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Advanced Mathematics 1

Trigonometric Equation of The Form

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Majadiliano
Mada za sehemu hiiTrigonometryMada 7

Trigonometric equations of the form acos⁡θ+bsin⁡θ=ca\cos\theta + b\sin\theta = c

Trigonometric equations of the form acos⁡θ+bsin⁡θ=ca\cos\theta + b\sin\theta = c, where a, b, and c are real numbers, can be solved by using t-formulae or by expressing it in the form of Rcos⁡(θ±α)=cR\cos(\theta \pm \alpha) = c or Rsin⁡(θ±α)=cR\sin(\theta \pm \alpha) = c.

Using t-formulae

Recall the double angle formulae:

  1. sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x \cos x
  2. cos⁡2x=cos⁡2x−sin⁡2x\cos 2x = \cos^2 x - \sin^2 x

Both equations for sin⁡2x\sin 2x and cos⁡2x\cos 2x can be expressed in terms of tan⁡θ2\tan \frac{\theta}{2}.

From sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x \cos x:

sin⁡2x=2sin⁡xcos⁡x1=2sin⁡xcos⁡xcos⁡2x+sin⁡2x=2sin⁡xcos⁡x1+sin⁡2xcos⁡2x=2tan⁡x1+tan⁡2x\sin 2x = \frac{2\sin x \cos x}{1} = \frac{2\sin x \cos x}{\cos^2 x + \sin^2 x} = \frac{\frac{2\sin x}{\cos x}}{1 + \frac{\sin^2 x}{\cos^2 x}} = \frac{2\tan x}{1 + \tan^2 x}

Therefore, sin⁡2x=2tan⁡x1+tan⁡2x\sin 2x = \frac{2\tan x}{1 + \tan^2 x} (7.7)

Now, let θ=2x\theta = 2x, then x=θ2x = \frac{\theta}{2}, equation (7.7) becomes:

sin⁡θ=2tan⁡θ21+tan⁡2θ2\sin \theta = \frac{2\tan\frac{\theta}{2}}{1 + \tan^2\frac{\theta}{2}}

Let t=tan⁡θ2t = \tan\frac{\theta}{2}, then sin⁡θ=2t1+t2\sin \theta = \frac{2t}{1 + t^2}. This is called the t-formula for sin⁡θ\sin\theta.

Example 1

Solve the equation 5cos⁡θ−2sin⁡θ=25\cos \theta - 2\sin \theta = 2 for 0∘≤θ≤360∘0^\circ \le \theta \le 360^\circ by using the substitution t=tan⁡θ2t = \tan\frac{\theta}{2}.

Solution:

Substituting the t-formulae into the equation:

5(1−t21+t2)−2(2t1+t2)=25\left(\frac{1 - t^2}{1 + t^2}\right) - 2\left(\frac{2t}{1 + t^2}\right) = 2

5(1−t2)−4t=2(1+t2)5(1 - t^2) - 4t = 2(1 + t^2)

5−5t2−4t=2+2t25 - 5t^2 - 4t = 2 + 2t^2

7t2+4t−3=07t^2 + 4t - 3 = 0

(7t−3)(t+1)=0(7t - 3)(t + 1) = 0

t=37 or t=−1t = \frac{3}{7} \text{ or } t = -1

If t=37t = \frac{3}{7}, tan⁡θ2=37\tan\frac{\theta}{2} = \frac{3}{7}, so θ2≈23.2∘\frac{\theta}{2} \approx 23.2^\circ, and θ≈46.4∘\theta \approx 46.4^\circ or 180∘+46.4∘=226.4∘180^\circ + 46.4^\circ = 226.4^\circ

If t=−1t = -1, tan⁡θ2=−1\tan\frac{\theta}{2} = -1, so θ2=−45∘\frac{\theta}{2} = -45^\circ or 135∘135^\circ, and θ=−90∘\theta = -90^\circ or 270∘270^\circ.

Therefore, the solutions for 0∘≤θ≤360∘0^\circ \le \theta \le 360^\circ are approximately 46.4∘46.4^\circ and 270∘270^\circ.

Expressing acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta in the form Rcos⁡(θ±α)R\cos(\theta \pm \alpha) or Rsin⁡(θ±α)R\sin(\theta \pm \alpha)

The technique of expressing acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta in the form of Rcos⁡(θ±α)R\cos(\theta \pm \alpha) or Rsin⁡(θ±α)R\sin(\theta \pm \alpha) is useful in finding maximum and minimum values of trigonometric equations of the form acos⁡θ+bsin⁡θ=ca\cos\theta + b\sin\theta = c.

