Calculus Notes: Average Velocity, Instantaneous Velocity, and Introduction to Limits

Position, Average Velocity, and the Secant Line

  • Definitions and Formulas:

    • Position Function: Let s(t)s(t) represent the position of an object as a function of time tt.
    • Time Interval: Consider a time interval bounded between two values, denoted as [a,b][a, b].
    • Change in Position (Displacement): Measured by evaluating position at the ending time minus position at the beginning time:     Δs=s(b)s(a)\Delta s = s(b) - s(a)
    • Change in Time:     Δt=ba\Delta t = b - a
    • Average Velocity Formula:     Average Velocity=ΔsΔt=s(b)s(a)ba\text{Average Velocity} = \frac{\Delta s}{\Delta t} = \frac{s(b) - s(a)}{b - a}
  • Geometric Interpretation via Secant Line Slope:

    • Plot the position function s(t)s(t) on a Cartesian coordinate system with time tt on the horizontal axis and position ss on the vertical axis.
    • Identify two points on the graph corresponding to the boundaries of time interval [a,b][a, b]:
    • First point: (a,s(a))(a, s(a))
    • Second point: (b,s(b))(b, s(b))
    • Applying the standard slope formula (change in yy over change in xx) between these two ordered pairs yields:     Slope=s(b)s(a)ba\text{Slope} = \frac{s(b) - s(a)}{b - a}
    • The average velocity over time interval [a,b][a, b] equals the slope of the secant line passing through points (a,s(a))(a, s(a)) and (b,s(b))(b, s(b)).

Instantaneous Velocity and Tangent Lines

  • Distinction Between Velocity Types:

    • Average Velocity: Represents average rate of motion across a extended time interval [a,b][a, b].
    • Instantaneous Velocity: Describes exact velocity at a single specific instant in time t=at = a
  • Approximation via Interval Reduction:

    1. Select a small time interval containing time instant aa.
    2. Calculate average velocity across this initial interval to obtain a rough estimate.
    3. Refine the approximation by choosing progressively smaller time intervals surrounding aa.
    4. As interval width shrinks toward zero, the secant line rotates and approaches the tangent line.
    5. Instantaneous velocity at t=at = a equals the slope of the tangent line to position function s(t)s(t) at point (a,s(a))(a, s(a)).

Questions and Discussion: Theoretical Concept of Instantaneous Change

  • Theoretical Paradox:

    • Question: How can change occur at a single instant of time? Velocity implies movement, which requires elapsed time. At an isolated instant, how can change exist?
  • Metaphor and Clarification:

    • Vehicle Speedometer Metaphor: When driving a car and viewing the speedometer at a specific moment, reading 60miles per hour60\,\text{miles per hour} measures speed at that exact instant.
    • If speed remains constant over the subsequent hour, distance traveled will be 60miles60\,\text{miles}.
    • Velocity continuously fluctuates, yet at every single instant, an object possesses an instantaneous speed due to ongoing motion.

Physics Application: Free-Falling Object (Galileo's Law)

  • Galileo's Law of Falling Bodies:

    • If an object is dropped and falls freely under gravity (ignoring air resistance), distance fallen is directly proportional to time squared:     s(t)=4.9t2s(t) = 4.9 t^2
    • Units: Time tt in seconds (s\text{s}), position s(t)s(t) in meters (m\text{m}).
    • Scenario: Object dropped from top of a 450m450\,\text{m} building.
  • Problem Setup:

    • Determine instantaneous velocity at time t=5st = 5\,\text{s}.
    • Direct derivative calculations are avoided; numerical approximation via shrinking intervals is applied.
  • Sequential Numerical Approximations:

    • Interval 1: [5,5.1][5, 5.1]

    • Ending position: s(5.1)=4.9×5.12=127.449ms(5.1) = 4.9 \times 5.1^2 = 127.449\,\text{m}

    • Beginning position: s(5)=4.9×52=122.5ms(5) = 4.9 \times 5^2 = 122.5\,\text{m}

    • Average velocity:       Average Velocity=s(5.1)s(5)5.15=4.9×5.124.9×520.1=127.449122.50.1=49.49m/s\text{Average Velocity} = \frac{s(5.1) - s(5)}{5.1 - 5} = \frac{4.9 \times 5.1^2 - 4.9 \times 5^2}{0.1} = \frac{127.449 - 122.5}{0.1} = 49.49\,\text{m/s}

    • Interval 2: [5,5.05][5, 5.05]

