Issues arise when the denominator is zero, i.e., when . This leads to undefined points at . In general, any angle of the form , where is an odd integer, should be excluded from the domain since tangent is undefined at these values.
The denominator becomes zero when , corresponding to . In general, is undefined for angles of the form , where is an integer. These angles should be excluded from the domain of cotangent.
To determine the range of the tangent function, consider the point on the unit circle corresponding to the angle , and let be a real number such that .
In other words, since can be any real number and , the range of the tangent function consists of all real numbers. A similar method can be used to show that the range of the cotangent function is also the set of all real numbers.
When , corresponding to , the denominator becomes zero. In general, is undefined for angles of the form , where is an integer, and these values should be excluded from the domain.
we see that is undefined when . This occurs at , and thus any angle of the general form , where is an odd integer, should be excluded from the domain of .
In Subsection 1.5.4, we learned that the tangent function is periodic with a period of . To graph , we focus on plotting one period and then repeat those values to complete the graph.
We also know that the domain of tangent includes all real numbers except any angle of the form , where is an odd integer. These values are excluded since tangent is undefined there. In fact, any line of the form (e.g. and ) is a vertical asymptote
Knowing the location of the vertical asymptotes, we choose the interval to plot our points for tangent. This interval has a length of (one period), allowing us to repeat the values to complete the graph of tangent over the entire domain.
Recall from Definition 1.3.2 that on the unit circle, the expression denotes the ratio of the -coordinate to the -coordinate of a point associated with an angle . This ratio changes dynamically as varies from zero to .
As approaches zero, the -value tends to zero, and approaches 1, resulting in being a small fraction. Conversely, as approaches , the -value approaches 1, while becomes extremely small and near zero. This causes to evaluate as a fraction divided by a very small number, producing a large number. A similar effect occurs when is between and zero, except is negative in this range. This behavior is shown in Figure 2.2.9.
Figure2.2.9.As moves from to , this figure plots the values of . Move the slider for to see how changing the angle affects . Note that while we will generally be using radians when graphing trigonometric functions, this figure uses degrees to help visualize the angle.
Notice the symmetrical nature of the tangent function’s graph with respect to the origin, a feature explained in Section 1.5.7, where we learned that tangent is an odd function.
Since the graph in Figure 2.2.11 represents one period, we can complete the graph of by extending the pattern in both directions to obtain Figure 2.2.12.
The domain of the cotangent function is defined for all angles except those of the form , where is an integer. These excluded values correspond to vertical asymptotes. In fact, any line of the form , where is an integer, serves as a vertical asymptote. Additionally, as we learned in Subsection 1.5.4, the cotangent function has a period of . We can construct a plot for it in a manner similar to how we constructed the tangent function, as illustrated in Figure 2.2.13.
Figure2.2.13.As moves from to , this figure plots the values of . Move the slider for to see how changing the angle affects . Note that while we will generally be using radians when graphing trigonometric functions, this figure uses degrees to help visualize the angle.
The cosecant function has vertical asymptotes at points , where is an integer, corresponding to the values where the function is undefined. These points are the same ones excluded from the domain of . As discussed in Subsection 1.5.4, the cosecant function has a period of . Given this, we choose to examine its behavior within one period, specifically from to , since this interval spans one complete period of the cosecant function.
As approaches zero, sine decreases to zero, making cosecant approach positive infinity. Increasing towards , increases to , and cosecant decreases to . As moves from to , sine approaches zero, causing to approach infinity.
Similarly, for nearing , becomes a small, negative number near zero, resulting in approaching negative infinity. As increases to , decreases to , and increases to . Finally, from to , approaches a small negative number, causing cosecant to approach negative infinity. This behavior is shown in Figure 2.2.15.
Figure2.2.15.As moves from to , this figure plots the values of and . Move the slider for to see how changing the angle affects . Note that while we will generally be using radians when graphing trigonometric functions, this figure uses degrees to help visualize the angle.
Since the graph in Figure 2.2.17 represents one period, we can complete the graph of by extending the pattern in both directions to obtain Figure 2.2.18.
Notice the graph of the cosecant function is symmetric with respect to the origin, confirming what we learned in Section 1.5.7, that cosecant is an odd function.
As discussed earlier in this section, the secant function has a domain for all real numbers except angles of , where is an integer. These excluded values correspond to the vertical asymptotes of the secant function. With a period of , we can focus on the interval to . The construction of the secant function plot follows a similar approach to that used for the cosecant function, as illustrated in Figure 2.2.19.
Figure2.2.19.As moves from to , this figure plots the values of and . Move the slider for to see how changing the angle affects . Note that while we will generally be using radians when graphing trigonometric functions, this figure uses degrees to help visualize the angle.
Notice the graph of the secant function is symmetric about the -axis, and thus secant is an even function, confirming what we learned in Section 1.5.7.
Similar to the graphs of sine and cosine, the graphs of the other trigonometric functions can undergo vertical stretching and compressing, horizontal stretching and compressing, phase shifts, vertical shift transformations, and reflections about the - and -axes. However, unlike the sine and cosine functions, there is no amplitude for the other trigonometric functions. These transformations are listed in Definition 2.2.21.
the transformations are the same as above, except for the phase shift and vertical asymptotes where you replace with . If the phase shift is to the right, and if it is to the left.
Figure2.2.24.The transformations of the tangent function graph, starting with a baseline of along with graphs with a vertical stretch, a vertical compression, and a reflection about the -axis.
Figure2.2.26.The transformations of the cotangent function graph, starting with a baseline of along with graphs with a horizontal stretch, a horizontal compression, and a reflection about the -axis.
Figure2.2.29.Manipulate the graphs of tangent and cotangent by adjusting the sliders for ,,, and . Observe the effects on period, phase and vertical shifts, as well as reflections about the - and -axes. Additionally, you can toggle between the tangent and cotangent graphs by selecting the corresponding function.
Figure2.2.30.Manipulate the graphs of cosecant and secant by adjusting the sliders for ,,, and . Observe the effects on period, phase and vertical shifts, as well as reflections about the - and -axes. Additionally, you can toggle between the cosecant and secant graphs by selecting the corresponding function.
When navigating the open ocean, maintaining a straight course poses challenges due to limited visual markers. One technique involves the steersperson using the positions of shadows cast by objects on the canoe—such as crew members, railings, and sails—to keep them fixed on the deck, ensuring a straight trajectory. However, if the canoe veers off course, the changing position of the canoe relative to the sun leads to a shift in the shadows. Observing these shadow movements allows the steersperson to make course corrections. It’s important to note that this method is effective only over a short duration, as the sun’s continuous movement across the sky causes ongoing changes in shadow positions. To illustrate the limitations over extended periods, consider the example of the Samoan double-hulled voyaging vaʻa, Gaualofa, with a 14-meter-high mast. The length of the shadow is modeled by
where is the shadow length in meters and represents the hours since 6 am (assuming sunrise at 6 am and sunset at 6 pm). In each of the following questions, calculate the length of the shadow, rounded to the nearest tenth of a meter, for the given time.
An observer on Rangiroa spots the Faʻafaite, a double-hulled voyaging canoe from Tahiti, sailing off the north coast of the atoll, maintaining a distance of three nautical miles from the shore and traveling east. Let represent the angle formed between the line from the observer to the vaʻa and a line extending due north from the observer, measured in radians. The angle is negative if the vaʻa is to the left of the observer and positive when to the right, as shown in the figure above. The distance (in nautical miles), denoted by from Faʻafaite to the observer is given by the function
In each of the following questions, calculate the distance from the observer to Faʻafaite, , in nautical miles, for the given angle . Round your answer to two decimal places.