Expressing acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta in the form of Rcos⁡(θ−α)R\cos(\theta - \alpha)

Using the compound angle formula for Rcos⁡(θ−α)R\cos(\theta - \alpha) gives:

Rcos⁡(θ−α)≡acos⁡θ+bsin⁡θ≡Rcos⁡θcos⁡α+Rsin⁡θsin⁡αR\cos(\theta - \alpha) \equiv a\cos\theta + b\sin\theta \equiv R\cos\theta\cos\alpha + R\sin\theta\sin\alpha

Comparing the coefficients of cos⁡θ\cos\theta gives:

a=Rcos⁡αa = R\cos\alpha ………………………………………… (i)

Comparing the coefficients of sin⁡θ\sin\theta gives:

b=Rsin⁡αb = R\sin\alpha ………………………………………… (ii)

Squaring and adding equations (i) and (ii) gives:

a2+b2=R2cos⁡2α+R2sin⁡2αa^2 + b^2 = R^2\cos^2\alpha + R^2\sin^2\alpha

a2+b2=R2(cos⁡2α+sin⁡2α)a^2 + b^2 = R^2(\cos^2\alpha + \sin^2\alpha)

R2=a2+b2R^2 = a^2 + b^2

R=a2+b2R = \sqrt{a^2 + b^2} (where R is positive)

The value of α\alpha is obtained by dividing equation (ii) by equation (i):

tan⁡α=Rsin⁡αRcos⁡α=ba\tan\alpha = \frac{R\sin\alpha}{R\cos\alpha} = \frac{b}{a}

α=tan⁡−1(ba)\alpha = \tan^{-1}\left(\frac{b}{a}\right)

Example 2

Express 3cos⁡θ−4sin⁡θ3\cos\theta - 4\sin\theta in the form of Rcos⁡(θ−α)R\cos(\theta - \alpha).

Solution:

Let 3cos⁡θ−4sin⁡θ=Rcos⁡(θ−α)=Rcos⁡θcos⁡α+Rsin⁡θsin⁡α3\cos\theta - 4\sin\theta = R\cos(\theta - \alpha) = R\cos\theta\cos\alpha + R\sin\theta\sin\alpha

Comparing coefficients:

Rcos⁡α=3R\cos\alpha = 3

Rsin⁡α=−4R\sin\alpha = -4

R=32+(−4)2=25=5R = \sqrt{3^2 + (-4)^2} = \sqrt{25} = 5

tan⁡α=−43\tan\alpha = \frac{-4}{3}

α=tan⁡−1(−43)≈−53.1∘\alpha = \tan^{-1}\left(\frac{-4}{3}\right) \approx -53.1^\circ (or 306.9°)

Therefore, 3cos⁡θ−4sin⁡θ=5cos⁡(θ+53.1∘)3\cos\theta - 4\sin\theta = 5\cos(\theta + 53.1^\circ).

Example 3

Show that 5cos⁡θ−12sin⁡θ5\cos\theta - 12\sin\theta can be expressed in the form 13cos⁡(θ+67.4∘)13\cos(\theta + 67.4^\circ).

Solution:

Let 5cos⁡θ−12sin⁡θ=Rcos⁡(θ+α)5\cos\theta - 12\sin\theta = R\cos(\theta + \alpha)

Comparing coefficients:

Rcos⁡α=5R\cos\alpha = 5

Rsin⁡α=−12R\sin\alpha = -12

R=52+(−12)2=169=13R = \sqrt{5^2 + (-12)^2} = \sqrt{169} = 13

tan⁡α=−125\tan\alpha = \frac{-12}{5}

α≈−67.4∘\alpha \approx -67.4^\circ (or 292.6°)

Therefore, 5cos⁡θ−12sin⁡θ=13cos⁡(θ+67.4∘)5\cos\theta - 12\sin\theta = 13\cos(\theta + 67.4^\circ).

