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VICMath MethodsSyllabus dot point

How is the definite integral used to compute the average value of a function, total change from a rate of change, and related applications?

Applications of integration including the average value of a function on a closed interval, total change from a rate of change function, and kinematics (displacement and distance from velocity)

A focused answer to the VCE Math Methods Unit 4 key-knowledge point on applications of integration. Average value of a function, total change from a rate function, kinematics (displacement from velocity), and the recurring Paper 2 contexts in volume of water, drug concentration and population modelling.

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What this dot point is asking

VCAA wants you to use the definite integral in three application contexts: the average value of a function on a closed interval, the total change of a quantity from a given rate of change, and kinematics (displacement and distance from velocity). The dot point bridges the abstract calculus of Unit 3 to the modelling Paper 2 SAC and exam.

Average value of a function

The average value of ff on [a,b][a, b] is:

fΛ‰=1bβˆ’a∫abf(x) dx\bar f = \frac{1}{b - a} \int_{a}^{b} f(x) \, dx

Geometrically, fΛ‰\bar f is the height of the rectangle on [a,b][a, b] whose area equals ∫abf(x) dx\int_{a}^{b} f(x) \, dx. The rectangle has width (bβˆ’a)(b - a) and area equal to the integral, so its height is the integral divided by the width.

Procedure

  1. Compute the definite integral ∫abf(x) dx\int_{a}^{b} f(x) \, dx.
  2. Divide by the interval length bβˆ’ab - a.

Why it matters

In modelling contexts, average value is the natural "typical level" of a continuous quantity over time. The average temperature over a day, the average flow rate, the average drug concentration. All are integrals divided by interval length.

Example

Average value of f(x)=sin⁑(x)f(x) = \sin(x) on [0,Ο€][0, \pi].

fΛ‰=1Ο€βˆ’0∫0Ο€sin⁑(x) dx=1Ο€[βˆ’cos⁑(x)]0Ο€=1Ο€((βˆ’(βˆ’1))βˆ’(βˆ’1))=1Ο€β‹…2=2Ο€\bar f = \frac{1}{\pi - 0} \int_{0}^{\pi} \sin(x) \, dx = \frac{1}{\pi} [-\cos(x)]_{0}^{\pi} = \frac{1}{\pi} ((-(-1)) - (-1)) = \frac{1}{\pi} \cdot 2 = \frac{2}{\pi}.

Average value approximately 0.6370.637.

Total change from a rate of change

If r(t)=dQdtr(t) = \frac{dQ}{dt} is the rate of change of a quantity QQ with respect to time, the total change over [t1,t2][t_1, t_2] is:

Q(t2)βˆ’Q(t1)=∫t1t2r(t) dtQ(t_2) - Q(t_1) = \int_{t_1}^{t_2} r(t) \, dt

This is the fundamental theorem of calculus applied to a rate function.

Procedure

  1. Identify the rate function r(t)r(t).
  2. Compute the definite integral.
  3. Interpret the result in the context's units.

Worked contexts

Water flowing into / out of a container. Rate in litres per minute integrated over time gives volume in litres.

Drug concentration in blood. Rate of change of concentration integrated gives concentration change.

Population growth. Rate of change of population integrated gives population change.

Energy flow. Power (rate of energy transfer) integrated gives energy.

Example

Water flows into a tank at r(t)=3+0.5tr(t) = 3 + 0.5 t litres per minute, 0≀t≀100 \leq t \leq 10 minutes. Volume added in the first 10 minutes:

V=∫010(3+0.5t) dt=[3t+0.25t2]010=30+25=55V = \int_{0}^{10} (3 + 0.5 t) \, dt = [3 t + 0.25 t^2]_{0}^{10} = 30 + 25 = 55 litres.

Kinematics: displacement and distance from velocity

The velocity v(t)v(t) of a particle is the rate of change of its position x(t)x(t), so v(t)=dxdtv(t) = \frac{dx}{dt}.

Displacement (signed)

The displacement of the particle on [t1,t2][t_1, t_2] is:

x(t2)βˆ’x(t1)=∫t1t2v(t) dtx(t_2) - x(t_1) = \int_{t_1}^{t_2} v(t) \, dt

Displacement is signed: positive if the net motion is in the positive direction, negative if in the negative direction, zero if the particle returns to its starting point.

Distance travelled (unsigned)

The total distance travelled is the integral of speed (always non-negative):

Distance=∫t1t2∣v(t)βˆ£β€‰dt\text{Distance} = \int_{t_1}^{t_2} \lvert v(t) \rvert \, dt

If the velocity changes sign on the interval, the distance is not the same as the displacement. Compute distance by splitting the interval at the zeros of vv and summing the absolute values of each piece.

Procedure for distance

  1. Find the zeros of v(t)v(t) on [t1,t2][t_1, t_2]. These are the times when the particle changes direction.
  2. Split the interval at each zero.
  3. Compute ∣∫v dt∣\lvert \int v \, dt \rvert on each sub-interval and sum.

Example

A particle has velocity v(t)=2tβˆ’6v(t) = 2t - 6 for 0≀t≀50 \leq t \leq 5 seconds.

Displacement. ∫05(2tβˆ’6) dt=[t2βˆ’6t]05=(25βˆ’30)βˆ’0=βˆ’5\int_{0}^{5} (2t - 6) \, dt = [t^2 - 6t]_{0}^{5} = (25 - 30) - 0 = -5.

Displacement is βˆ’5-5 metres (5 metres in the negative direction net).

Distance. v(t)=0v(t) = 0 at t=3t = 3. Split at t=3t = 3.

