Single-Variable-Calculus ยท Unit 2 ยท Video 1 ยท Interactive Practice

Twice the Average: The Derivative as a Rate of Change

IKey Formulas

FormulaNameWhat it measures
ฮ”yฮ”x=f(x2)โˆ’f(x1)x2โˆ’x1\dfrac{\Delta y}{\Delta x} = \dfrac{f(x_2) - f(x_1)}{x_2 - x_1}Average rate of changeSlope of the chord across the interval
dydx=limโกฮ”xโ†’0ฮ”yฮ”x\dfrac{dy}{dx} = \displaystyle\lim_{\Delta x \to 0} \dfrac{\Delta y}{\Delta x}Instantaneous rate of changeSlope of the tangent at a single instant
h(t)=80โˆ’5t2h(t) = 80 - 5t^2Pumpkin drop, height in metresh(0)=80h(0) = 80 and h(4)=0h(4) = 0 โ€” a four-second fall
dhdt=โˆ’10t,d2hdt2=โˆ’10\dfrac{dh}{dt} = -10t, \qquad \dfrac{d^2h}{dt^2} = -10Speed and accelerationEach is the rate of change of the one above it

Key Insight: The pumpkin averages โˆ’20-20 m/s over the whole fall but lands with hโ€ฒ(4)=โˆ’40h'(4) = -40 m/s. An average taken over an interval can miss the moment that matters by a factor of two.

IIVisualization 1 โ€” Average Rate of Change Over an Interval

Between any two instants of the fall, one number summarises the motion: the slope of the chord.

๐Ÿ’ก On this parabola the average works out to โˆ’5(t1+t2)-5(t_1 + t_2), so no interval inside the four-second fall can average the โˆ’40-40 m/s the pumpkin reaches at impact.

IIIVisualization 2 โ€” Closing the Window on the Instant

As the averaging window closes on t=4t = 4, the chord slope runs from โˆ’20-20 all the way to โˆ’40-40.

๐Ÿ’ก Two honest footnotes on the model: the real building is a little taller than 8080 m, and h=80โˆ’5t2h = 80 - 5t^2 ignores air resistance.

IVVisualization 3 โ€” Height, Speed, Acceleration

Each graph's slope is the next graph's height, from height down to a constant acceleration.

๐Ÿ’ก Read the chain upward instead and it explains the formula: a constant acceleration of โˆ’10-10 m/sยฒ forces the speed to be linear in tt, which forces the height to be quadratic.

VQuiz Questions

Problem 1 ยท Average Rate on an Interval

Given: the pumpkin's height is h(t)=80โˆ’5t2h(t) = 80 - 5t^2 metres โ€” find the average rate of change of hh over 1โ‰คtโ‰ค21 \le t \le 2.

โœ… Correct! h(1)=75h(1) = 75 and h(2)=60h(2) = 60, so the chord slope is 60โˆ’752โˆ’1=โˆ’15\frac{60 - 75}{2 - 1} = -15 m/s.
โŒ Not quite. Those are the instantaneous speeds at the two endpoints: hโ€ฒ(1)=โˆ’10h'(1) = -10 and hโ€ฒ(2)=โˆ’20h'(2) = -20. An average rate needs the chord, h(2)โˆ’h(1)2โˆ’1\frac{h(2) - h(1)}{2 - 1}, not a tangent.
โŒ Right size, wrong sign. The numerator is final minus initial, h(2)โˆ’h(1)=60โˆ’75=โˆ’15h(2) - h(1) = 60 - 75 = -15, and the pumpkin is falling, so the rate is negative.
Show solution

Evaluate the height at both ends of the interval:

h(1)=80โˆ’5(1)2=75,h(2)=80โˆ’5(2)2=60h(1) = 80 - 5(1)^2 = 75, \qquad h(2) = 80 - 5(2)^2 = 60

Now form the difference quotient over ฮ”t=2โˆ’1=1\Delta t = 2 - 1 = 1:

