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Advanced Mathematics 1

Trigonometric Identities

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Mada za sehemu hiiTrigonometryMada 7

Trigonometric identities

Consider the right-angled triangle shown in Figure 7.2.

Right-angled triangle diagram

Using Pythagoras' theorem:

AB2+BC2=AC2AB^2 + BC^2 = AC^2

Since AC=rAC = r, AB=xAB = x, and BC=yBC = y, then:

x2+y2=r2x^2 + y^2 = r^2

Divide throughout by r2r^2:

x2r2+y2r2=r2r2\frac{x^2}{r^2} + \frac{y^2}{r^2} = \frac{r^2}{r^2}

(xr)2+(yr)2=1\left(\frac{x}{r}\right)^2 + \left(\frac{y}{r}\right)^2 = 1

But cos⁡θ=xr\cos \theta = \frac{x}{r} and sin⁡θ=yr\sin \theta = \frac{y}{r}.

Substituting the values for cos⁡θ\cos \theta and sin⁡θ\sin \theta gives:

cos⁡2θ+sin⁡2θ=1(7.1)\cos^2 \theta + \sin^2 \theta = 1 \quad (7.1)

Two similar identities can be deduced from equation (7.1) as follows:

Divide by sin⁡2θ\sin^2 \theta both sides of equation (7.1):

cos⁡2θsin⁡2θ+sin⁡2θsin⁡2θ=1sin⁡2θ\frac{\cos^2 \theta}{\sin^2 \theta} + \frac{\sin^2 \theta}{\sin^2 \theta} = \frac{1}{\sin^2 \theta}

whereas, cot⁡θ=cos⁡θsin⁡θ\cot \theta = \frac{\cos \theta}{\sin \theta}

cot⁡2θ+1=csc⁡2θ(7.2)\cot^2 \theta + 1 = \csc^2 \theta \quad (7.2)

Again, divide by cos⁡2θ\cos^2 \theta both sides of equation (7.1):

cos⁡2θcos⁡2θ+sin⁡2θcos⁡2θ=1cos⁡2θ\frac{\cos^2 \theta}{\cos^2 \theta} + \frac{\sin^2 \theta}{\cos^2 \theta} = \frac{1}{\cos^2 \theta}

whereas, tan⁡θ=sin⁡θcos⁡θ\tan \theta = \frac{\sin \theta}{\cos \theta}

1+tan⁡2θ=sec⁡2θ(7.3)1 + \tan^2 \theta = \sec^2 \theta \quad (7.3)

Equations (7.1), (7.2), and (7.3) are also known as Pythagorean identities as they express the Pythagorean theorem in terms of trigonometric functions.

Example 1

Simplify sin⁡θ+cos⁡θcot⁡θ\sin \theta + \cos \theta \cot \theta.

Solution:

sin⁡θ+cos⁡θcot⁡θ=sin⁡θ+cos⁡θcos⁡θsin⁡θ\sin \theta + \cos \theta \cot \theta = \sin \theta + \cos \theta \frac{\cos \theta}{\sin \theta}

=sin⁡2θ+cos⁡2θsin⁡θ= \frac{\sin^2 \theta + \cos^2 \theta}{\sin \theta}

Since sin⁡2θ+cos⁡2θ=1\sin^2 \theta + \cos^2 \theta = 1,

=1sin⁡θ= \frac{1}{\sin \theta}

=csc⁡θ= \csc \theta

Therefore, sin⁡θ+cos⁡θcot⁡θ=csc⁡θ\sin \theta + \cos \theta \cot \theta = \csc \theta.

Example 2

If x=sin⁡θx = \sin \theta, then show that tan⁡θ=x1−x2\tan \theta = \frac{x}{\sqrt{1 - x^2}}.

