Chapter 15. Slope Approximation
Volume 3, Why Slopes and More Math.
Saying precisely how to compute a quantity, defines it.
Numerical methods for calculating a number or quantity exactly or in a
limiting fashion are employed in mathematics as (computational)
definitions. Informal non-computational descriptions of numbers and
quantities have no precise role, except perhaps to supply motivation for
the computational definition. And in this motivational category falls the
previous description of slopes. This chapter provides an approximation
and then a computational definition for slopes.
-
[Play
Video] 3 minutes: Common changes of notation in the limits that
yield the slope or derivative.
Slope Calculation
[Play
Video] 4.5 minutes: Approximating Slope of a tangent line, or
taking the approximation to Limit, when possible, to give a definition
of the slope of a tangent. Saying how to compute or approximate a
number or quantity defines.
So far the slope to a curve y = f(x) at a point
(x1,y1) =
(x1,f(x1)) has been physically
or graphically associated with the slope of a short ski whose midpoint
touches a smooth - not too bumpy - curve at the point
(x1,f(x1)). The following
diagram shows or suggests how the slope of such a ski resting on the
curve at the point (x1,y1) could be
approximated by the slope of a short chord joining
(x1,y1) to a nearby second point
(x2,y2) =
(x2,f(x2)) on the curve.
h
The function $f(x)$ is assumed to be continuous at
x1 - without jumps or other discontinuity there.
Consider the following.
-
The chord or line segment joining the point $(x_1,y_1)$ to the
point $(x_2,y_2)=(x_2,f(x_2)$ has slope
\[m_{chord}=\frac{y_2-y_1}{x_2-x_1}=\frac{\Delta y}{\Delta x} \] and
equation $y=m_{chord}(x-x_1)+ y_1$. When the ski travels between
$x=x_1$ and $x=x_2$, its slope is (or should be) approximated by the
slope $m_{chord}$ of the chord, alias line segment.
-
We suppose the point $(x_1,y_1)$ is fixed in place. In other words,
suppose it is not moving. We further suppose the point $(x_2,y_2)=
(x_2,f(x_2))$ moves along the curve $y=f(x)$ towards the point
$(x_1,y_1)$. The slope $m$ of the line segment through these two
points \em should \rm approach the slope $m_{ski} =f'(x_1)$ of a ski
on the curve at $(x_1,y_1)$.
-
In the motion just described, as the point $(x_2,y_2)= (x_2,f(x_2))$
moves along the curve $y=f(x)$ towards the point $(x_1,y_1)$, the
abscissa $x_2$ should move closer to $x_1$. The difference $\Delta x
=x_2-x_1$ should also become closer and closer to zero. Thus we
expect the approximation \[ m_{ski}\approx \frac{\Delta y }{\Delta
x}= \frac{y_2-y_1}{x_2-x_1} =\frac{f(x_2)-f(x_1)}{x_2-x_1} \] to
improve when $(x_2,y_2)= (x_2,f(x_2))$ approaches $(x_1,y_1)=
(x_1,f(x_1))$ and/or as $x_2$ approaches $x_1$.
-
The continuity of $f(x)$ at $x_1$ implies the moving point
$(x_2,y_2)= (x_2,f(x_2))$ will approach the non-moving, that is fixed
point, $(x_1,y_1)= (x_1,f(x_1))$ when the abscissa $x_2$ approaches
$x_1$ or equivalently, when $\Delta x =x_2-x_1$ approaches $0$.
-
Note the arrow $\to$ will be employed as shorthand for the phrase
approaches or goes to.
If the graphical and physical expectations hold, then $m_{ski}=f'(x_1)$
should be the limiting value of $\frac{\Delta y }{\Delta x}$ as $\Delta
x$ $\to$ 0. The better and better calculation of this limit should
provide an arithmetic means for approximating the expected slope of the
ski with greater and greater accuracy to an arbitrary number of decimal
places. \em The limiting value of the segment slope should equal that of
the ski. \rm This provides the computational definition and the
mathematical one as well. See the next section.