ฮ”hฮ”t=h(2)โˆ’h(1)2โˆ’1=60โˆ’751=โˆ’15ย m/s\frac{\Delta h}{\Delta t} = \frac{h(2) - h(1)}{2 - 1} = \frac{60 - 75}{1} = -15 \ \mathrm{m/s}

As a check, the general average over [t1,t2][t_1, t_2] for this height is

โˆ’5t22+5t12t2โˆ’t1=โˆ’5(t1+t2),\frac{-5t_2^2 + 5t_1^2}{t_2 - t_1} = -5(t_1 + t_2),

and โˆ’5(1+2)=โˆ’15-5(1 + 2) = -15. Notice it lies between hโ€ฒ(1)=โˆ’10h'(1) = -10 and hโ€ฒ(2)=โˆ’20h'(2) = -20, as an average of a steadily increasing speed must.

Problem 2 ยท Watch the Order of Subtraction

Given: a student computes the pumpkin's average velocity over the whole fall as 80โˆ’04โˆ’0=+20\dfrac{80 - 0}{4 - 0} = +20 m/s, but the correct value is โˆ’20-20 m/s. Which single step is wrong?

โœ… Correct! h(4)โˆ’h(0)4โˆ’0=0โˆ’804=โˆ’20\frac{h(4) - h(0)}{4 - 0} = \frac{0 - 80}{4} = -20 m/s. Writing 80โˆ’080 - 0 on top reverses the change in height and flips the sign.
โŒ That fixes the answer by accident. Reversing the bottom gives 80โˆ’4=โˆ’20\frac{80}{-4} = -20, the right number โ€” but the definition pins the order in both slots at once: h(t2)โˆ’h(t1)t2โˆ’t1\frac{h(t_2) - h(t_1)}{t_2 - t_1}, with the same t2t_2 on top and bottom.
โŒ Not quite. h(4)=80โˆ’5(4)2=0h(4) = 80 - 5(4)^2 = 0 is correct, and 0โ‰คtโ‰ค40 \le t \le 4 really is the whole fall. The error is in the order of subtraction.
Show solution

The average rate of change is defined as

ฮ”hฮ”t=h(t2)โˆ’h(t1)t2โˆ’t1,\frac{\Delta h}{\Delta t} = \frac{h(t_2) - h(t_1)}{t_2 - t_1},

with the later value first in both the numerator and the denominator. Here t1=0t_1 = 0, t2=4t_2 = 4, h(0)=80h(0) = 80 and h(4)=0h(4) = 0:

ฮ”hฮ”t=0โˆ’804โˆ’0=โˆ’804=โˆ’20ย m/s\frac{\Delta h}{\Delta t} = \frac{0 - 80}{4 - 0} = \frac{-80}{4} = -20 \ \mathrm{m/s}

The student wrote h(t1)โˆ’h(t2)h(t_1) - h(t_2) on top while keeping t2โˆ’t1t_2 - t_1 underneath, which negates the whole quotient. The minus sign is not decoration: it records that the height is decreasing, so the pumpkin averages 2020 m/s downward.

Problem 3 ยท A Shorter Drop, End to End

Given: a stone is released from a 4545 m ledge and its height is s(t)=45โˆ’5t2s(t) = 45 - 5t^2 metres, with tt in seconds.

When does it reach the ground?

How fast is it moving at impact?

โœ… Correct! s(t)=0s(t) = 0 at t=3t = 3, and sโ€ฒ(t)=โˆ’10ts'(t) = -10t gives sโ€ฒ(3)=โˆ’30s'(3) = -30 m/s โ€” again exactly twice the โˆ’15-15 m/s average over the fall.
โŒ Check the landing time. Set 45โˆ’5t2=045 - 5t^2 = 0, so 5t2=455t^2 = 45, t2=9t^2 = 9 and t=3t = 3 s.
โŒ Check the impact speed. Differentiate first โ€” sโ€ฒ(t)=โˆ’10ts'(t) = -10t โ€” and only then substitute the landing time.
โŒ That is the average, not the instant. s(3)โˆ’s(0)3โˆ’0=0โˆ’453=โˆ’15\frac{s(3) - s(0)}{3 - 0} = \frac{0 - 45}{3} = -15 m/s is the chord slope over the whole fall; the impact speed is the tangent slope at t=3t = 3.
Show solution

Step 1 โ€” landing time. The stone is on the ground when s(t)=0s(t) = 0:

45โˆ’5t2=0โ€…โ€ŠโŸนโ€…โ€Št2=9โ€…โ€ŠโŸนโ€…โ€Št=3ย s45 - 5t^2 = 0 \;\Longrightarrow\; t^2 = 9 \;\Longrightarrow\; t = 3 \ \mathrm{s}

(The root t=โˆ’3t = -3 is before the release.)

