Differential-Equations Β· Unit 8 Β· Video 1 Β· Interactive Practice

Cartesian Method: Rationalise, Then Take the Real Part

IKey Formulas

FormulaNameRole
y~=11+i(Ο‰/k) eiΟ‰t,y=Re(y~)\tilde{y} = \dfrac{1}{1 + i(\omega/k)}\,e^{i\omega t},\quad y = \mathrm{Re}(\tilde{y})Complex solutionSolves y~β€²+ky~=keiΟ‰t\tilde{y}' + k\tilde{y} = k e^{i\omega t}; its real part solves yβ€²+ky=kcos⁑ωty' + ky = k\cos\omega t
11+i(Ο‰/k)=1βˆ’i(Ο‰/k)1+(Ο‰/k)2\dfrac{1}{1 + i(\omega/k)} = \dfrac{1 - i(\omega/k)}{1 + (\omega/k)^2}RationaliseMultiply top and bottom by the conjugate 1βˆ’i(Ο‰/k)1 - i(\omega/k)
eiΟ‰t=cos⁑ωt+isin⁑ωte^{i\omega t} = \cos\omega t + i\sin\omega tEuler's definitionPuts the exponential in Cartesian form
y=cos⁑ωt+(Ο‰/k)sin⁑ωt1+(Ο‰/k)2y = \dfrac{\cos\omega t + (\omega/k)\sin\omega t}{1 + (\omega/k)^2}Cartesian answerA cosine plus a multiple of a sine, same frequency Ο‰\omega

Key Insight: Of the four terms in (1βˆ’iΟ‰k)(cos⁑ωt+isin⁑ωt)\left(1 - i\frac{\omega}{k}\right)(\cos\omega t + i\sin\omega t), only two are real β€” and in the last one the minus from the conjugate and the minus from i2=βˆ’1i^2 = -1 cancel, giving +Ο‰ksin⁑ωt+\frac{\omega}{k}\sin\omega t.

IIVisualization 1 β€” Multiply by the Conjugate

Multiplying Ξ±=1+i(Ο‰/k)\alpha = 1 + i(\omega/k) by its conjugate Ξ±Λ‰\bar{\alpha} lands on the real axis at 1+(Ο‰/k)21 + (\omega/k)^2.

IIIVisualization 2 β€” Two of the Four Terms Are Real

In (1βˆ’iΟ‰k)(cos⁑ωt+isin⁑ωt)\left(1 - i\frac{\omega}{k}\right)(\cos\omega t + i\sin\omega t), the terms with no factor of ii or two factors of ii are real.

IVVisualization 3 β€” Same Curve, Two Formulas

The Cartesian sum and the polar single cosine trace one curve; only the polar form displays its amplitude and lag.

πŸ’‘ Reading the amplitude and the lag straight off cos⁑ωt+(Ο‰/k)sin⁑ωt\cos\omega t + (\omega/k)\sin\omega t takes the sinusoidal identity, which the next video states.

VQuiz Questions

Problem 1 Β· Rationalise the Coefficient

Given: ω/k=2\omega/k = 2, so the coefficient of eiωte^{i\omega t} is 11+2i\dfrac{1}{1 + 2i} — write it in Cartesian form.

βœ… Correct! The denominator (1+2i)(1βˆ’2i)=1+4=5(1 + 2i)(1 - 2i) = 1 + 4 = 5 is real, and the numerator is the conjugate 1βˆ’2i1 - 2i.
❌ The reciprocal of a sum is not the sum of the reciprocals. 11+2iβ‰ 1+12i\frac{1}{1 + 2i} \neq 1 + \frac{1}{2i}; multiply top and bottom by the conjugate instead.
❌ Check the numerator. Multiplying by 1βˆ’2i1βˆ’2i\frac{1 - 2i}{1 - 2i} puts the conjugate 1βˆ’2i1 - 2i on top, not 1+2i1 + 2i.
❌ Check the denominator. (1+2i)(1βˆ’2i)=1βˆ’(2i)2=1βˆ’4i2(1 + 2i)(1 - 2i) = 1 - (2i)^2 = 1 - 4i^2, and i2=βˆ’1i^2 = -1 makes it 1+4=51 + 4 = 5, not 1βˆ’41 - 4.
❌ Not quite. Multiply top and bottom by the conjugate 1βˆ’2i1 - 2i.
Show solution

Multiply top and bottom by the conjugate of the denominator:

11+2iβ‹…1βˆ’2i1βˆ’2i=1βˆ’2i(1+2i)(1βˆ’2i).\frac{1}{1 + 2i}\cdot\frac{1 - 2i}{1 - 2i} = \frac{1 - 2i}{(1 + 2i)(1 - 2i)}.

