (mm)
    • Formula: d=xnd = \sum |x_n| (Total length travelled).
  • Displacement:

    • Definition: The length and direction of the straight line that connects the initial position to the final position. It describes how far an object is from its starting point.
    • Type of Quantity: Vector (magnitude and direction).
    • Symbol: Δx\Delta x, Δy\Delta y, Δz\Delta z, or d\vec{d}
    • SI Unit: meters (mm)
    • Formula: Δx=xfxi\Delta x = x_f - x_i
  • Relationship: Distance is always greater than or equal to displacement (dΔxd \ge |\Delta x|). They are equal only if the object travels in a single straight line without reversing direction.

Speed and Velocity

These quantities combine the concepts of space (displacement/distance) and time.

  • Speed:

    • Definition: The rate of change in position; how fast an object is changing its position within a span of time.
    • Type of Quantity: Scalar.
    • Symbol: vv or ss
    • SI Unit: meters per second (m/sm/s or ms1m\,s^{-1}
    • Formula: v=dtv = \frac{d}{t}
  • Velocity:

    • Definition: The rate of change in position with respect to a reference point and direction.
    • Type of Quantity: Vector.
    • Symbol: v\vec{v}
    • SI Unit: meters per second (m/sm/s)
    • Formula: v=Δxt\vec{v} = \frac{\Delta x}{t}

Acceleration

  • Definition: The rate of change in the velocity of an object.
  • Criteria for Acceleration: An object is accelerating if:
    1. The magnitude of the velocity changes (speeding up or slowing down).
    2. The direction of motion changes.
    3. Both the magnitude and the direction of the velocity change.
  • Type of Quantity: Vector.
  • SI Unit: meters per second squared (m/s2m/s^2
  • Formula: a=vfvita = \frac{v_f - v_i}{t}
Signs of Acceleration
  • Positive Acceleration: The acceleration (aa) and velocity (vv) are in the same direction. The object is speeding up.
  • Negative Acceleration (Deceleration): The acceleration (aa) and velocity (vv) are in opposite directions. The object is slowing down.
  • Zero Acceleration: The object is either at rest or traveling at a constant velocity.

Uniform Acceleration and Kinematic Equations

Uniform acceleration occurs when the velocity of an object changes at a fixed rate throughout the motion.

Constant Velocity vs. Constant Acceleration

  • Constant Velocity: The object has a constant magnitude and direction. It covers equal displacements in equal time intervals.
  • Constant Acceleration: The velocity is not constant, but the rate of change of velocity is constant.

The Four Kinematic Equations (Constant Acceleration Equations - CAE)

These equations are used to solve for unknown variables in one-dimensional uniformly accelerated motion. Each equation is independent of one specific motion descriptor.

  1. Displacement-Independent Equation:     v=v0+atv = v_0 + at

  2. Acceleration-Independent Equation:     Δx=v+v02t\Delta x = \frac{v + v_0}{2} t

  3. Final Velocity-Independent Equation:     Δx=v0t+12at2\Delta x = v_0 t + \frac{1}{2} a t^2

  4. Time-Independent Equation:     v2=v02+2aΔxv^2 = v_0^2 + 2 a \Delta x

Where:

  • vv = final velocity
  • v0v_0 = initial velocity
  • aa = acceleration
  • tt = elapsed time
  • Δx\Delta x = displacement (xx0x - x_0

Problem-Solving Strategies

To convert verbal descriptions of motion into mathematical equations, follow these steps:

  1. Read the problem carefully.
  2. Identify Given Values: List all known variables (v,v0,a,t,Δxv, v_0, a, t, \Delta x).
  3. Identify the Unknown: Write what variable is being asked for.
  4. Select the Equation: Choose the kinematic equation that contains the given values and the unknown variable.
  5. Watch for Implicit Givens: Phrases like "starts from rest" imply v0=0m/sv_0 = 0\,m/s. Phrases like "comes to a stop" imply v=0m/sv = 0\,m/s.
  6. Unit Consistency: Ensure all units match (e.g., all in meters and seconds) before calculation.

Examples and Applications

Example 1: Calculating Acceleration

A car uniformly accelerates from rest to reach a maximum velocity of 16.67m/s16.67\,m/s in 10s10\,s.