    • Right endpoint moved closer to 55

    • Average velocity:       Average Velocity=s(5.05)s(5)5.055=4.9×5.0524.9×520.05=124.99225122.50.05=49.245m/s\text{Average Velocity} = \frac{s(5.05) - s(5)}{5.05 - 5} = \frac{4.9 \times 5.05^2 - 4.9 \times 5^2}{0.05} = \frac{124.99225 - 122.5}{0.05} = 49.245\,\text{m/s}

    • Interval 3: [5,5.01][5, 5.01]

    • Right endpoint shifted to 5.015.01

    • Average velocity = 49.049m/s49.049\,\text{m/s}

    • Interval 4: [5,5.001][5, 5.001]

    • Right endpoint shifted to 5.0015.001

    • Average velocity = 49.0049m/s49.0049\,\text{m/s}

  • Tabulated Trend Analysis:

    • Interval [5,5.1][5, 5.1]: 49.49m/s49.49\,\text{m/s}
    • Interval [5,5.05][5, 5.05]: 49.245m/s49.245\,\text{m/s}
    • Interval [5,5.01][5, 5.01]: 49.049m/s49.049\,\text{m/s}
    • Interval [5,5.001][5, 5.001]: 49.0049m/s49.0049\,\text{m/s}
    • Convergence Target: As interval size approaches zero, average velocities converge toward 49m/s49\,\text{m/s}.
    • Instantaneous velocity at t=5st = 5\,\text{s} equals 49m/s49\,\text{m/s}.

Section 2.2: The Limit of a Function

  • Theoretical Foundation:

    • Limit concept focuses on function behavior as input variable xx approaches target value aa without reaching aa
    • Notation:     limxaf(x)=L\lim_{x \to a} f(x) = L
  • Example 1: Simple Continuous Linear Function

    • Function: f(x)=2xf(x) = 2x
    • Target Input: x3x \to 3
    • Approaching x=3x = 3 from the Left (x<3x < 3):
    • x=2    f(2)=4x = 2 \implies f(2) = 4
    • x=2.5    f(2.5)=5x = 2.5 \implies f(2.5) = 5
    • x=2.9    f(2.9)=5.8x = 2.9 \implies f(2.9) = 5.8
    • x=2.99    f(2.99)=5.98x = 2.99 \implies f(2.99) = 5.98
    • x=2.999    f(2.999)=5.998x = 2.999 \implies f(2.999) = 5.998
    • Numerical trend approaches 66
    • Approaching x=3x = 3 from the Right (x>3x > 3):
    • x=4    f(4)=8x = 4 \implies f(4) = 8
    • x=3.5    f(3.5)=7x = 3.5 \implies f(3.5) = 7
    • x=3.1    f(3.1)=6.2x = 3.1 \implies f(3.1) = 6.2
    • x=3.01    f(3.01)=6.02x = 3.01 \implies f(3.01) = 6.02
    • x=3.001    f(3.001)=6.002x = 3.001 \implies f(3.001) = 6.002
    • Numerical trend approaches 66
    • Result:     limx3(2x)=6\lim_{x \to 3} (2x) = 6
    • Geometric Visualization: Straight line graph containing points (0,0)(0,0), (1,2)(1,2), (2,4)(2,4), (3,6)(3,6), (4,8)(4,8), (5,10)(5,10). Moving along the line from either direction approaches point (3,6)(3,6).
  • Example 2: Function Undefined at Target Point

    • Scenario: Function f(x)f(x) where f(2)f(2) does not exist (undefined due to division by zero or structural hole).
    • Evaluating limit as x2x \to 2 using numerical inputs:
    • x=2.5    f(2.5)=0.2222x = 2.5 \implies f(2.5) = 0.2222
    • x=2.1    f(2.1)=0.244x = 2.1 \implies f(2.1) = 0.244
    • x=2.01    f(2.01)=0.249x = 2.01 \implies f(2.01) = 0.249
    • x=2.001    f(2.001)=0.2499x = 2.001 \implies f(2.001) = 0.2499
    • Numerical Trend: Function values approach 0.250.25
    • Limit Value:     limx2f(x)=0.25\lim_{x \to 2} f(x) = 0.25
    • Key Principle: A limit can exist at x=ax = a even when f(a)f(a) is undefined. Limits evaluate neighboring behavior, ignoring exact point values.
  • Example 3: Discontinuous Function with Isolated Point