The cross terms βˆ’2i+2i-2i + 2i cancel, and i2=βˆ’1i^2 = -1:

(1+2i)(1βˆ’2i)=1βˆ’4i2=1+4=5.(1 + 2i)(1 - 2i) = 1 - 4i^2 = 1 + 4 = 5. 11+2i=1βˆ’2i5=15βˆ’25i.\frac{1}{1 + 2i} = \frac{1 - 2i}{5} = \frac{1}{5} - \frac{2}{5}i.

This is the general formula 1βˆ’i(Ο‰/k)1+(Ο‰/k)2\frac{1 - i(\omega/k)}{1 + (\omega/k)^2} with Ο‰/k=2\omega/k = 2.

Problem 2 Β· Keep the Real Terms (Watch the Sign)

Given: Ο‰/k=3\omega/k = 3 β€” find Re[(1βˆ’3i)(cos⁑ωt+isin⁑ωt)]\mathrm{Re}\big[(1 - 3i)(\cos\omega t + i\sin\omega t)\big].

βœ… Correct! The real terms are 1β‹…cos⁑ωt1\cdot\cos\omega t and (βˆ’3i)(isin⁑ωt)=+3sin⁑ωt(-3i)(i\sin\omega t) = +3\sin\omega t.
❌ Watch the sign. (βˆ’3i)(isin⁑ωt)=βˆ’3i2sin⁑ωt=+3sin⁑ωt(-3i)(i\sin\omega t) = -3i^2\sin\omega t = +3\sin\omega t: the minus from the conjugate and the minus from i2i^2 cancel.
❌ That is the imaginary part. sin⁑ωt\sin\omega t and βˆ’3cos⁑ωt-3\cos\omega t come from the two cross terms, each carrying a single factor of ii.
❌ One real term is missing. The last term has two factors of ii, and iβ‹…i=βˆ’1i \cdot i = -1 is real.
❌ Not quite. Keep the terms with zero or two factors of ii.
Show solution

The product has four terms:

1β‹…cos⁑ωt,1β‹…isin⁑ωt,βˆ’3icos⁑ωt,βˆ’3iβ‹…isin⁑ωt.1\cdot\cos\omega t,\quad 1\cdot i\sin\omega t,\quad -3i\cos\omega t,\quad -3i\cdot i\sin\omega t.

The middle two each carry one factor of ii, so they are imaginary and drop out of the real part. The last one is βˆ’3i2sin⁑ωt=+3sin⁑ωt-3i^2\sin\omega t = +3\sin\omega t.

Re[(1βˆ’3i)(cos⁑ωt+isin⁑ωt)]=cos⁑ωt+3sin⁑ωt.\mathrm{Re}\big[(1 - 3i)(\cos\omega t + i\sin\omega t)\big] = \cos\omega t + 3\sin\omega t.

Problem 3 Β· Solve a Specific Equation

Given: yβ€²+4y=4cos⁑2ty' + 4y = 4\cos 2t β€” find the sinusoidal solution by the Cartesian method.

βœ… Correct! With Ο‰/k=12\omega/k = \frac{1}{2}, y=cos⁑2t+12sin⁑2t5/4y = \frac{\cos 2t + \frac{1}{2}\sin 2t}{5/4}.
❌ Watch the sign. The real part of (1βˆ’12i)(cos⁑2t+isin⁑2t)\left(1 - \tfrac{1}{2}i\right)(\cos 2t + i\sin 2t) is cos⁑2t+12sin⁑2t\cos 2t + \tfrac{1}{2}\sin 2t, with a plus.
❌ The real factor in front is missing. Rationalising leaves 11+(Ο‰/k)2=45\frac{1}{1 + (\omega/k)^2} = \frac{4}{5} in front of everything.
❌ Check Ο‰/k\omega/k. Here Ο‰=2\omega = 2 and k=4k = 4, so Ο‰/k=12\omega/k = \frac{1}{2}, not 22.
❌ Not quite. Identify kk and Ο‰\omega, then use y=cos⁑ωt+(Ο‰/k)sin⁑ωt1+(Ο‰/k)2y = \frac{\cos\omega t + (\omega/k)\sin\omega t}{1 + (\omega/k)^2}.
Show solution

Matching yβ€²+ky=kcos⁑ωty' + ky = k\cos\omega t gives k=4k = 4, Ο‰=2\omega = 2, so Ο‰/k=12\omega/k = \frac{1}{2}.

