michael.nestel.me/math/ap-calculus-ab/ball

Is the ball ever stopped?

For teachers & tutors

Is the Ball Ever Stopped?

A pop-up fly hangs at the top of its arc. Average velocity, instantaneous velocity, and the limit that connects them.

CED topics

  • 1.1 Introducing Calculus: Can Change Occur at an Instant?
  • 2.1 Defining Average and Instantaneous Rates of Change at a Point
  • 2.2 Defining the Derivative of a Function and Using Derivative Notation
  • 2.3 Estimating Derivatives of a Function at a Point

Individual problems also preview:

  • 5.1 Using the Mean Value Theorem

Big idea and practices

Big idea: rate of change at an instant, the limit of average rates over shrinking intervals: the derivative, the tangent slope. CED: CHA-1, CHA-2; the calculator item previews the Mean Value Theorem (FUN-1, topic 5.1).

Practices: 1.D, 1.E (difference quotients, the limit definition, table estimates); 2.B (graph, table, formula); 3.E (the velocity's sign just before and just after 2.5 seconds); 4.B, 4.C (units; f′(a){f'(a)}, dhdt{\frac{dh}{dt}}, limit notation).

45-minute plan

  1. 0–5 minRead both hooks; pairs read "Is it stopped?" together and pick in it (or circle on the printout). Vote: stopped at the top?
  2. 5–10 minChallenge 1 in pairs. Units before the number.
  3. 10–18 minSecant explorable and its three prompts, then Challenge 2.
  4. 18–26 minWhole class: difference quotient, limit, f′(a){f'(a)} as tangent slope; h{h} versus Δt{\Delta t}; tangent explorable.
  5. 26–34 minPairs read the worked example thread together, then Challenge 3.
  6. 34–40 minChallenge 4 with calculators, then the reveal.
  7. 40–45 minExit ticket and reflection.

Pairs read each thread together; at each question, both answer before tapping Next.

Homework: the fluency set. Review Fluency 6, the AP form, next class.

Launch questions

  • A pop-up hangs at the top. Stopped? For how long?
  • Speed is distance over time. At one instant, what distance, over what time?
  • 30 miles in 45 minutes: your speed at minute 20?
  • Up and back down: is the average velocity zero? Does where it lands matter?

Misconceptions and how to respond

  • “Stopped means stopped for a while.” Velocity drops by 32 ft/s every second; v=0{v = 0} only for an instant. Drag the tangent explorable through 2.5 seconds.
  • Averaging heights. Watch for 86 on Challenge 1. Ask for units.
  • Last row as answer. Watch for 15.984 on Challenge 2, the average on [2,2.001]{[2, 2.001]}; they go to 16, which no row equals.
  • Plugging in 0 first gives 0/0{0/0}. Expand, subtract, divide, then take the limit; Fluency 6 gives feedback on this.
  • Trip average. Watch for 14 on Challenge 3: 56 feet in 4 seconds, not the reading at 4 seconds.
  • “It comes back down, so the average is zero.” Watch for 2.5 on Challenge 4, right only for a catch at bat height. Landing 6 feet lower puts the answer past the peak.
  • Rounding early. Watch for 2.535 on Challenge 4: 5.07 ÷ 2. Keep four decimals in T{T}.
  • Averaging from 0. Watch for 30 on the exit ticket, the average over the first 5 seconds.

Support and extension

Support

  • Table the height at 0 through 5 seconds, 6, 70, 102, 102, 70, and 6 feet, and the average velocities between, 64, 32, 0, −32, and −64 ft/s. Where does the sign flip?
  • Units before every quotient.
  • Board expand, subtract, divide for the first limit; erase it for the next.
  • Pairs: one runs the explorable, one records readouts and predicts the next.

Extension

  • For h(t)=at2+bt+c{h(t) = at^2 + bt + c}, show the average velocity on [p,q]{[p, q]} is h′ ⁣(p+q2){h'\!\left(\frac{p + q}{2}\right)}. Why is Challenge 4's answer exactly half the landing time?
  • Why does averaging over [2−Δt,2+Δt]{[2 - \Delta t, 2 + \Delta t]} give exactly 16 for every Δt{\Delta t}? What does that say about centered table estimates?
  • Back at its starting height at 5 seconds, falling at 80 ft/s, its launch speed: why? Use symmetry and v(t)=80−32t{v(t) = 80 - 32t}.
  • Why is the landing speed more than 80 ft/s? (8106≈82.365{8\sqrt{106} \approx 82.365} ft/s: it falls 6 feet farther than it rose.)