Expressing acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta in the form Rsin⁡(θ+α)R\sin(\theta + \alpha)

Using the compound angle formula for Rsin⁡(θ+α)R\sin(\theta + \alpha) gives:

acos⁡θ+bsin⁡θ=R(sin⁡θcos⁡α+cos⁡θsin⁡α)a\cos\theta + b\sin\theta = R(\sin\theta\cos\alpha + \cos\theta\sin\alpha)

Comparing coefficients:

b=Rcos⁡αb = R\cos\alpha ………………………………………… (i)

a=Rsin⁡αa = R\sin\alpha ………………………………………… (ii)

Squaring and adding equations (i) and (ii) gives:

a2+b2=R2a^2 + b^2 = R^2

R=a2+b2R = \sqrt{a^2 + b^2}

Dividing equation (ii) by equation (i) gives:

tan⁡α=ab\tan\alpha = \frac{a}{b}

α=tan⁡−1(ab)\alpha = \tan^{-1}\left(\frac{a}{b}\right)

Example 4

Express 7cos⁡θ+24sin⁡θ7\cos\theta + 24\sin\theta in the form of Rsin⁡(θ+α)R\sin(\theta + \alpha).

Solution:

Let 7cos⁡θ+24sin⁡θ=Rsin⁡(θ+α)7\cos\theta + 24\sin\theta = R\sin(\theta + \alpha)

Comparing coefficients:

Rcos⁡α=24R\cos\alpha = 24

Rsin⁡α=7R\sin\alpha = 7

R=72+242=25R = \sqrt{7^2 + 24^2} = 25

tan⁡α=724\tan\alpha = \frac{7}{24}

α≈16.3∘\alpha \approx 16.3^\circ

Therefore, 7cos⁡θ+24sin⁡θ=25sin⁡(θ+16.3∘)7\cos\theta + 24\sin\theta = 25\sin(\theta + 16.3^\circ).

Example 5

Find the maximum and minimum values of 24sin⁡θ−7cos⁡θ24\sin\theta - 7\cos\theta, stating the values of θ\theta for which the maximum and minimum values are attained.

Solution:

Let 24sin⁡θ−7cos⁡θ=Rsin⁡(θ−α)24\sin\theta - 7\cos\theta = R\sin(\theta - \alpha)

R=242+(−7)2=576+49=625=25R = \sqrt{24^2 + (-7)^2} = \sqrt{576 + 49} = \sqrt{625} = 25

tan⁡α=−724\tan\alpha = \frac{-7}{24}

α≈−16.3∘\alpha \approx -16.3^\circ

So, 24sin⁡θ−7cos⁡θ=25sin⁡(θ+16.3∘)24\sin\theta - 7\cos\theta = 25\sin(\theta + 16.3^\circ)

Since −1≤sin⁡(θ+16.3∘)≤1-1 \le \sin(\theta + 16.3^\circ) \le 1, the maximum value is 25 (when sin⁡(θ+16.3∘)=1\sin(\theta + 16.3^\circ) = 1) and the minimum value is -25 (when sin⁡(θ+16.3∘)=−1\sin(\theta + 16.3^\circ) = -1).

For the maximum value:

sin⁡(θ+16.3∘)=1\sin(\theta + 16.3^\circ) = 1

θ+16.3∘=90∘\theta + 16.3^\circ = 90^\circ

θ=73.7∘\theta = 73.7^\circ

For the minimum value:

sin⁡(θ+16.3∘)=−1\sin(\theta + 16.3^\circ) = -1

θ+16.3∘=270∘\theta + 16.3^\circ = 270^\circ

θ=253.7∘\theta = 253.7^\circ

Therefore, the maximum value is 25 at θ=73.7∘\theta = 73.7^\circ, and the minimum value is -25 at θ=253.7∘\theta = 253.7^\circ.

Example 6

Show that 13cos⁡λ+7sin⁡λ13\cos\lambda + 7\sin\lambda can be expressed in the form 218cos⁡(λ−α)\sqrt{218}\cos(\lambda - \alpha), where tan⁡α=713\tan\alpha = \frac{7}{13}. Hence, find the maximum and minimum values of the function, giving the corresponding values of λ\lambda.

Solution:

Let 13cos⁡λ+7sin⁡λ=Rcos⁡(λ−α)13\cos\lambda + 7\sin\lambda = R\cos(\lambda - \alpha)

R=132+72=169+49=218R = \sqrt{13^2 + 7^2} = \sqrt{169 + 49} = \sqrt{218}

tan⁡α=713\tan\alpha = \frac{7}{13}

α≈28.3∘\alpha \approx 28.3^\circ

So, 13cos⁡λ+7sin⁡λ=218cos⁡(λ−28.3∘)13\cos\lambda + 7\sin\lambda = \sqrt{218}\cos(\lambda - 28.3^\circ)

The maximum value is 218\sqrt{218} (when cos⁡(λ−28.3∘)=1\cos(\lambda - 28.3^\circ) = 1), and the minimum value is −218-\sqrt{218} (when cos⁡(λ−28.3∘)=−1\cos(\lambda - 28.3^\circ) = -1).