Solution:

Given x=sin⁡θx = \sin \theta

sin⁡θ=x\sin \theta = x

sin⁡2θ=x2\sin^2 \theta = x^2

Since 1−sin⁡2θ=cos⁡2θ1 - \sin^2 \theta = \cos^2 \theta,

cos⁡2θ=1−x2\cos^2 \theta = 1 - x^2

cos⁡θ=1−x2\cos \theta = \sqrt{1 - x^2}

tan⁡θ=sin⁡θcos⁡θ=x1−x2\tan \theta = \frac{\sin \theta}{\cos \theta} = \frac{x}{\sqrt{1 - x^2}}

Therefore, if x=sin⁡θx = \sin \theta, then tan⁡θ=x1−x2\tan \theta = \frac{x}{\sqrt{1 - x^2}}.

Example 3

Solve the equation 2sin⁡2θ−1=cos⁡θ2\sin^2 \theta - 1 = \cos \theta, for values of θ\theta between 0° and 360°.

Solution:

Given 2sin⁡2θ−1=cos⁡θ2\sin^2 \theta - 1 = \cos \theta

2sin⁡2θ−cos⁡θ−1=02\sin^2 \theta - \cos \theta - 1 = 0

But sin⁡2θ=1−cos⁡2θ\sin^2 \theta = 1 - \cos^2 \theta, thus,

2(1−cos⁡2θ)−cos⁡θ−1=02(1 - \cos^2 \theta) - \cos \theta - 1 = 0

2−2cos⁡2θ−cos⁡θ−1=02 - 2\cos^2 \theta - \cos \theta - 1 = 0

−2cos⁡2θ−cos⁡θ+1=0-2\cos^2 \theta - \cos \theta + 1 = 0

2cos⁡2θ+cos⁡θ−1=02\cos^2 \theta + \cos \theta - 1 = 0

Factorizing the resulted quadratic equation gives:

(2cos⁡θ−1)(cos⁡θ+1)=0(2\cos \theta - 1)(\cos \theta + 1) = 0

Hence 2cos⁡θ−1=02\cos \theta - 1 = 0 or cos⁡θ+1=0\cos \theta + 1 = 0

cos⁡θ=12orcos⁡θ=−1\cos \theta = \frac{1}{2} \quad \text{or} \quad \cos \theta = -1

If cos⁡θ=12\cos \theta = \frac{1}{2}, θ=60∘,300∘\theta = 60^\circ, 300^\circ.

If cos⁡θ=−1\cos \theta = -1, θ=180∘\theta = 180^\circ.

Therefore, the values of θ\theta between 0° and 360° are 60°, 180°, and 300°.

Example 4

Solve the equation 4cos⁡θ−3sec⁡θ=2tan⁡θ4\cos \theta - 3\sec \theta = 2\tan \theta, for 0∘≤θ≤180∘0^\circ \le \theta \le 180^\circ.

Solution:

Given 4cos⁡θ−3sec⁡θ=2tan⁡θ4\cos \theta - 3\sec \theta = 2\tan \theta

4cos⁡θ−3cos⁡θ=2sin⁡θcos⁡θ4\cos \theta - \frac{3}{\cos \theta} = \frac{2\sin \theta}{\cos \theta}

Multiplying both sides by cos⁡θ\cos \theta gives:

4cos⁡2θ−3=2sin⁡θ4\cos^2 \theta - 3 = 2\sin \theta

4cos⁡2θ−2sin⁡θ−3=04\cos^2 \theta - 2\sin \theta - 3 = 0

But cos⁡2θ=1−sin⁡2θ\cos^2 \theta = 1 - \sin^2 \theta

4(1−sin⁡2θ)−2sin⁡θ−3=04(1 - \sin^2 \theta) - 2\sin \theta - 3 = 0

4−4sin⁡2θ−2sin⁡θ−3=04 - 4\sin^2 \theta - 2\sin \theta - 3 = 0

−4sin⁡2θ−2sin⁡θ+1=0-4\sin^2 \theta - 2\sin \theta + 1 = 0

4sin⁡2θ+2sin⁡θ−1=04\sin^2 \theta + 2\sin \theta - 1 = 0

Using the quadratic formula for sin⁡θ\sin \theta:

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