On [0,3][0, 3]: v<0v < 0 for t<3t < 3. ∫03(2tβˆ’6) dt=[t2βˆ’6t]03=9βˆ’18=βˆ’9\int_{0}^{3} (2t - 6) \, dt = [t^2 - 6t]_{0}^{3} = 9 - 18 = -9. Distance on this piece: βˆ£βˆ’9∣=9|-9| = 9.

On [3,5][3, 5]: v>0v > 0 for t>3t > 3. ∫35(2tβˆ’6) dt=(25βˆ’30)βˆ’(9βˆ’18)=βˆ’5βˆ’(βˆ’9)=4\int_{3}^{5} (2t - 6) \, dt = (25 - 30) - (9 - 18) = -5 - (-9) = 4. Distance: 44.

Total distance: 9+4=139 + 4 = 13 metres.

Note: displacement βˆ’5-5 differs from distance 1313 because the particle changed direction at t=3t = 3.

Position from velocity (with initial condition)

If v(t)=dxdtv(t) = \frac{dx}{dt} and x(0)=x0x(0) = x_0 is the initial position, then:

x(t)=x0+∫0tv(s) dsx(t) = x_0 + \int_{0}^{t} v(s) \, ds

Use this to find the position function from the velocity function and an initial condition.

Average rate of change

The average rate of change of a quantity over an interval is:

rΛ‰=TotalΒ changeIntervalΒ length=Q(t2)βˆ’Q(t1)t2βˆ’t1=1t2βˆ’t1∫t1t2r(t) dt\bar r = \frac{\text{Total change}}{\text{Interval length}} = \frac{Q(t_2) - Q(t_1)}{t_2 - t_1} = \frac{1}{t_2 - t_1} \int_{t_1}^{t_2} r(t) \, dt

This is the average value of the rate function. The same formula applies to velocity (average velocity = displacement / time) and speed (average speed = distance / time).

Common errors

Forgetting to divide by interval length. The average value formula is the integral divided by bβˆ’ab - a. Reporting the integral itself as the "average value" earns no marks.

Mixing displacement and distance. Displacement is signed; distance is the sum of absolute values over direction-change-split pieces. The two are equal only when the velocity does not change sign on the interval.

Forgetting to split at zeros of velocity. For distance, you must split at every zero of vv. A single integral of ∣v(t)∣\lvert v(t) \rvert also works mathematically but is messier than splitting.

Wrong sign in ∫v dt\int v \, dt. If vv is negative on part of the interval, the integral is negative; that is fine for displacement but you must take absolute values for distance.

Units forgotten. Application questions are scored partly on units. Reporting "5" when the answer is "5 litres per minute" loses contextual marks.

Calculator-only set-up. Paper 2 expects you to set up the integral by hand (state the integrand and the limits) and use the calculator only for evaluation. A blank "by calculator, the answer is 9.20" without the set-up usually loses set-up marks.

In one sentence

The definite integral is the natural tool for three applications: the average value of a function on [a,b][a, b] is the integral divided by bβˆ’ab - a; the total change of a quantity over an interval is the integral of its rate of change; and in kinematics, the integral of velocity gives signed displacement while the integral of speed (or split-interval absolute integrals of velocity) gives total distance travelled.

Past exam questions, worked

Real questions from past VCAA papers on this dot point, with our answer explainer.

2024 VCAA Paper 13 marksFind the average value of $f(x) = 3 x^2 - 2$ on the interval $[1, 3]$.
Show worked answer β†’

The average value of ff on [a,b][a, b] is fΛ‰=1bβˆ’a∫abf(x) dx\bar f = \frac{1}{b - a} \int_{a}^{b} f(x) \, dx.

Antiderivative. ∫(3x2βˆ’2) dx=x3βˆ’2x\int (3 x^2 - 2) \, dx = x^3 - 2x.

Definite integral. [x3βˆ’2x]13=(27βˆ’6)βˆ’(1βˆ’2)=21βˆ’(βˆ’1)=22[x^3 - 2x]_{1}^{3} = (27 - 6) - (1 - 2) = 21 - (-1) = 22.

Average value. fΛ‰=13βˆ’1β‹…22=222=11\bar f = \frac{1}{3 - 1} \cdot 22 = \frac{22}{2} = 11.

Markers reward the correct formula, the definite integral evaluation, and division by interval length.

2023 VCAA Paper 25 marksWater flows out of a tank at a rate $r(t) = 2 + 4 t e^{-t}$ litres per minute, where $t$ is measured in minutes. (a) Find the total volume of water that has flowed out in the first 3 minutes. (b) Find the average rate of flow over the same interval.
Show worked answer β†’

(a) Total volume.

V=∫03(2+4teβˆ’t) dtV = \int_{0}^{3} (2 + 4 t e^{-t}) \, dt.

The first term: ∫032 dt=6\int_{0}^{3} 2 \, dt = 6.

The second term: ∫034teβˆ’t dt\int_{0}^{3} 4 t e^{-t} \, dt requires technology in Paper 2; using a CAS, this evaluates to approximately 4(1βˆ’4eβˆ’3)β‰ˆ3.204(1 - 4 e^{-3}) \approx 3.20 (to 2 decimal places).

Total: approximately 6+3.20=9.206 + 3.20 = 9.20 litres.

(b) Average rate.

rΛ‰=Vt2βˆ’t1=9.203β‰ˆ3.07\bar r = \frac{V}{t_2 - t_1} = \frac{9.20}{3} \approx 3.07 litres per minute.

Markers reward the definite integral set-up for total volume, calculator-active evaluation, and the average-rate formula (total / interval).

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