For the maximum value:

λ−28.3∘=0∘\lambda - 28.3^\circ = 0^\circ

λ=28.3∘\lambda = 28.3^\circ

For the minimum value:

λ−28.3∘=180∘\lambda - 28.3^\circ = 180^\circ

λ=208.3∘\lambda = 208.3^\circ

Example 7

Solve the equation 52=4cos⁡2x+3sin⁡2x5\sqrt{2} = 4\cos 2x + 3\sin 2x for values in the interval −180∘≤x≤180∘-180^\circ \le x \le 180^\circ.

Solution:

Let 4cos⁡2x+3sin⁡2x=Rsin⁡(2x+α)4\cos 2x + 3\sin 2x = R\sin(2x + \alpha)

R=42+32=5R = \sqrt{4^2 + 3^2} = 5

tan⁡α=43\tan\alpha = \frac{4}{3}

α≈53.1∘\alpha \approx 53.1^\circ

So, 52=5sin⁡(2x+53.1∘)5\sqrt{2} = 5\sin(2x + 53.1^\circ)

sin⁡(2x+53.1∘)=2\sin(2x + 53.1^\circ) = \sqrt{2}

Since the maximum value of sine is 1, and 2>1\sqrt{2} > 1, there are no solutions to this equation.

Example 8

Solve the equation 3cos⁡x+sin⁡x=23\cos x + \sin x = 2 for 0∘≤x≤360∘0^\circ \le x \le 360^\circ.

Solution:

Let 3cos⁡x+sin⁡x=Rcos⁡(x−α)3\cos x + \sin x = R\cos(x - \alpha)

R=32+12=10R = \sqrt{3^2 + 1^2} = \sqrt{10}

tan⁡α=13\tan\alpha = \frac{1}{3}

α≈18.4∘\alpha \approx 18.4^\circ

So, 10cos⁡(x−18.4∘)=2\sqrt{10}\cos(x - 18.4^\circ) = 2

cos⁡(x−18.4∘)=210\cos(x - 18.4^\circ) = \frac{2}{\sqrt{10}}

x−18.4∘≈±50.8∘x - 18.4^\circ \approx \pm 50.8^\circ

x≈69.2∘ or x≈−32.4∘+360∘=327.6∘x \approx 69.2^\circ \text{ or } x \approx -32.4^\circ + 360^\circ = 327.6^\circ

Therefore, the solutions are approximately x=69.2∘x = 69.2^\circ and 327.6∘327.6^\circ.

General solutions of trigonometric equations

A general solution is a solution that contains all possible solutions of a given trigonometric equation.

Consider the graph of the straight lines y=ay = a, where −1≤a≤1-1 \le a \le 1, and y=cos⁡θy = \cos \theta as shown in Figure 7.5:

Graph showing the intersection of y = a and y = cos theta

The principal value of the equation cos⁡θ=a\cos \theta = a is α=cos⁡−1a\alpha = \cos^{-1} a. Since the cosine function is periodic with a period of 360∘360^\circ or 2π2\pi radians, other solutions are obtained by adding or subtracting multiples of 360∘360^\circ or 2π2\pi to ±α\pm\alpha.

The general solution of the equation cos⁡θ=a\cos\theta = a where −1≤a≤1-1 \le a \le 1 is given as:

In degrees: θ=±α+360∘n\theta = \pm\alpha + 360^\circ n, where α=cos⁡−1a\alpha = \cos^{-1} a and n is an integer.

In radians: θ=±α+2πn\theta = \pm\alpha + 2\pi n, where α=cos⁡−1a\alpha = \cos^{-1} a and n is an integer.

Similarly, the general solutions for sine and tangent are:

In degrees:

  1. If sin⁡θ=sin⁡α\sin \theta = \sin \alpha, then θ=n180∘+(−1)nα\theta = n180^\circ + (-1)^n \alpha
  2. If tan⁡θ=tan⁡α\tan \theta = \tan \alpha, then θ=α+180∘n\theta = \alpha + 180^\circ n

In radians:

  1. If sin⁡θ=sin⁡α\sin \theta = \sin \alpha, then θ=nπ+(−1)nα\theta = n\pi + (-1)^n \alpha
  2. If tan⁡θ=tan⁡α\tan \theta = \tan \alpha, then θ=α+nπ\theta = \alpha + n\pi

where n is an integer.

Example 1

Find the general solution of the equation cos⁡x+sin⁡x=1\cos x + \sin x = 1, giving your answer in terms of π\pi.