Without devices

  • Print the lesson page as the handout. Students circle their predictions.
  • Secant: board the averages on [2,2+width]{[2, 2 + \text{width}]} for widths of 1, 0.5, 0.2, 0.1, 0.05, 0.02, 0.01, 0.005, 0.002, and 0.001 s, in order: 0, 8, 12.8, 14.4, 15.2, 15.68, 15.84, 15.92, 15.968, and 15.984 ft/s. What do they approach? Prove it with Challenge 2.
  • Tangent: sketch the parabola from the support table; lay a ruler along it at 1, 2.5, and 4 seconds.
  • Grade with the answer key below.
  • Collect the exit ticket on paper.

Answer key

Every problem in the order the lesson gives them, with the answer the page accepts and my full write-up. Answer boxes check only the final number, so ask students for their work.

  1. Challenge 1

    No calculator · CED 1.1, 2.1

    A pop-up's height after t{t} seconds is h(t)=6+80t−16t2{h(t) = {6 + 80t - 16t^2}} feet. Find its average velocity from t=1{t = 1} to t=2{t = 2} seconds.

    Answer: 32

    1. Average velocity: h(2)−h(1)2−1{\dfrac{h(2) - h(1)}{2 - 1}}.
    2. Heights, in feet: h(1)=6+80−16\displaystyle h(1) = 6 + 80 - 16=70\displaystyle = 70h(2)=6+160−64\displaystyle h(2) = 6 + 160 - 64=102\displaystyle = 102
    3. 102−702−1=32{\dfrac{102 - 70}{2 - 1} = \boxed{32}}: the ball rises 32 feet in that second, an average velocity of 32 ft/s.

    Common wrong answers

    • 86: That's the average height, not change in height over change in time.
    • 48: That's the average from t = 0 to t = 2. Start at t = 1.
    • -32: Same order on top and bottom: h(2) − h(1) over 2 − 1.
    • 102: That's the height at t = 2, not a velocity.
  2. Challenge 2

    No calculator · CED 1.1, 2.1, 2.2

    Same ball: h(t)=6+80t−16t2{h(t) = {6 + 80t - 16t^2}} feet after t{t} seconds. Its average velocity on [2,2+Δt]{[2, 2 + \Delta t]} as Δt{\Delta t} shrinks: Δt (s)average velocity (ft/s)100.114.40.0115.840.00115.984\begin{array}{c|c} \Delta t \text{ (s)} & \text{average velocity (ft/s)} \\ \hline 1 & 0 \\ 0.1 & 14.4 \\ 0.01 & 15.84 \\ 0.001 & 15.984 \end{array} Use the limit definition to find v(2){v(2)}, the velocity at t=2{t = 2} seconds: limΔt→0⁡h(2+Δt)−h(2)Δt{\displaystyle\lim_{\Delta t \to 0} \frac{h(2 + \Delta t) - h(2)}{\Delta t}}

    Answer: 16

    1. h(2)=6+160−64=102{h(2) = 6 + 160 - 64 = 102}.
    2. Expand h(2+Δt){h(2 + \Delta t)}: h(2+Δt)=6+80(2+Δt)−16(2+Δt)2\displaystyle h(2 + \Delta t) = 6 + 80(2 + \Delta t) - 16(2 + \Delta t)^2put in 2+Δt{2 + \Delta t} for t{t}=6+160+80Δt−64−64Δt−16(Δt)2\displaystyle = 6 + 160 + 80\Delta t - 64 - 64\Delta t - 16(\Delta t)^2multiply out=102+16Δt−16(Δt)2\displaystyle = 102 + 16\Delta t - 16(\Delta t)^2combine like terms
    3. Subtract h(2)=102{h(2) = 102}, divide by Δt{\Delta t}, and factor it out of the top; since Δt≠0{\Delta t \ne 0}, it cancels: h(2+Δt)−h(2)=16Δt−16(Δt)2\displaystyle h(2 + \Delta t) - h(2) = 16\Delta t - 16(\Delta t)^2Δt(16−16Δt)Δt=16−16Δt\displaystyle \frac{\cancel{\Delta t}(16 - 16\Delta t)}{\cancel{\Delta t}} = 16 - 16\Delta t Check: Δt=0.001{\Delta t = 0.001} gives 15.984{15.984}, the table's last row.
    4. As Δt→0{\Delta t \to 0}, 16−16Δt→16{16 - 16\Delta t \to \boxed{16}}: at t=2{t = 2} the ball rises at 16 ft/s.

