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AI HL · AHL 9

Differential Equations

AHL 9.3

Separable equations in context: growth, decay and harder forms

AHL 9.3

Separable equations in context: growth, decay and harder forms

Target: I can find the constant of proportionality k from an initial amount and an initial rate of change. (+6 more)

By the end of this section

Key points

Growth and decay

  • \(\dfrac{dN}{dt}=kN\) gives \(N=N_0e^{kt}\). For decay write \(\dfrac{dm}{dt}=-km\) with \(k>0\), and \(m=m_0e^{-kt}\).
  • Find \(k\) from the start: \(k=\dfrac{\text{initial rate}}{\text{initial amount}}\). A rate of decrease of 12 when the amount is 80 gives \(\dfrac{dm}{dt}=-12\) and \(k=\dfrac{12}{80}\).
  • Half-life: solve \(\tfrac12m_0=m_0e^{-kt}\), so \(t=\dfrac{\ln2}{k}\). The time to "disappear" in a model that reaches zero comes from setting the quantity to 0.

Inverse proportion and other models

  • \(\dfrac{dV}{dt}=\dfrac{k}{V}\) separates to \(\int V\,dV=\int k\,dt\), so \(V^2=2kt+c\). Find \(k\) from the start: \(k=\text{rate}\times V\).
  • To "show that" \(\dfrac{dV}{dt}=\dfrac{2000}{V}\): write \(\dfrac{dV}{dt}=\dfrac kV\), put in the initial values and solve for \(k\).
  • For \(\dfrac{dv}{dt}=a-bv\) separate to \(\int\dfrac{1}{a-bv}\,dv=\int dt\). The velocity levels off at \(\dfrac ab\).
  • Distance is the integral of velocity: \(s=\displaystyle\int_0^{T}v\,dt\). The calculator evaluates it.

A sphere

  • \(V=\tfrac43\pi r^3\) and the surface area is \(S=4\pi r^2\). These are in the formula booklet.
  • By the chain rule \(\dfrac{dV}{dt}=4\pi r^2\dfrac{dr}{dt}\). If \(\dfrac{dV}{dt}=-kS\) then \(\dfrac{dr}{dt}=-k\): the radius shrinks at a constant rate.

Harder separations

  • \(e^{x+y}=e^xe^y\). That is what makes \(\dfrac{dy}{dx}=e^{x+y}\) separable: \(\displaystyle\int e^{-y}dy=\int e^{x}dx\).
  • A square root has two values. Use the initial condition to choose: if \(y=-3\) at the start, take \(y=-\sqrt{\ldots}\).
  • An implicit solution such as \(\cos y-2\cos x=c\) can give two values of \(y\) for one \(x\). A restricted domain tells you which ones to keep.

Cooling and mixing

  • Newton's law of cooling: \(\dfrac{dT}{dt}=-k(T-A)\), where \(A\) is the surrounding temperature and \(k>0\). The quantity that decays is \(T-A\), so \(T=A+Be^{-kt}\).
  • Use two readings: the start gives \(B\), a later reading gives \(k\). Keep the full value of \(k\) for later working.
  • Mixing: \(\dfrac{dm}{dt}=\text{rate in}-\text{rate out}\). Rate in = concentration in × flow in. Rate out = \(\dfrac{m}{V}\) × flow out, when the tank is stirred.
  • Both models have the form \(\dfrac{dy}{dt}=a-by\). The solution levels off at \(\dfrac ab\): the room temperature, or the salt mass the tank settles at.

On the calculator

Evaluating a definite integral

  • Enter the velocity as a function of t.
  • Evaluate its definite integral from 0 to the time given.
  • Write the value to 3 significant figures, with units.

Screenshot and video to come

Worked examples

Problems like the ones in class. Pick one, try it, then open the working.
Decay and half-life

The mass \(m\) mg of a drug in the blood decreases at a rate proportional to \(m\). At first \(m=80\) and the mass is decreasing at 12 mg per hour. Find \(k\) in \(\dfrac{dm}{dt}=-km\), find \(m\) in terms of \(t\), and find how long it takes for the mass to halve.

Working
  1. Find k

    \(12=k\times80\ \Rightarrow\ k=0.15\)

    At the start dm/dt = −12 and m = 80.

  2. Separate

    \(\int\dfrac1m\,dm=\int-0.15\,dt\)

    m > 0, so no modulus.

  3. Solve for m

    \(\ln m=-0.15t+c\ \Rightarrow\ m=Ae^{-0.15t}\)

    At t = 0, m = 80, so A = 80.

  4. The model

    \(m=80e^{-0.15t}\)

  5. Half the mass

    \(40=80e^{-0.15t}\ \Rightarrow\ t=\dfrac{\ln2}{0.15}=4.62\)

    About 4.62 hours.