Rationalise:

11+12i=1βˆ’12i1+14=45(1βˆ’12i).\frac{1}{1 + \tfrac{1}{2}i} = \frac{1 - \tfrac{1}{2}i}{1 + \tfrac{1}{4}} = \frac{4}{5}\left(1 - \tfrac{1}{2}i\right).

Real part:

y=45 Re[(1βˆ’12i)(cos⁑2t+isin⁑2t)]=45(cos⁑2t+12sin⁑2t)=45cos⁑2t+25sin⁑2t.y = \frac{4}{5}\,\mathrm{Re}\Big[\left(1 - \tfrac{1}{2}i\right)(\cos 2t + i\sin 2t)\Big] = \frac{4}{5}\left(\cos 2t + \tfrac{1}{2}\sin 2t\right) = \frac{4}{5}\cos 2t + \frac{2}{5}\sin 2t.

Check: yβ€²=βˆ’85sin⁑2t+45cos⁑2ty' = -\frac{8}{5}\sin 2t + \frac{4}{5}\cos 2t and 4y=165cos⁑2t+85sin⁑2t4y = \frac{16}{5}\cos 2t + \frac{8}{5}\sin 2t, so yβ€²+4y=205cos⁑2t=4cos⁑2ty' + 4y = \frac{20}{5}\cos 2t = 4\cos 2t βœ“

Problem 4 Β· A Sine Input (Transfer)

Given: yβ€²+ky=ksin⁑ωty' + ky = k\sin\omega t. Since sin⁑ωt=Im(eiΟ‰t)\sin\omega t = \mathrm{Im}(e^{i\omega t}), the same y~\tilde{y} works with y=Im(y~)y = \mathrm{Im}(\tilde{y}) β€” find yy.

βœ… Correct! The imaginary terms are 1β‹…isin⁑ωt1\cdot i\sin\omega t and βˆ’iΟ‰kcos⁑ωt-i\frac{\omega}{k}\cos\omega t; here the minus survives because no i2i^2 appears.
❌ Watch the sign. The term βˆ’iΟ‰kcos⁑ωt-i\frac{\omega}{k}\cos\omega t has only one factor of ii, so nothing cancels its minus.
❌ That is the real part. It solves the cosine equation; a sine input needs the imaginary part of y~\tilde{y}.
❌ Check the denominator. Rationalising gives 1+(Ο‰/k)21 + (\omega/k)^2; the square root belongs to the polar amplitude, which multiplies a single cosine.
❌ Not quite. Keep the terms with exactly one factor of ii.
Show solution

As before,

y~=11+(Ο‰/k)2(1βˆ’iΟ‰k)(cos⁑ωt+isin⁑ωt).\tilde{y} = \frac{1}{1 + (\omega/k)^2}\left(1 - i\frac{\omega}{k}\right)(\cos\omega t + i\sin\omega t).

The front factor is real, so it stays in front. Of the four terms, the imaginary ones are the two cross terms:

1β‹…isin⁑ωtandβˆ’iΟ‰kcos⁑ωt.1\cdot i\sin\omega t \quad\text{and}\quad -i\frac{\omega}{k}\cos\omega t.

Taking their coefficients of ii:

y=Im(y~)=sin⁑ωtβˆ’(Ο‰/k)cos⁑ωt1+(Ο‰/k)2.y = \mathrm{Im}(\tilde{y}) = \frac{\sin\omega t - (\omega/k)\cos\omega t}{1 + (\omega/k)^2}.

Check: write r=ω/kr = \omega/k, so kr=ωkr = \omega and rω=kr2r\omega = kr^2. Then

yβ€²+ky=(Ο‰cos⁑ωt+rΟ‰sin⁑ωt)+(ksin⁑ωtβˆ’Ο‰cos⁑ωt)1+r2=k(1+r2)sin⁑ωt1+r2=ksin⁑ωtΒ βœ“y' + ky = \frac{(\omega\cos\omega t + r\omega\sin\omega t) + (k\sin\omega t - \omega\cos\omega t)}{1 + r^2} = \frac{k(1 + r^2)\sin\omega t}{1 + r^2} = k\sin\omega t\ \checkmark

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