    • Scenario: Graph featuring an open circle at (a,L)(a, L) and a solid point at (a,M)(a, M).
    • Direct Function Evaluation:     f(a)=Mf(a) = M
    • Limit Evaluation:     limxaf(x)=L\lim_{x \to a} f(x) = L
    • Principle: Disconnections or isolated defined values do not affect limits. The limit remains LL as long as surrounding curves approach LL

One-Sided Limits

  • Right-Sided Limit:

    • Notation:     limxa+f(x)\lim_{x \to a^+} f(x)
    • Definition: Evaluates behavior of f(x)f(x) as xx approaches aa exclusively from values strictly greater than aa (moving from right to left).
  • Left-Sided Limit:

    • Notation:     limxaf(x)\lim_{x \to a^-} f(x)
    • Definition: Evaluates behavior of f(x)f(x) as xx approaches aa exclusively from values strictly less than aa (moving from left to right).
  • Jump Discontinuities:

    • Functions containing vertical jumps at x=ax = a yield distinct left-sided and right-sided limits matching the respective boundaries of each branch.

Position Function: Let s(t)s(t) show where an object is at any time tt.

  • Time Interval: Think of a time period between two points, [a,b][a, b].
  • Change in Position (Displacement): This tells us how much the position has changed from the start to the end of the time period: riangles=s(b)s(a)riangle s = s(b) - s(a).
  • Change in Time: rianglet=bariangle t = b - a.
  • Average Velocity Formula: The average speed of the object during the time period is given by: extAverageVelocity=rianglesrianglet=s(b)s(a)baext{Average Velocity} = \frac{ riangle s}{ riangle t} = \frac{s(b) - s(a)}{b - a}.

Geometric Interpretation via Secant Line Slope:

  • When we plot the position function s(t)s(t) on a graph with time on the horizontal axis and position on the vertical axis, we can see how it moves.
  • We mark the starting point at (a,s(a))(a, s(a)) and the endpoint at (b,s(b))(b, s(b)).
  • The average velocity equals the slope (or steepness) of the line connecting these two points, which is calculated with: extSlope=s(b)s(a)baext{Slope} = \frac{s(b) - s(a)}{b - a}.

Instantaneous Velocity and Tangent Lines:

  • Average Velocity: This is how fast something moves over a period of time, [a,b][a, b].
  • Instantaneous Velocity: This is how fast something is moving at a specific moment in time, at t=at = a.
  • To find instantaneous velocity, we look at smaller and smaller time intervals around aa. As we make the intervals tiny, the average velocity over those intervals gives us the instantaneous speed at that moment.

Questions and Discussion:

  • Theoretical Concept of Instantaneous Change:
    • How can something change at an exact moment? Typically, we think movement needs some time. Can there be change at a single instant?
    • Think of a car speedometer. When you check it, it may show 60extmilesperhour60 ext{ miles per hour}, which tells you the speed right at that moment. If it stays that way, you'll travel 60extmiles60 ext{ miles} in an hour. Although speed changes all the time, at every moment, the car has a speed due to its continuous motion.

Physics Application: Free-Falling Object (Galileo's Law):

  • Galileo's Law of Falling Bodies: If an object falls freely without any air resistance, the distance it falls is related to the time squared: s(t)=4.9t2s(t) = 4.9 t^2.
  • Example Problem: What is the speed of an object after it falls for 5extseconds5 ext{ seconds}? Instead of calculating directly, we can approximate by using smaller intervals.
    • Starting Interval: [5,5.1][5, 5.1]:
      • Find positions at these times:
      • s(5.1)=4.9imes5.12=127.449extms(5.1) = 4.9 imes 5.1^2 = 127.449 ext{ m}
      • s(5)=4.9imes52=122.5extms(5) = 4.9 imes 5^2 = 122.5 ext{ m}
      • Therefore, average velocity = s(5.1)s(5)5.15=127.449122.50.1=49.49extm/s\frac{s(5.1) - s(5)}{5.1 - 5} = \frac{127.449 - 122.5}{0.1} = 49.49 ext{ m/s}.
    • Repeat for smaller intervals, like [5,5.05][5, 5.05], to get more precise velocity readings:
      • Average velocity = 49.245extm/s49.245 ext{ m/s}.
  • As the intervals get very small, the average velocities all get closer to 49extm/s49 ext{ m/s}. That means the exact speed of the object at t=5extsecondst = 5 ext{ seconds} is approximately 49extm/s49 ext{ m/s}.