    Common wrong answers

    • 15.984: That's the average on [2, 2.001]. Find the number the averages approach.
    • 102: That's the height at t = 2, not a velocity.
    • 0: That's the average on [2, 3]. Let Δt shrink toward 0.
    • 32: That's the average on [1, 2]. Find the velocity at the instant t = 2.
  3. Worked example

    No calculator · CED 2.2

    The pop-up's height is h(t)=6+80t−16t2{h(t) = {6 + 80t - 16t^2}} feet after t{t} seconds, from bat to landing. Use the limit definition to find its velocity v(t){v(t)}. Then: is the ball ever stopped, and if so, at what time?

    Worked on the page: 2.5

    1. Start from the limit definition: the velocity v(t){\teal{v(t)}} is the limit of the average velocity h(t+Δt)−h(t)Δt{\orange{\dfrac{h(t + \Delta t) - h(t)}{\Delta t}}} as Δt→0{\Delta t \to 0}.
    2. Expand h(t+Δt){h(t + \Delta t)}: h(t+Δt)=6+80(t+Δt)−16(t+Δt)2\displaystyle h(t + \Delta t) = 6 + 80(t + \Delta t) - 16(t + \Delta t)^2put in t+Δt{t + \Delta t} for t{t}=6+80t+80Δt−16t2−32tΔt−16(Δt)2\displaystyle = 6 + 80t + 80\Delta t - 16t^2 - 32t\Delta t - 16(\Delta t)^2multiply out
    3. Subtract h(t)=6+80t−16t2{h(t) = 6 + 80t - 16t^2}. Every term without a Δt{\Delta t} cancels: h(t+Δt)−h(t)=6+80t+80Δt−16t2−32tΔt−16(Δt)2−6−80t+16t2\displaystyle h(t + \Delta t) - h(t) = \cancel{6} + \cancel{80t} + 80\Delta t - \cancel{16t^2} - 32t\Delta t - 16(\Delta t)^2 - \cancel{6} - \cancel{80t} + \cancel{16t^2}subtract each term=80Δt−32tΔt−16(Δt)2\displaystyle = 80\Delta t - 32t\Delta t - 16(\Delta t)^2
    4. Divide by Δt{\Delta t} for the average velocity, then let Δt→0{\Delta t \to 0} for the velocity: h(t+Δt)−h(t)Δt=80−32t−16Δt\displaystyle \orange{\frac{h(t + \Delta t) - h(t)}{\Delta t}} = 80 - 32t - 16\Delta tΔt≠0{\Delta t \ne 0}v(t)=80−32t\displaystyle \teal{v(t)} = \teal{80 - 32t}let Δt→0{\Delta t \to 0} So v(t)=80−32t{v(t) = 80 - 32t} ft/s. Check: v(2)=80−64=16{v(2) = 80 - 64 = 16}, as in Challenge 2.
    5. Stopped means v(t)=0{v(t) = 0}: 80−32t=0\displaystyle 80 - 32t = 0t=2.5\displaystyle t = \boxed{2.5} Yes, at the top, 2.5 s, but only for an instant: v>0{v > 0} just before and v<0{v < 0} just after.
  4. Challenge 3

    No calculator · CED 2.1, 2.2

    A car leaving a parking lot has gone s(t)=3t2+2t{s(t) = 3t^2 + 2t} feet after t{t} seconds, for 0≤t≤10{0 \le t \le 10}. What does its speedometer read at t=4{t = 4} seconds, in feet per second? It only moves forward, so the reading is its velocity, limΔt→0⁡s(4+Δt)−s(4)Δt{\displaystyle\lim_{\Delta t \to 0} \frac{s(4 + \Delta t) - s(4)}{\Delta t}}. Step one, done for you: s(4+Δt)=3(4+Δt)2+2(4+Δt)\displaystyle s(4 + \Delta t) = 3(4 + \Delta t)^2 + 2(4 + \Delta t)=56+26Δt+3(Δt)2\displaystyle = 56 + 26\Delta t + 3(\Delta t)^2