Step 2 โ€” impact speed. Differentiate, using ddt(45)=0\frac{d}{dt}(45) = 0 and ddtt2=2t\frac{d}{dt}t^2 = 2t:

dsdt=โˆ’5โ‹…2t=โˆ’10tโŸนsโ€ฒ(3)=โˆ’10(3)=โˆ’30ย m/s\frac{ds}{dt} = -5 \cdot 2t = -10t \qquad\Longrightarrow\qquad s'(3) = -10(3) = -30 \ \mathrm{m/s}

Compare with the average.

ฮ”sฮ”t=0โˆ’453โˆ’0=โˆ’15ย m/s\frac{\Delta s}{\Delta t} = \frac{0 - 45}{3 - 0} = -15 \ \mathrm{m/s}

The impact speed is twice the average again โ€” that factor of two is not special to 8080 m, it is what a quadratic height with a start from rest always produces.

Problem 4 ยท From Charge to Current

Given: the charge on a plate is q(t)=3t2+1tq(t) = 3t^2 + \dfrac{1}{t} coulombs and the current is i=dqdti = \dfrac{dq}{dt} โ€” find the current at t=1t = 1 s.

โœ… Correct! ddt(3t2)=6t\frac{d}{dt}(3t^2) = 6t and ddttโˆ’1=โˆ’tโˆ’2\frac{d}{dt}t^{-1} = -t^{-2}, so i(t)=6tโˆ’1t2i(t) = 6t - \frac{1}{t^2} and i(1)=6โˆ’1=5i(1) = 6 - 1 = 5 A.
โŒ Check the sign of the second term. The power rule at n=โˆ’1n = -1 gives (โˆ’1)tโˆ’2=โˆ’1t2(-1)t^{-2} = -\frac{1}{t^2}, so that term is subtracted: 6โˆ’1=56 - 1 = 5, not 6+16 + 1.
โŒ The 1t\frac{1}{t} term is not constant. Its derivative is โˆ’1t2-\frac{1}{t^2}, which contributes โˆ’1-1 at t=1t = 1.
โŒ Not quite. Differentiate term by term with the power rule: 3t2โ†’6t3t^2 \to 6t and tโˆ’1โ†’โˆ’tโˆ’2t^{-1} \to -t^{-2}, then set t=1t = 1.
Show solution

Current is the rate of change of charge, so the whole problem is one derivative. Write the second term as a power:

q(t)=3t2+tโˆ’1q(t) = 3t^2 + t^{-1}

The power rule ddttn=ntโ€‰nโˆ’1\frac{d}{dt}t^n = nt^{\,n-1} was proved for n=1,2,3,โ€ฆn = 1, 2, 3, \dots, but it also holds at n=โˆ’1n = -1 โ€” that is exactly the rule ddt1t=โˆ’1t2\frac{d}{dt}\frac{1}{t} = -\frac{1}{t^2} obtained straight from the limit definition:

dqdt=3(2t)+(โˆ’1)tโˆ’2=6tโˆ’1t2\frac{dq}{dt} = 3(2t) + (-1)t^{-2} = 6t - \frac{1}{t^2}

Evaluate at t=1t = 1:

i(1)=6(1)โˆ’112=6โˆ’1=5ย Ai(1) = 6(1) - \frac{1}{1^2} = 6 - 1 = 5 \ \mathrm{A}

Same derivative, new reading: with qq in coulombs and tt in seconds, dq/dtdq/dt comes out in coulombs per second โ€” amperes.

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