Video walkthrough coming
Growth and a value at a time

A culture of cells grows at a rate proportional to the number of cells \(N\). At first there are 1500 cells and the number is increasing at 90 cells per minute. Find \(k\) in \(\dfrac{dN}{dt}=kN\), then the number of cells after 20 minutes, to 3 significant figures.

Working
  1. Find k

    \(90=k\times1500\ \Rightarrow\ k=0.06\)

    Initial rate ÷ initial amount.

  2. Solve

    \(\int\dfrac1N\,dN=\int0.06\,dt\ \Rightarrow\ N=Ae^{0.06t}\)

    N > 0.

  3. Use N = 1500 at t = 0

    \(N=1500e^{0.06t}\)

    A = 1500.

  4. At t = 20

    \(N=1500e^{1.2}=4980\)

    About 4980 cells.

Video walkthrough coming
Inverse proportion in context

A gas bubble is inflated at a rate inversely proportional to its volume \(V\) cm³. Initially \(V=250\) and the volume is increasing at 8 cm³ per second. Show that \(\dfrac{dV}{dt}=\dfrac{2000}{V}\) and find \(V\) in terms of \(t\). Give the value of \(k\) that you find.

Working
  1. Set up

    \(\dfrac{dV}{dt}=\dfrac kV\)

    Inversely proportional to V.

  2. Use the start

    \(8=\dfrac{k}{250}\ \Rightarrow\ k=2000\)

    So dV/dt = 2000/V, as required.

  3. Separate

    \(\int V\,dV=\int2000\,dt\)

  4. Integrate

    \(\dfrac{V^2}{2}=2000t+c\)

    At t = 0, V = 250: c = 31 250.

  5. Solve for V

    \(V^2=4000t+62\,500,\ \ V=\sqrt{4000t+62\,500}\)

    V is positive.

Video walkthrough coming
Terminal velocity and distance

A ball sinks through oil. Its velocity \(v\) m s⁻¹ after \(t\) seconds satisfies \(\dfrac{dv}{dt}=9-0.3v\), and \(v=0\) when \(t=0\). Find \(v\) in terms of \(t\), then the distance it falls in the first 4 seconds.

Working
  1. Separate

    \(\int\dfrac{1}{9-0.3v}\,dv=\int1\,dt\)

  2. Integrate

    \(-\dfrac{1}{0.3}\ln(9-0.3v)=t+c\)

    9 − 0.3v > 0 at the start.

  3. Solve for v

    \(\ln(9-0.3v)=-0.3t+c_1\ \Rightarrow\ 9-0.3v=Ae^{-0.3t}\)

    v = 0 at t = 0 gives A = 9.

  4. The velocity

    \(v=30\left(1-e^{-0.3t}\right)\)

    v approaches 30 m s⁻¹, since 9 ÷ 0.3 = 30.

  5. Distance

    From the calculator: \(\int_0^4 30\left(1-e^{-0.3t}\right)dt=50.1\)

    Distance is the integral of velocity. About 50.1 m.

Video walkthrough coming
Newton's law of cooling

A cup of coffee at 90 °C is left in a room at 20 °C. Its temperature \(T\) °C after \(t\) minutes decreases at a rate proportional to \(T-20\). After 5 minutes the coffee is at 62 °C. Write down a differential equation for \(T\), find \(T\) in terms of \(t\), and find how long it takes to cool to 35 °C.

Working
  1. The equation

    \(\dfrac{dT}{dt}=-k(T-20),\ k>0\)

    The rate is proportional to T − 20. T falls towards 20, so the rate is negative.

  2. Separate

    \(\int\dfrac{1}{T-20}\,dT=\int-k\,dt\)

    T > 20, so no modulus is needed.

  3. Solve for T

    \(\ln(T-20)=-kt+c\ \Rightarrow\ T=20+Ae^{-kt}\)

    T = 90 when t = 0, so A = 70.

  4. Find k

    \(62=20+70e^{-5k}\ \Rightarrow\ k=\dfrac{\ln(70/42)}{5}=0.102\)

    Keep the full value of k in later working.

  5. The model

    \(T=20+70e^{-0.102t}\)

    T approaches the room temperature, 20 °C.

  6. Time to reach 35

    \(35=20+70e^{-kt}\ \Rightarrow\ t=\dfrac{\ln(70/15)}{k}=15.1\)

    About 15.1 minutes.

Video walkthrough coming
A mixing tank

A tank holds 200 litres of pure water. Salt solution of concentration 0.2 kg per litre flows in at 10 litres per minute. The mixture is stirred and flows out at 10 litres per minute, so the volume stays at 200 litres. After \(t\) minutes the tank holds \(m\) kg of salt. Write down a differential equation for \(m\), solve it, and find the mass of salt after 20 minutes.

Working
  1. Rate in

    \(0.2\times10=2\) kg per minute

    Concentration times flow.

  2. Rate out

    \(\dfrac{m}{200}\times10=0.05m\) kg per minute

    The tank is stirred, so the concentration is m ÷ 200.

