Reciprocal trigonometric ratios
A stay wire runs from the top of a radio mast near Athlone down to the ground, 15 m from the base of the mast. The wire makes an angle $\alpha$ with the ground, so its length is $15\sec\alpha$. If all you know is that $\cot\alpha = \frac{3}{4}$, can you find the length of the wire? We will answer this at the end.
Sine, cosine and tangent each have a "partner": their reciprocal. They are just inverted fractions, but they are worth mastering because they save steps when you simplify expressions and solve equations.
Three new ratios: secant, cosecant and cotangent
Each of the three new ratios is, by definition, the reciprocal of one of the ratios you already know.
Given that $\sin \alpha = \frac{3}{5}$ and that $\alpha$ is an angle in the first quadrant, calculate the exact value of $\csc \alpha$ and $\sec \alpha$.
Given that $\sin \alpha = \frac{3}{5}$ and that $\alpha$ is an angle in the first quadrant, calculate the exact value of $\csc \alpha$ and $\sec \alpha$.
Consider the acute angle $\alpha = 85^\circ$. a) Without using a calculator to obtain the numerical value, reasonably estimate whether $\sec(85^\circ)$ will be a number…
Consider the acute angle $\alpha = 85^\circ$.
- a) Without using a calculator to obtain the numerical value, reasonably estimate whether $\sec(85^\circ)$ will be a number less than $1$, close to $1$, or much greater than $1$. Justify your prediction by analysing what happens to the value of $\cos \alpha$ on the unit circle as $\alpha$ approaches $90^\circ$ and taking into account the definition $\sec \alpha = \frac{1}{\cos \alpha}$.
- b) Knowing that $\cos(85^\circ) \approx 0.0872$, calculate the value of $\sec(85^\circ)$ rounded to two decimal places and check whether your qualitative estimation was correct.
- c) Based on this behaviour, is it possible to find any real angle $\theta$ such that $\sec \theta = 0.5$? Justify your answer from the range of values that the cosine function can take.
Exact values of the reciprocal ratios
Since they are direct reciprocals, the exact values of secant, cosecant and cotangent come from inverting the table of sine, cosine and tangent that you already know.
For other angles, use the reference angle and the sign from the CAST diagram. Remember also that $30°=\frac{\pi}{6}$, $45°=\frac{\pi}{4}$ and $60°=\frac{\pi}{3}$.
Determine the exact value of $\sec 60^\circ$ and $\cot 45^\circ$ without using a calculator.
Determine the exact value of $\sec 60^\circ$ and $\cot 45^\circ$ without using a calculator.
Calculate the exact value of $\cot \frac{\pi}{6}$ and $\csc \frac{\pi}{4}$.
Calculate the exact value of $\cot \frac{\pi}{6}$ and $\csc \frac{\pi}{4}$.
Evaluate the following expression giving its exact value, without using decimal approximations: $\sec(120^\circ) + \csc(210^\circ) - \cot(315^\circ)$.
Evaluate the following expression giving its exact value, without using decimal approximations: $\sec(120^\circ) + \csc(210^\circ) - \cot(315^\circ)$.
Pythagorean identities with the reciprocals
The fundamental identity $\sin^2\alpha+\cos^2\alpha=1$ has two "reciprocal" versions, which are obtained by dividing the whole equation by $\cos^2\alpha$ or by $\sin^2\alpha$.
If $\tan \beta = \frac{4}{3}$ and $0 < \beta < \frac{\pi}{2}$, use the fundamental identity $1 + \tan^2 \beta = \sec^2 \beta$ to calculate $\sec \beta$.
If $\tan \beta = \frac{4}{3}$ and $0 < \beta < \frac{\pi}{2}$, use the fundamental identity $1 + \tan^2 \beta = \sec^2 \beta$ to calculate $\sec \beta$.
Given that $\cos \theta = \frac{1}{3}$, calculate the exact numerical value of the expression $\sec^2 \theta - 1$.
Given that $\cos \theta = \frac{1}{3}$, calculate the exact numerical value of the expression $\sec^2 \theta - 1$.
Given that $\sec \alpha = -\frac{13}{5}$ and that $\pi < \alpha < \frac{3\pi}{2}$, calculate the exact value of the remaining trigonometric ratios (sine, cosine,…
Given that $\sec \alpha = -\frac{13}{5}$ and that $\pi < \alpha < \frac{3\pi}{2}$, calculate the exact value of the remaining trigonometric ratios (sine, cosine, tangent, cosecant and cotangent).
Sign and existence by quadrant
Since $\sec\alpha$ has the same sign as $\cos\alpha$, and $\csc\alpha$ and $\cot\alpha$ have the same sign as $\sin\alpha$ and $\tan\alpha$ respectively, the table of signs for the three original ratios also works for the reciprocals, without learning anything new.
An angle $\gamma$ satisfies $\sec \gamma < 0$ and $\csc \gamma > 0$. Determine, with reasons, which quadrant of the unit circle the angle $\gamma$ lies in.
An angle $\gamma$ satisfies $\sec \gamma < 0$ and $\csc \gamma > 0$. Determine, with reasons, which quadrant of the unit circle the angle $\gamma$ lies in.
If $\cot \alpha = 2$ and $\alpha$ belongs to the third quadrant, determine the sign and exact value of $\tan \alpha$ and $\csc \alpha$.
If $\cot \alpha = 2$ and $\alpha$ belongs to the third quadrant, determine the sign and exact value of $\tan \alpha$ and $\csc \alpha$.
Given that $\csc x = 3$ and that the angle $x$ belongs to the second quadrant, calculate the exact value of the expression $E = \frac{\sec x + \tan x}{\cot x}$.