    Answer: 26

    1. Done for you: s(4+Δt)=3(4+Δt)2+2(4+Δt)\displaystyle s(4 + \Delta t) = 3(4 + \Delta t)^2 + 2(4 + \Delta t)=48+24Δt+3(Δt)2+8+2Δt\displaystyle = 48 + 24\Delta t + 3(\Delta t)^2 + 8 + 2\Delta tmultiply out=56+26Δt+3(Δt)2\displaystyle = 56 + 26\Delta t + 3(\Delta t)^2combine like terms
    2. Subtract s(4)=48+8=56{s(4) = 48 + 8 = 56}: s(4+Δt)−s(4)=26Δt+3(Δt)2\displaystyle s(4 + \Delta t) - s(4) = 26\Delta t + 3(\Delta t)^2
    3. Divide by Δt{\Delta t} and factor it out of the top; since Δt≠0{\Delta t \ne 0}, it cancels: Δt(26+3Δt)Δt=26+3Δt\displaystyle \frac{\cancel{\Delta t}(26 + 3\Delta t)}{\cancel{\Delta t}} = 26 + 3\Delta t
    4. As Δt→0{\Delta t \to 0}, 26+3Δt→26{26 + 3\Delta t \to \boxed{26}}: the speedometer reads 26 ft/s, about 18 mph. The trip average is only 56÷4=14{56 \div 4 = 14} ft/s.

    Common wrong answers

    • 14: That's the trip average, 56 feet in 4 seconds. Find the speed at the instant t = 4.
    • 29: That's the average on [4, 5], Δt = 1. Let Δt shrink toward 0.
    • 56: That's the distance by t = 4, not a speed.
  5. Challenge 4

    Calculator · CED 2.1, 5.1

    The pop-up's height is h(t)=6+80t−16t2{h(t) = {6 + 80t - 16t^2}} feet after t{t} seconds, and its velocity is v(t)=80−32t{v(t) = 80 - 32t} ft/s. It leaves the bat 6 feet above the ground and lands on the ground (h=0{h = 0}). At what time t{t}, in seconds, does its velocity equal its average velocity over the whole flight?

    Answer: 2.537 (or 2.536)

    1. It lands when h(t)=0{h(t) = 0}: 6+80t−16t2=0\displaystyle 6 + 80t - 16t^2 = 016t2−80t−6=0\displaystyle 16t^2 - 80t - 6 = 0times −1{-1} The positive root is the landing time T{T}, in seconds: T=80+6,78432\displaystyle T = \frac{80 + \sqrt{6{,}784}}{32}quadratic formula=10+1064≈5.074\displaystyle = \frac{10 + \sqrt{106}}{4} \approx 5.074
    2. Average velocity over the flight, in ft/s: h(T)−h(0)T−0=0−6T≈−1.183\displaystyle \frac{h(T) - h(0)}{T - 0} = \frac{0 - 6}{T} \approx -1.183 Negative: the ball ends 6 feet lower.
    3. Set v(t){v(t)} equal to that average and solve for t{t}, in seconds: 80−32t=−6T\displaystyle 80 - 32t = -\frac{6}{T}t=80+6/T32≈2.537\displaystyle t = \frac{80 + 6/T}{32} \approx 2.537
    4. Cross-check: for quadratic h{h}, the average velocity over an interval equals the velocity at its midpoint, and T2{\dfrac{T}{2}} is 2.53695… s. So t≈2.537{t \approx \boxed{2.537}} s (or 2.536 s, truncated), just after the peak at 2.5 s. As a polynomial, h{h} is continuous on [0,T]{[0, T]} and differentiable on (0,T){(0, T)}, so the Mean Value Theorem guarantees this time exists.

    Common wrong answers

    • 2.5: That's the peak, where v = 0. The average is 0 only for a landing at the starting height; this ball lands 6 feet lower.
    • 5.074: That's the landing time. Find when v(t) equals the flight's average velocity.
    • -1.183: That's the average velocity itself. Find the time when v(t) equals it.
    • 2.535: That's 5.07 ÷ 2: T was rounded too early. Keep four decimals in T; round only at the end.
  6. Fluency 1

    No calculator · CED 2.1

    Find the average rate of change of f(x)=x2+3x{f(x) = x^2 + 3x} on [1,4]{[1, 4]}.

    Answer: 8

    1. f(4)=16+12=28{f(4) = 16 + 12 = 28} and f(1)=1+3=4{f(1) = 1 + 3 = 4}.
    2. Difference quotient: f(4)−f(1)4−1=28−43\displaystyle \frac{f(4) - f(1)}{4 - 1} = \frac{28 - 4}{3}=243\displaystyle = \frac{24}{3}
    3. The average rate of change is 8.

