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Unit 1: Limits and Continuity

Introducing Calculus: Can Change Occur at an Instant?

Explain why an average rate of change can't be computed at a single instant, and find the instantaneous rate as the limit of average rates over shrinking intervals.

Topic 1.1 · 8 min read

A car's speedometer shows one number at one moment: 50 km/h right now. But speed is distance divided by time, and in a single instant the car covers no distance in no time. Around 450 BCE the Greek philosopher Zeno of Elea pushed this into a paradox: at any one instant a flying arrow occupies a space exactly its own size, so at that instant it is not moving, and yet it gets to the target.

Average rate of change

When a quantity f(x)f(x) changes as xx goes from aa to bb, its average rate of change on [a,b][a, b] is the change in output divided by the change in input:

f(b)−f(a)b−a.\frac{f(b) - f(a)}{b - a}.

Its units are output units per input unit: meters per second, gallons per minute, dollars per year. On a graph it is the slope of the secant line, the straight line through the two points (a,f(a))(a, f(a)) and (b,f(b))(b, f(b)).

Take a ball tossed straight up from the ground. Rounding gravity to 10 m/s², its height after tt seconds is s(t)=20t−5t2s(t) = 20t - 5t^2 meters, so s(1)=15s(1) = 15, s(2)=20s(2) = 20 and s(3)=15s(3) = 15. Its average velocity on [1,2][1, 2] is

s(2)−s(1)2−1=20−151=5 m/s.\frac{s(2) - s(1)}{2 - 1} = \frac{20 - 15}{1} = 5 \text{ m/s}.

On [1,3][1, 3] the average velocity is 15−152=0\frac{15 - 15}{2} = 0 m/s, even though the ball was never sitting still: it rose for one second and fell back for one second. An average rate describes the interval as a whole and erases what happened inside it. The longer the interval, the more it erases.

Why an instant breaks the formula

To get the velocity at exactly t=1t = 1, the obvious move is to make both endpoints equal to 1:

s(1)−s(1)1−1=00.\frac{s(1) - s(1)}{1 - 1} = \frac{0}{0}.

This is not 0 and it is not a very large number. It is undefined, because division by zero has no answer. And 00\frac{0}{0} is undefined in a particularly unhelpful way: the equation 0⋅q=00 \cdot q = 0 holds for every number qq, so no single number deserves to be called the quotient. The average-rate formula needs the input to change. At a single instant it doesn't, so the formula has nothing to say there, and this is Zeno's arrow in algebra.

Instantaneous rate as a limit of average rates

The way out is to use intervals that contain the instant and shrink toward it. Each one has a perfectly good average rate, and you watch where those averages head. For the ball at t=1t = 1, use the interval from 1 to 1+h1 + h, where hh is a small number, positive (the interval extends to the right of 1) or negative (to the left).

hhIntervalAverage velocity (m/s)
0.10.1[1,1.1][1, 1.1]9.59.5
0.010.01[1,1.01][1, 1.01]9.959.95
0.0010.001[1,1.001][1, 1.001]9.9959.995
−0.001-0.001[0.999,1][0.999, 1]10.00510.005
−0.01-0.01[0.99,1][0.99, 1]10.0510.05
−0.1-0.1[0.9,1][0.9, 1]10.510.5

From both sides the averages close in on 10. Algebra shows why. For any h≠0h \neq 0,

s(1+h)−s(1)h=20(1+h)−5(1+h)2−15h=10h−5h2h=10−5h.\frac{s(1+h) - s(1)}{h} = \frac{20(1+h) - 5(1+h)^2 - 15}{h} = \frac{10h - 5h^2}{h} = 10 - 5h.

Cancelling hh is legal precisely because h≠0h \neq 0; the average is never computed over an interval of length zero. But the expression 10−5h10 - 5h makes it plain that when hh is close to 0, the average velocity is close to 10, and it can be brought as close to 10 as you like by taking hh small enough. That target value is the instantaneous velocity: 10 m/s upward at t=1t = 1. The averages from the right are below 10 and those from the left are above 10 because the ball is slowing down, so a later interval catches it moving more slowly.

On the graph, each average rate is the slope of a secant line through (1,15)(1, 15). As the second point slides toward (1,15)(1, 15), the secant lines turn and settle on one line, the tangent line, whose slope is the instantaneous rate.