Given that $\csc x = 3$ and that the angle $x$ belongs to the second quadrant, calculate the exact value of the expression $E = \frac{\sec x + \tan x}{\cot x}$.
Simplifying expressions and proving identities
To simplify expressions involving reciprocal ratios, it is best to convert everything to sine and cosine: this is usually the shortest route to getting factors to cancel.
Simplify the following trigonometric expression as much as possible: $\cos x \times \sec x + \sin x \times \csc x$.
Simplify the following trigonometric expression as much as possible: $\cos x \times \sec x + \sin x \times \csc x$.
Simplify the following trigonometric expression to obtain a single ratio: $\frac{\sec x}{\csc x} \times \cot^2 x$.
Simplify the following trigonometric expression to obtain a single ratio: $\frac{\sec x}{\csc x} \times \cot^2 x$.
Prove the following trigonometric identity: $\frac{1}{\sec x + \tan x} = \sec x - \tan x$.
Prove the following trigonometric identity: $\frac{1}{\sec x + \tan x} = \sec x - \tan x$.
Solving equations
To solve an equation with secants, cosecants or cotangents, rewrite it with $\sin$, $\cos$ or $\tan$, solve as usual, then use the CAST diagram to list every solution in the given interval.
For a system such as $\csc x+\sec y=4$ and $\csc x-\sec y=2$, treat $\csc x$ and $\sec y$ as the two unknowns: adding gives $\csc x=3$ and subtracting gives $\sec y=1$. Then solve for $x$ and $y$.
Solve the following trigonometric equation, stating all solutions in the interval $[0, 2\pi]$: $2\csc x + 4 = 0$.
Solve the following trigonometric equation, stating all solutions in the interval $[0, 2\pi]$: $2\csc x + 4 = 0$.
Solve the trigonometric equation $\sec^2 x + \tan x = 3$ in the interval $[0^\circ, 360^\circ)$.
Solve the trigonometric equation $\sec^2 x + \tan x = 3$ in the interval $[0^\circ, 360^\circ)$.
Determine all values of $x \in [0, 2\pi)$ satisfying the trigonometric equation $\csc x + \cot x = \sqrt{3}$.
Determine all values of $x \in [0, 2\pi)$ satisfying the trigonometric equation $\csc x + \cot x = \sqrt{3}$.
Reciprocals in triangles and in physics
In a right-angled triangle, $\sec\alpha=\dfrac{\text{hypotenuse}}{\text{adjacent}}$, $\csc\alpha=\dfrac{\text{hypotenuse}}{\text{opposite}}$ and $\cot\alpha=\dfrac{\text{adjacent}}{\text{opposite}}$. So they give lengths in one step: the hypotenuse is the adjacent side times $\sec\alpha$, or the opposite side times $\csc\alpha$.
The angles $\theta$ and $\beta=90°-\theta$ are complementary, so $\tan\theta=\cot\beta$.
Back to the beginning: Since $\cot\alpha=\frac{3}{4}$, we have $\tan\alpha=\frac{4}{3}$. Then $\sec^2\alpha=1+\frac{16}{9}=\frac{25}{9}$, so $\sec\alpha=\frac53$ (acute angle). The wire has length $15\cdot\frac{5}{3}=25$ m.
A spotlight illuminates a wall from the ground. The horizontal distance from the spotlight to the base of the wall is $10$ m. The upper light ray forms an angle $\alpha$…
A spotlight illuminates a wall from the ground. The horizontal distance from the spotlight to the base of the wall is $10$ m. The upper light ray forms an angle $\alpha$ with the ground. The length of the light ray from the spotlight to the highest illuminated point on the wall is $L$. Express $L$ using the secant ratio and calculate its exact value if $\cot \alpha = \frac{3}{4}$.
In solar photovoltaic installations in the west of Ireland, the relative air mass ($AM$) models the relative path length that direct radiation travels through the…
In solar photovoltaic installations in the west of Ireland, the relative air mass ($AM$) models the relative path length that direct radiation travels through the Earth's atmosphere. For zenith angles $\theta$ not too close to the horizon ($0^\circ \le \theta \le 75^\circ$), the approximation $AM = \sec \theta$ is used. The zenith angle $\theta$ and the solar elevation angle above the ground $\beta$ are complementary, that is, $\theta + \beta = 90^\circ$.
In a measurement taken at a weather station in Galway, it is recorded that the cotangent of the solar elevation angle is $\cot \beta = \frac{4}{3}$.
- a) Prove algebraically, from the definitions of the reciprocal trigonometric functions and the trigonometric ratios of complementary angles, that $\sec \theta = \csc \beta$.
- b) Without calculating the angle value in degrees and using only the Pythagorean identities from this topic, determine the exact value of the air mass $AM$ at that station.
- c) Interpret mathematically what happens to the expression $AM = \sec \theta$ when the Sun is located exactly on the horizon (sunset, $\beta = 0^\circ$, which corresponds to $\theta = 90^\circ$). Explain why this model ceases to be applicable at that moment.
In an optics experiment, a laser beam passes through a glass block with flat, parallel faces. The path of the beam inside the glass has length…
In an optics experiment, a laser beam passes through a glass block with flat, parallel faces. The path of the beam inside the glass has length $L = h \times \sec \theta_r$, where $h = 5$ cm is the thickness of the block and $\theta_r$ is the angle of refraction. If the ray is incident from air at an angle $\theta_i = 60^\circ$ and the refractive index of the glass is $n = \sqrt{2}$, calculate the exact length $L$ travelled by the laser inside the block. (Note: Snell's law states that $\sin \theta_i = n \times \sin \theta_r$).