  3. The equation

    \(\dfrac{dm}{dt}=2-0.05m\)

    Rate of change = rate in − rate out.

  4. Solve

    \(\int\dfrac{1}{2-0.05m}\,dm=\int dt\ \Rightarrow\ 2-0.05m=Ae^{-0.05t}\)

    m = 0 at t = 0, so A = 2.

  5. The model

    \(m=40\left(1-e^{-0.05t}\right)\), so \(m(20)=25.3\)

    The salt approaches 40 kg, since 2 ÷ 0.05 = 40.

Video walkthrough coming
A dissolving sphere

A spherical sweet dissolves. Its volume decreases at a rate proportional to its surface area. When the volume is 18 cm³ the volume is decreasing at 2.4 cm³ per minute. Find \(\dfrac{dr}{dt}\), where \(r\) cm is the radius, and the time for the sweet to dissolve completely, in minutes.

Working
  1. The model

    \(\dfrac{dV}{dt}=-kS=-k\times4\pi r^2\)

    A decrease proportional to surface area.

  2. Chain rule

    \(\dfrac{dV}{dt}=4\pi r^2\dfrac{dr}{dt}\ \Rightarrow\ \dfrac{dr}{dt}=-k\)

    The 4πr² cancels: the radius shrinks at a constant rate.

  3. Radius now

    \(18=\tfrac43\pi r^3\ \Rightarrow\ r=1.626\)

    Surface area S = 4π × 1.626² = 33.21 cm².

  4. Find k

    \(2.4=k\times33.21\ \Rightarrow\ k=0.0723\)

    So dr/dt = −0.0723 cm per minute.

  5. Time to dissolve

    \(t=\dfrac{1.626}{0.0723}=22.5\)

    The radius falls from 1.63 cm to 0 at a constant rate.

Video walkthrough coming
An exponent that splits

Given that \(\dfrac{dy}{dx}=e^{2x+y}\) and \(y=0\) when \(x=0\), find \(y\) in terms of \(x\). The general solution is \(e^{-y}=A-\tfrac12e^{2x}\). Find \(A\).

Working
  1. Split the exponent

    \(\dfrac{dy}{dx}=e^{2x}e^{y}\)

    This is what makes it separable.

  2. Separate

    \(\int e^{-y}\,dy=\int e^{2x}\,dx\)

    Divide by e^y.

  3. Integrate

    \(-e^{-y}=\tfrac12e^{2x}+c\)

  4. Use x = 0, y = 0

    \(-1=\tfrac12+c\ \Rightarrow\ c=-1.5,\ A=1.5\)

    e⁰ = 1.

  5. Solve for y

    \(e^{-y}=1.5-\tfrac12e^{2x}\ \Rightarrow\ y=-\ln\left(1.5-\tfrac12e^{2x}\right)\)

Video walkthrough coming
Choosing the sign of the root

Given that \(y\dfrac{dy}{dx}=6x^2\) and that \(y=-3\) when \(x=1\), find \(y\) in terms of \(x\). Then find \(y\) when \(x=2\), to 3 significant figures.

Working
  1. Separate and integrate

    \(\int y\,dy=\int6x^2\,dx\ \Rightarrow\ \dfrac{y^2}{2}=2x^3+c\)

  2. Use x = 1, y = −3

    \(\dfrac92=2+c\ \Rightarrow\ c=2.5\)

    Square the −3 first.

  3. Solve for y²

    \(y^2=4x^3+5\)

  4. Choose the sign

    \(y=-\sqrt{4x^3+5}\)

    y is negative at x = 1, so take the negative root.

  5. At x = 2

    \(y=-\sqrt{37}=-6.08\)

Video walkthrough coming
An implicit solution and two values

Given \(\dfrac{dy}{dx}=\dfrac{2\sin x}{\sin y}\), show that the general solution is \(\cos y-2\cos x=c\). A solution has \(y=\dfrac\pi3\) when \(x=\dfrac\pi2\). For \(0\le x\le\pi\) and \(-\pi\le y\le\pi\), find the positive value of \(y\) when \(x=\dfrac{2\pi}{3}\), to 3 significant figures.

Working
  1. Separate

    \(\int\sin y\,dy=\int2\sin x\,dx\)

    Multiply by sin y.

  2. Integrate

    \(-\cos y=-2\cos x+c_1\)

  3. Rearrange

    \(\cos y-2\cos x=c\)

    c = −c₁. This is the result to be shown.

  4. Use the point

    \(\cos\tfrac\pi3-2\cos\tfrac\pi2=\tfrac12\ \Rightarrow\ c=\tfrac12\)

  5. At x = 2π/3

    \(\cos y=\tfrac12+2\cos\tfrac{2\pi}{3}=-\tfrac12\)

  6. Two values in the domain

    \(y=\pm\dfrac{2\pi}{3}=\pm2.09\)

    Both lie in −π ≤ y ≤ π. The positive one is 2.09.

Video walkthrough coming