Solution:

Express cos⁡x+sin⁡x\cos x + \sin x in the form Rcos⁡(x−α)R\cos(x - \alpha):

R=12+12=2R = \sqrt{1^2 + 1^2} = \sqrt{2}

tan⁡α=11=1, so α=π4\tan\alpha = \frac{1}{1} = 1, \text{ so } \alpha = \frac{\pi}{4}

The equation becomes: 2cos⁡(x−π4)=1\sqrt{2}\cos(x - \frac{\pi}{4}) = 1

cos⁡(x−π4)=12\cos(x - \frac{\pi}{4}) = \frac{1}{\sqrt{2}}

x−π4=±π4+2nπx - \frac{\pi}{4} = \pm\frac{\pi}{4} + 2n\pi

Case 1: x−π4=π4+2nπx - \frac{\pi}{4} = \frac{\pi}{4} + 2n\pi

x=π2+2nπx = \frac{\pi}{2} + 2n\pi

Case 2: x−π4=−π4+2nπx - \frac{\pi}{4} = -\frac{\pi}{4} + 2n\pi

x=2nπx = 2n\pi

Therefore, the general solutions are x=π2+2nπx = \frac{\pi}{2} + 2n\pi and x=2nπx = 2n\pi, where n is an integer.

Example 2

Find the general solution of the equation cot⁡x+csc⁡x=3\cot x + \csc x = \sqrt{3}, giving the answer in terms of π\pi.

Solution:

cos⁡xsin⁡x+1sin⁡x=3\frac{\cos x}{\sin x} + \frac{1}{\sin x} = \sqrt{3}

cos⁡x+1=3sin⁡x\cos x + 1 = \sqrt{3}\sin x

3sin⁡x−cos⁡x=1\sqrt{3}\sin x - \cos x = 1

Express 3sin⁡x−cos⁡x\sqrt{3}\sin x - \cos x in the form Rsin⁡(x−α)R\sin(x - \alpha):

R=(3)2+(−1)2=3+1=2R = \sqrt{(\sqrt{3})^2 + (-1)^2} = \sqrt{3 + 1} = 2

tan⁡α=−13, so α=−π6 or 5π6.\tan\alpha = \frac{-1}{\sqrt{3}}, \text{ so } \alpha = -\frac{\pi}{6} \text{ or } \frac{5\pi}{6}. Using the positive value is easier for this example.

The equation becomes: 2sin⁡(x−5π6)=12\sin(x - \frac{5\pi}{6}) = 1

sin⁡(x−5π6)=12\sin(x - \frac{5\pi}{6}) = \frac{1}{2}

x−5π6=nπ+(−1)nπ6x - \frac{5\pi}{6} = n\pi + (-1)^n \frac{\pi}{6}

x=nπ+(−1)nπ6+5π6x = n\pi + (-1)^n \frac{\pi}{6} + \frac{5\pi}{6}

Example 3

Use the t-formulae to find the general solution of the equation 2cos⁡x−sin⁡x=12\cos x - \sin x = 1, giving the answers in radians.

Solution:

Using the t-formulae, where t=tan⁡x2t = \tan\frac{x}{2}:

2(1−t21+t2)−2t1+t2=12\left(\frac{1 - t^2}{1 + t^2}\right) - \frac{2t}{1 + t^2} = 1

2−2t2−2t=1+t22 - 2t^2 - 2t = 1 + t^2

3t2+2t−1=03t^2 + 2t - 1 = 0

(3t−1)(t+1)=0(3t - 1)(t + 1) = 0

t=13 or t=−1t = \frac{1}{3} \text{ or } t = -1

Case 1: tan⁡x2=13\tan\frac{x}{2} = \frac{1}{3}

x2=arctan⁡(13)+nπ\frac{x}{2} = \arctan\left(\frac{1}{3}\right) + n\pi

x=2arctan⁡(13)+2nπ≈0.6435+2nπx = 2\arctan\left(\frac{1}{3}\right) + 2n\pi \approx 0.6435 + 2n\pi

Case 2: tan⁡x2=−1\tan\frac{x}{2} = -1

x2=−π4+nπ\frac{x}{2} = -\frac{\pi}{4} + n\pi

x=−π2+2nπx = -\frac{\pi}{2} + 2n\pi

Therefore, the general solutions are x≈0.6435+2nπx \approx 0.6435 + 2n\pi and x=−π2+2nπx = -\frac{\pi}{2} + 2n\pi, where n is an integer.

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