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Suppose f(x) is an otherwise continuous function, but has a point removed. Such a discontinuity is called a removable discontinuity because if the point is returned there is a continuous function again. Here is one way to zap a point. Let g(x) be defined as

g(x)=\left( \cfrac{x-c}{x-c} \right)f(x)

The point at x=c cannot be in the domain of g(x) because that would imply division by zero. The factor in front can be canceled otherwise when x is not equal to c.

\includegraphics[width= 5in]{../images/FunctionHole.pdf}

\caption{A hole in an otherwise continuous function is drawn with an open circle.}


Example 1. With f(x) everywhere a continuous function and g(x) defined as above, calculate

\mathop{\lim }\limits_{x\to c} g(x)=\mathop{\lim }\limits_{x\to c} \left(\cfrac{x-c}{x-c} \right)f(x)

Solution 1. We can use the properties of limits and continuity of f(x) to write

\mathop{\lim }\limits_{x\to c} g(x)=\mathop{\lim }\limits_{x\to c} \cfrac{x-c}{x-c} f(x)=\mathop{\lim }\limits_{x\to c} \cfrac{x-c}{x-c} \mathop{\lim }\limits_{x\to c} f(x)=\mathop{\lim }\limits_{x\to c} \cfrac{x-c}{x-c} \mathop{\lim }\limits_{x\to c} f(c)=f(c)

When in doubt, calculate the left and right hand limits and see if they are equal.

{\mathop{\lim }\limits_{x\to c^{+} } \cfrac{x-c}{x-c} =\mathop{\lim }\limits_{\varepsilon \to 0^{+} } \cfrac{c+\varepsilon -c}{c+\varepsilon -c} =\mathop{\lim }\limits_{\varepsilon \to 0^{+} } \cfrac{\varepsilon }{\varepsilon } =1} \\ {\mathop{\lim }\limits_{x\to c^{-} } \cfrac{x-c}{x-c} =\mathop{\lim }\limits_{\varepsilon \to 0^{+} } \cfrac{c-\varepsilon -c}{c-\varepsilon -c} =\mathop{\lim }\limits_{\varepsilon \to 0^{+} } \cfrac{-\varepsilon }{-\varepsilon } =1}

Again I have I have used in the first equation the fact that

\mathop{\lim }\limits_{x\to c^{+} } f(x)=\mathop{\lim }\limits_{\varepsilon \to 0^{+} } f(c+\varepsilon )

This substitution with epsilon always as a positive number can help us keep the sign of the calculation straight. Since the left hand and right hand limits are equal and have the value one we can say.

\mathop{\lim }\limits_{x\to c} g(x)=f(c)

We have found a situation where there is a hole in a function but we get the same result as if the function was continuous there. Also since we have shown that the limit of a product of functions is the product of limits, then we have proved a useful theorem which we can call the cancellation theorem.



Theorem 1. If f(x) is any function such that

\mathop{\lim }\limits_{x\to c} f(x)

exists then

\mathop{\lim }\limits_{x\to c} \cfrac{x-c}{x-c} f(x)=\mathop{\lim}\limits_{x\to c} f(x)


Example 2. If g(x) is the function

g(x)=\mathop{\lim }\limits_{x\to c} \cfrac{(x-c)^{3} }{(x-c)^{3} } f(x)

Solution 2. Since the limit of a product can be written as a product of limits we can write.

 {\mathop{\lim }\limits_{x\to c} \cfrac{(x-c)^{3} }{(x-c)^{3} } f(x)} = {\mathop{\lim }\limits_{x\to c} \cfrac{x-c}{x-c} \mathop{\lim }\limits_{x\to c} \cfrac{x-c}{x-c} \mathop{\lim }\limits_{x\to c} \cfrac{x-c}{x-c} \mathop{\lim }\limits_{x\to c} f(x)} \\ = {\mathop{\lim }\limits_{x\to c} f(x)}

The same holds for any integer of the prefactor provided

\mathop{\lim }\limits_{x\to c} f(x)

exists.


Example 3. Calculate the following limit using the limit cancellation theorem

\mathop{\lim }\limits_{x\to 1} f(x)=\mathop{\lim }\limits_{x\to 1} \cfrac{x^{3} -1}{x-1}

Solution 3. A direct substitution of x = 1 results in an indeterminate form 0/0. This will require further analysis. First factor the expression then use the limit cancellation theorem.

 {L}={\mathop{\lim }\limits_{x\to 1} \cfrac{(x-1)(x^{2} +x+1)}{(x-1)} } \\ {} ={\mathop{\lim }\limits_{x\to 1} (x^{2} +x+1)} \\={3}

These examples should give an intuitive sense of when factors are cancelable.

Another case where we can’t use continuity to evaluate a limit is when a jump discontinuity occurs. An example of such a function with a jump discontinuity is the step function defined as

 \theta (x)=\left\{ \begin{array}{l} 1 \quad x\ge 0 \\ 0 \quad x<0 \end{array}\right.


Example 4. Find

\mathop{\lim }\limits_{x\to 0} \theta (x)

Solution 4. The function jumps directly from zero to one at x = 0 so we don’t expect there to be a limit there. To prove this, we examine the one sided limits at x = 0.

\mathop{\lim }\limits_{x\to 0^{-} } \theta (x)=0\quad \quad \mathop{\lim }\limits_{x\to 0^{+} } \theta (x)=1

Since the one sided limits are different we say that the limit does not exist.

\mathop{\lim }\limits_{x\to 0} \theta (x) = DNE


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