The graph of s(t) = 20t minus 5t squared for t from 0 to 4, a downward parabola through (0, 0), (1, 15), (2, 20), (3, 15) and (4, 0). Three lines pass through (1, 15): a dashed secant to (3, 15) with slope 0, a dash-dot secant to (2, 20) with slope 5, and the dotted tangent line at t = 1 with slope 10.

The notation lim⁡h→0\lim\limits_{h \to 0} reads "the limit as hh approaches 0" and asks where the values head as hh gets close to 0, never what happens at h=0h = 0 itself. Topic 1.2 makes the notation precise, and in Unit 2 this same limit becomes the derivative.

When there is no single rate

The averages don't always agree. For f(x)=∣x∣f(x) = |x| at x=0x = 0, the average rate on [0,h][0, h] is ∣h∣−0h\frac{|h| - 0}{h}. For every h>0h > 0 this equals 11, and for every h<0h < 0 it equals −1-1. Intervals to the right all say the rate is 1, intervals to the left all say it is −1-1, and shrinking them never brings the two answers together. So ∣x∣|x| has no instantaneous rate of change at 0; its graph has a sharp corner there, and no single tangent line. The instantaneous rate exists only when the average rates on both sides approach the same number, which is why the definition checks both.

Worked examples

Worked exampleExample 1: the averages, then the limit

Let f(x)=1xf(x) = \dfrac{1}{x}. Write the average rate of change of ff on the interval between 22 and 2+h2 + h as a simplified expression in hh, and use it to find the instantaneous rate of change of ff at x=2x = 2.

Show solution

Combine the fractions in the numerator over the common denominator 2(2+h)2(2+h), then divide by hh:

f(2+h)−f(2)h=12+h−12h=2−(2+h)2(2+h)h=−h2h(2+h)=−12(2+h),h≠0.\frac{f(2+h) - f(2)}{h} = \frac{\frac{1}{2+h} - \frac{1}{2}}{h} = \frac{\frac{2 - (2+h)}{2(2+h)}}{h} = \frac{-h}{2h(2+h)} = \frac{-1}{2(2+h)}, \quad h \neq 0.

The point of simplifying is to get rid of the hh in the denominator, the factor that makes the original quotient 00\frac{0}{0} at h=0h = 0. As a check, h=0.1h = 0.1 gives −14.2≈−0.238-\frac{1}{4.2} \approx -0.238 and h=−0.1h = -0.1 gives −13.8≈−0.263-\frac{1}{3.8} \approx -0.263, on either side of −0.25-0.25.

As hh approaches 0, 2(2+h)2(2 + h) approaches 4, so the averages approach −14-\frac{1}{4}. The instantaneous rate of change of ff at x=2x = 2 is −14-\frac{1}{4}. The negative sign fits the graph: 1x\frac{1}{x} is decreasing for x>0x > 0.

Worked exampleExample 2: a rate you can only estimate for now (calculator)

Let g(x)=2xg(x) = 2^x. Estimate the instantaneous rate of change of gg at x=0x = 0 to three decimal places.

Show solution

The average rate on the interval between 0 and hh is 2h−20h=2h−1h\dfrac{2^h - 2^0}{h} = \dfrac{2^h - 1}{h}, and no algebra cancels the hh here, so compute averages on both sides with a calculator:

hh−0.01-0.01−0.001-0.0010.0010.0010.010.01
2h−1h\frac{2^h - 1}{h}0.690750.690750.692910.692910.693390.693390.695560.69556

The averages from the left increase and those from the right decrease, so the instantaneous rate is trapped between 0.692910.69291 and 0.693390.69339. Both round to 0.6930.693, so the rate is about 0.6930.693. Using intervals on both sides is what makes the estimate trustworthy: a single side gives a number that is off in the third decimal place unless hh is very small. Topic 3.1 shows the exact value is ln⁡2≈0.6931\ln 2 \approx 0.6931.

Worked exampleExample 3: rates from a table, in context (calculator)

Water flows into a tank. The amount of water in the tank, W(t)W(t) gallons, is measured at selected times tt minutes, as shown in the table below.

t (minutes)025710W(t) (gallons)200236275290302\begin{array}{c|ccccc} t \text{ (minutes)} & 0 & 2 & 5 & 7 & 10 \\ \hline W(t) \text{ (gallons)} & 200 & 236 & 275 & 290 & 302 \end{array}

(a) Find the average rate of change of WW over the interval 0≤t≤100 \le t \le 10. Indicate units of measure.

(b) Use the data in the table to estimate the rate at which the amount of water in the tank is changing at time t=6t = 6 minutes. Show the computation that leads to your answer, and indicate units.