    Common wrong answers

    • 24: Divide by the width of the interval, 4 − 1 = 3.
    • -8: Same order on top and bottom: f(4) − f(1) over 4 − 1.
  7. Fluency 2

    No calculator · CED 2.1, 2.3

    A runner's distance from the start, D(t){D(t)}, in meters, is measured every 10 seconds. Use the values at t=10{t = 10} and t=30{t = 30} to estimate D′(20){D'(20)}, the velocity at t=20{t = 20}. t (s)0102030D(t) (m)062128188\begin{array}{c|cccc} t \text{ (s)} & 0 & 10 & 20 & 30 \\ \hline D(t) \text{ (m)} & 0 & 62 & 128 & 188 \end{array}

    Answer: 6.3

    1. [10,30]{[10, 30]} is centered at t=20{t = 20}, so its average rate of change estimates D′(20){D'(20)}.
    2. From the table: D(30)−D(10)30−10=188−6220\displaystyle \frac{D(30) - D(10)}{30 - 10} = \frac{188 - 62}{20}=12620\displaystyle = \frac{126}{20}
    3. 12620=6.3{\dfrac{126}{20} = \boxed{6.3}}, so D′(20){D'(20)} is about 6.3 meters per second.

    Common wrong answers

    • 6.4: That's the average from t = 0 to t = 20. Use t = 10 and t = 30.
    • 6.6: That uses t = 10 and t = 20. Use t = 10 and t = 30.
    • 6: That uses t = 20 and t = 30. Use t = 10 and t = 30.
    • 126: Divide by the time between the readings, 30 − 10 = 20 seconds.
  8. Fluency 3

    No calculator · CED 2.1

    For f(x)=3x2{f(x) = 3x^2}, simplify f(2+h)−f(2)h{\dfrac{f(2 + h) - f(2)}{h}}, then evaluate it at h=0.1{h = 0.1}.

    Answer: 12.3

    1. f(2)=12{f(2) = 12}. Expand: f(2+h)=3(2+h)2\displaystyle f(2 + h) = 3(2 + h)^2=3(4+4h+h2)\displaystyle = 3(4 + 4h + h^2)=12+12h+3h2\displaystyle = 12 + 12h + 3h^2
    2. Subtract f(2){f(2)}, then divide by h{h}: f(2+h)−f(2)=12h+3h2\displaystyle f(2 + h) - f(2) = 12h + 3h^2f(2+h)−f(2)h=12+3h\displaystyle \frac{f(2 + h) - f(2)}{h} = 12 + 3hh≠0{h \ne 0}
    3. At h=0.1{h = 0.1}: 12+3(0.1)=12.3{12 + 3(0.1) = \boxed{12.3}}, the average rate of change of f{f} on [2,2.1]{[2, 2.1]}.

    Common wrong answers

    • 12: 12 is the limit, f′(2). Evaluate at h = 0.1.
    • 1.23: That's f(2.1) − f(2). Divide by h = 0.1.
  9. Fluency 4

    No calculator · CED 2.2

    Use the limit definition to find f′(3){f'(3)} for f(x)=x2−4x{f(x) = x^2 - 4x}.

    Answer: 2

    1. f(3)=9−12=−3{f(3) = 9 - 12 = -3}.
    2. f(3+h)=(3+h)2−4(3+h)\displaystyle f(3 + h) = (3 + h)^2 - 4(3 + h)=9+6h+h2−12−4h\displaystyle = 9 + 6h + h^2 - 12 - 4hmultiply out=−3+2h+h2\displaystyle = -3 + 2h + h^2
    3. Subtract f(3)=−3{f(3) = -3}, then divide by h{h}: f(3+h)−f(3)=2h+h2\displaystyle f(3 + h) - f(3) = 2h + h^2f(3+h)−f(3)h=2+h\displaystyle \frac{f(3 + h) - f(3)}{h} = 2 + hh≠0{h \ne 0}
    4. As h→0{h \to 0}, 2+h→2{2 + h \to 2}, so f′(3)=2{f'(3) = \boxed{2}}.

    Common wrong answers

    • -3: That's f(3), a function value, not a rate.
    • 3: That's the average on [3, 4], h = 1. Let h go to 0.
  10. Fluency 5

    No calculator · CED 2.2

    Use the limit definition to find f′(x){f'(x)} for f(x)=5x2+1{f(x) = 5x^2 + 1}. Then evaluate f′(−2){f'(-2)}.