  • Given: v0=0v_0 = 0, v=16.67m/sv = 16.67\,m/s, t=10st = 10\,s
  • Formula: a=vv0ta = \frac{v - v_0}{t}
  • Solution: a=16.67m/s0m/s10s=1.667m/s2a = \frac{16.67\,m/s - 0\,m/s}{10\,s} = 1.667\,m/s^2
  • (Note: The transcript result says 2m/s22\,m/s^2 likely as a rounded instructional placeholder, but the calculated value based on given numbers is 1.667m/s21.667\,m/s^2).

Example 2: Calculating Distance (Acceleration-Independent)

A ball rolled at a speed of 20m/s20\,m/s and changed its speed to 3m/s3\,m/s in 8s8\,s. What is the distance?

  • Given: v0=20m/sv_0 = 20\,m/s, v=3m/sv = 3\,m/s, t=8st = 8\,s
  • Formula: Δx=v+v02t\Delta x = \frac{v + v_0}{2} t
  • Solution: Δx=3m/s+20m/s2×8s=11.5m/s×8s=92m\Delta x = \frac{3\,m/s + 20\,m/s}{2} \times 8\,s = 11.5\,m/s \times 8\,s = 92\,m

Example 3: Constant Acceleration involving Maria

Maria rides her bicycle at an initial speed of 2m/s2\,m/s. She accelerates at 1m/s21\,m/s^2 for 4s4\,s. How far did she travel?

  • Given: v0=2m/sv_0 = 2\,m/s, a=1m/s2a = 1\,m/s^2, t=4st = 4\,s
  • Formula: Δx=v0t+12at2\Delta x = v_0 t + \frac{1}{2} a t^2
  • Solution: Δx=(2m/s)(4s)+12(1m/s2)(4s)2=8m+8m=16m\Delta x = (2\,m/s)(4\,s) + \frac{1}{2}(1\,m/s^2)(4\,s)^2 = 8\,m + 8\,m = 16\,m

Example 4: The Boar Problem (Two Unknowns)

A boar runs a distance of 70m70\,m in 6s6\,s. It reaches the second point with a velocity of 15m/s15\,m/s. Calculate the initial velocity and acceleration.

  • Given: Δx=70m\Delta x = 70\,m, t=6st = 6\,s, v=15m/sv = 15\,m/s
  • Step 1: Solve for v0v_0 using Δx=v+v02t\Delta x = \frac{v + v_0}{2} t
    • 70=15+v02×670 = \frac{15 + v_0}{2} \times 6
    • 70=(15+v0)×370 = (15 + v_0) \times 3
    • 23.33=15+v023.33 = 15 + v_0
    • v0=8.33m/sv_0 = 8.33\,m/s
  • Step 2: Solve for aa using v=v0+atv = v_0 + at
    • 15=8.33+a(6)15 = 8.33 + a(6)
    • 6.67=6a6.67 = 6a
    • a=1.11m/s2a = 1.11\,m/s^2

Questions & Discussion

  • Q: How can we say that an object is moving?
    • A: We say an object is moving if its position changes relative to a fixed observer or reference point over a period of time.
  • Q: Can you tell what each person sees in the figure (Relative Nature of Motion)?
    • A: Motion is relative. An observer standing on the ground (Observer A) might see a person (Observer B) inside a moving bus moving at the same speed as the bus. However, another person (Observer C) inside the bus would see Observer B as stationary. This illustrates that motion descriptors depend on the frame of reference.
  • Q: What are the assumptions of the four kinematics equations?
    • A: The primary assumption is that the acceleration is constant (a=constanta = \text{constant}) throughout the entire duration being measured.
  • Q: Practice Problem: A train attempted to stop from 43m/s43\,m/s over a distance of 111m111\,m. What is its acceleration?
    • A: Given v0=43m/sv_0 = 43\,m/s, v=0m/sv = 0\,m/s, Δx=111m\Delta x = 111\,m. Use v2=v02+2aΔxv^2 = v_0^2 + 2 a \Delta x.
    • 02=432+2a(111)0^2 = 43^2 + 2 a (111)
    • 1849=222a-1849 = 222 a
    • a=8.33m/s2a = -8.33\,m/s^2 (Deceleration).