Module 8 - Continuity | ||||||||||
Introduction | Lesson 1 | Lesson 2 | Lesson 3 | Self Test | ||||||||||
Lesson 8.2: Types of Discontinuities | ||||||||||
The discontinuity you investigated in Lesson 8.1 is called a removable discontinuity because it can be removed by redefining the function to fill a hole in the graph. In this lesson you will examine three other types of discontinuities: jump, oscillating, and infinite. A Jump Discontinuity
The function
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![]() The function is not continuous at x = 0 because x = 0 is not in the domain of the function.
The function is said to have a jump discontinuity because it jumps from y = -1 to y = 1 at x = 0. The left- and right-hand limits are defined as x approaches 0, but
![]() For any jump discontinuity, the one-sided limits are unequal. An Oscillating Discontinuity
The function
![]() It is hard to tell what is happening near x = 0 by looking at the graph. You can magnify a portion of the graph near x = 0 by using a feature in the Zoom menu called ZBox (Zoom Box).
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![]() This feature will allow you to magnify the region around the y-axis by drawing a box around the part of the window you want to magnify.
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You should see the outline of a box evolve as you move the cursor. ![]()
The region inside the box is magnified to fill the entire viewing screen. ![]() The Zoom Box feature magnifies the graph by adjusting the Window values to match the box corner coordinates. This window shows even more oscillations than the previous one.
![]() ![]()
No matter how many times you zoom in, the graph will continue to oscillate between y = 1 and y = -1. In fact, there are infinitely many oscillations packed near x = 0. That is why
An Infinite Discontinuity
The function y = tan(x) has a third type of discontinuity at
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8.2.1 Based on the graph, why do you think y = tan(x) is said to have an infinite discontinuity at
Click here for the answer. |
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