    Answer: -20

    1. f(x+h)=5(x+h)2+1\displaystyle f(x + h) = 5(x + h)^2 + 1=5x2+10xh+5h2+1\displaystyle = 5x^2 + 10xh + 5h^2 + 1multiply out
    2. Subtract f(x)=5x2+1{f(x) = 5x^2 + 1}, then divide by h{h}: f(x+h)−f(x)=10xh+5h2\displaystyle f(x + h) - f(x) = 10xh + 5h^2f(x+h)−f(x)h=10x+5h\displaystyle \frac{f(x + h) - f(x)}{h} = 10x + 5hh≠0{h \ne 0}
    3. As h→0{h \to 0}, this goes to f′(x)=10x{f'(x) = 10x}, so f′(−2)=−20{f'(-2) = \boxed{-20}}.

    Common wrong answers

    • 21: That's f(−2). Find f′(x), then substitute x = −2.
    • 20: Check the sign: f′(x) = 10x, and x is −2.
  11. Fluency 6

    No calculator · CED 2.2

    Evaluate limh→0⁡(4+h)3−64h{\displaystyle\lim_{h \to 0} \frac{(4 + h)^3 - 64}{h}}, the derivative of some function f{f} at some number a{a}.

    Answer: 48

    1. It is f′(4){f'(4)} for f(x)=x3{f(x) = x^3}, because f(4)=43=64{f(4) = 4^3 = 64}.
    2. Expand (4+h)3{(4 + h)^3}, subtract 64, then divide by h{h}: (4+h)3=64+48h+12h2+h3\displaystyle (4 + h)^3 = 64 + 48h + 12h^2 + h^3(4+h)3−64=48h+12h2+h3\displaystyle (4 + h)^3 - 64 = 48h + 12h^2 + h^3(4+h)3−64h=48+12h+h2\displaystyle \frac{(4 + h)^3 - 64}{h} = 48 + 12h + h^2h≠0{h \ne 0}
    3. As h→0{h \to 0}, the quotient goes to 48: f′(4)=48{f'(4) = \boxed{48}}.

    Common wrong answers

    • 64: 64 is f(4), a function value. The limit is the rate f′(4).
    • 0: h = 0 gives 0/0, which says nothing yet. And (4 + h)³ isn't 64 + h³: expand fully to 64 + 48h + 12h² + h³, simplify, then let h go to 0.
  12. Exit ticket

    No calculator · CED 2.1, 2.2

    A sliding hockey puck has gone s(t)=40t−2t2{s(t) = 40t - 2t^2} feet after t{t} seconds, for 0≤t≤10{0 \le t \le 10}. Use the limit definition to find how fast it moves at t=5{t = 5} seconds.

    Answer: 20

    1. s(5)=200−50=150{s(5) = 200 - 50 = 150}.
    2. Expand s(5+Δt){s(5 + \Delta t)}: s(5+Δt)=40(5+Δt)−2(5+Δt)2\displaystyle s(5 + \Delta t) = 40(5 + \Delta t) - 2(5 + \Delta t)^2put in 5+Δt{5 + \Delta t} for t{t}=200+40Δt−50−20Δt−2(Δt)2\displaystyle = 200 + 40\Delta t - 50 - 20\Delta t - 2(\Delta t)^2multiply out=150+20Δt−2(Δt)2\displaystyle = 150 + 20\Delta t - 2(\Delta t)^2combine like terms
    3. Subtract s(5)=150{s(5) = 150}, divide by Δt{\Delta t}, and factor it out of the top; since Δt≠0{\Delta t \ne 0}, it cancels: s(5+Δt)−s(5)=20Δt−2(Δt)2\displaystyle s(5 + \Delta t) - s(5) = 20\Delta t - 2(\Delta t)^2Δt(20−2Δt)Δt=20−2Δt\displaystyle \frac{\cancel{\Delta t}(20 - 2\Delta t)}{\cancel{\Delta t}} = 20 - 2\Delta t
    4. As Δt→0{\Delta t \to 0}, 20−2Δt→20{20 - 2\Delta t \to \boxed{20}}. At t=5{t = 5} the puck is moving at 20 ft/s.

    Common wrong answers

    • 30: That's the average over the first 5 seconds. Find the speed at the instant t = 5.
    • 150: That's the distance by t = 5, not a speed.
    • 18: That's the average on [5, 6], Δt = 1. Let Δt shrink toward 0.

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