(c) Can the data in the table determine the rate at t=6t = 6 exactly? Explain.

Show solution

(a) Divide the change in water by the change in time:

W(10)−W(0)10−0=302−20010=10.2 gallons per minute.\frac{W(10) - W(0)}{10 - 0} = \frac{302 - 200}{10} = 10.2 \text{ gallons per minute}.

(b) Use the smallest interval in the table that contains t=6t = 6, which is [5,7][5, 7], because the shorter the interval around the instant, the less it averages away:

W(7)−W(5)7−5=290−2752=7.5 gallons per minute.\frac{W(7) - W(5)}{7 - 5} = \frac{290 - 275}{2} = 7.5 \text{ gallons per minute}.

The amount of water is increasing at about 7.5 gallons per minute at t=6t = 6. Note how different this is from the 10.2 of part (a): the tank filled faster early on, and the long interval mixes that in.

(c) No. The rate at t=6t = 6 is the limit of average rates over intervals shrinking to t=6t = 6, so it depends on values of WW at times arbitrarily close to 6, and the table gives values only at 5 and 7. Plugging t=6t = 6 in for both endpoints gives 00\frac{0}{0}, which is undefined. The table supports an estimate, not an exact value.

Where students lose points

Check yourself

  1. Question 1

    A ball's height is s(t)s(t) meters at time tt seconds. Which expression gives the ball's instantaneous velocity at t=3t = 3?

    1. A

      s(3)−s(0)3−0\dfrac{s(3) - s(0)}{3 - 0}

    2. B

      lim⁡h→0s(3+h)−s(3)h\lim\limits_{h \to 0} \dfrac{s(3+h) - s(3)}{h}

    3. C

      s(3+h)−s(3)h\dfrac{s(3+h) - s(3)}{h} evaluated at h=0h = 0

    4. D

      lim⁡h→0s(3+h)\lim\limits_{h \to 0} s(3+h)

    Show answer

    B

    The instantaneous velocity is the limit of average velocities over intervals shrinking to t=3t = 3. Choice C tries to use an interval of length zero, which gives the undefined 00\frac{0}{0}; choice A is an average over three whole seconds, and choice D is where the height heads, not the velocity.

  2. Question 2

    Water drains from a tank. V(t)V(t) is the volume of water in the tank, in liters, at time tt minutes. Suppose lim⁡h→0V(5+h)−V(5)h=−3\lim\limits_{h \to 0} \dfrac{V(5+h) - V(5)}{h} = -3. Explain what this statement means in the context of the problem, with units.

    Show answer

    At time t=5t = 5 minutes, the volume of water in the tank is decreasing at a rate of 3 liters per minute.

    The limit of average rates over intervals shrinking to t=5t = 5 is the instantaneous rate of change of VV at that moment, in liters per minute, and the negative sign means decreasing. It does not say the tank holds 3 liters at t=5t = 5, and it does not say exactly 3 liters drain during the next minute: that would be an average rate over [5,6][5, 6], which can differ from the rate at the instant.

  3. Question 3

    For a function ff, the average rate of change on the interval between 11 and 1+h1 + h is 3.313.31, 3.03013.0301 and 3.0030013.003001 for h=0.1,0.01,0.001h = 0.1, 0.01, 0.001, and 2.712.71, 2.97012.9701 and 2.9970012.997001 for h=−0.1,−0.01,−0.001h = -0.1, -0.01, -0.001. What is the best estimate of the instantaneous rate of change of ff at x=1x = 1?

    1. A

      33

    2. B

      3.0033.003

    3. C

      3.313.31

    4. D

      00

    Show answer

    A

    The averages from the right decrease toward 3 and those from the left increase toward 3, so the rate is trapped between 2.9970012.997001 and 3.0030013.003001 and appears to be 3. Choice B is just the closest average from one side, which still contains the error from using a nonzero hh.

  4. Question 4

    Let f(x)=∣x−2∣f(x) = |x - 2|. Does ff have an instantaneous rate of change at x=2x = 2? Use average rates of change to explain.

    Show answer

    No. Average rates on intervals to the right of 2 all equal 11, and on intervals to the left of 2 all equal −1-1, so they don't approach a single number.

    On the interval between 2 and 2+h2 + h the average rate is ∣h∣h\frac{|h|}{h}, which is 11 for every h>0h > 0 and −1-1 for every h<0h < 0. Shrinking the intervals never brings the two sides together, so there is no instantaneous rate (the graph has a corner at x=2x = 2).

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