Limit Definition of Slopes
The slope $m$ to a curve $y=f(x)$ at $x=x_1$ is defined by the limit
calculation \[ f'(x_1)=\lim_{\mbox{ $\Delta x \to 0$}}\frac{\Delta
y}{\Delta x} \] The right hand side of the above equation may be read as
the limit as $\Delta x$ approaches zero of the ratio $\frac{\Delta
y}{\Delta x}$.
Computation of right hand side $\lim_{ \Delta x \to 0 }\frac{\Delta
y}{\Delta x}$ requires the existence of a number or quantity $L$ with the
following property in the absence of units.
For each whole number $k > 0$, there exist an $n>0$ such that
\[\left|L-\frac{\Delta y}{\Delta x} \right| \le \frac12\cdot 10^{-k}\]
if $0<|\Delta x| \le \frac12\cdot 10^{-n}$.
The value $\Delta x = 0$ is excluded as division by zero is not allowed.
Note that $\Delta y = f(x_2)-f(x_1)$. In the presence of units, the
preceding requirement becomes the following.
For each whole number $k > 0$, there exist an $n>0$ such that
\[\left|L-\frac{\Delta y}{\Delta x} \right| \le \frac12\cdot
10^{-k}\cdot \frac{\mbox{units of $y$}}{\mbox{units of $x$}}\] if
$0<|\Delta x| \le \frac12\cdot 10^{-n} \cdot \mbox{(units of x)}$.
The Physical Limit
In the case of a slope, our initial conception was that the slope of a
short ski whose midpoint was placed at a point
(x1,f(x1)) of a curve y
= f(x), would give the slope of the curve there, at least
approximately. Physically, there might be some error in the placement.
The ski has to be short enough so that the slope of the curve y =
f(x) does not change too much. The idea of a limit can be
seen here in the requirement that the ski be
short enough to lie on the curve y = f(x) and not
crossing several bumps or oscillations in it.
Tangent Line Revisited
The above limit definition is motivated by the graphical expectation or
suggestion that the slope of the line segment joining the non-moving
point (x1,y1) to the moving point
(x2,y2) should approach the slope of
a tangent line at the non-moving point
(x1,y1). The tangent line should be
the limiting position of the line extending this chord. See the previous
diagram.
Tangent Line Equation
When a skier is located on a curve $y=f(x)$ at $(x_1,y_1)=(x_1,f(x_1))$,
the slope of his or her ski is assumed to lie on a tangent line. This
tangent line has - or is now assumed to have - the equation \[
y=m_{tangent}(x-x_1)+y_1 \] where $m_{tangent}=f'(x_1)$ is given by a
limit $L$ discussed above. The foregoing represents the mathematical
definition of the tangent line to curve y = f(x) at
(x1,y1) =
(x1,f(x1)).

The linear function
where
$
m_{tangent} =f'(x_1)=m_{ski}
$
provides an approximation to the value of $y = f(x)$.
This linear approximation is discussed next.
Linear Approximation
Skip, maybe, on first reading.
Suppose for a given number $k > 0$, there exist an $n>0$ such
that \[\left|L-\frac{\Delta y}{\Delta x} \right| \le \epsilon =
\frac12\cdot 10^{-k}\] whenever $|\Delta x| \le \delta=\frac12\cdot
10^{-n}$, then the following holds whenever the inequality
$|x_2-x_1|=|\Delta x| \le \frac12\cdot 10^{-n}$ is satisfied.
-
The difference $L-\frac{\Delta y}{\Delta x}=c$ for some number $c$
with magnitude $|c|\le\epsilon= \frac12\cdot 10^{-k}$. The number
$c$ will depend on $x_2$.
-
The foregoing implies \[\frac{\Delta y}{\Delta x} =L-c\] and hence
that \[{\Delta y} =L{\Delta x}- c{\Delta x}\]
-
The latter in turn implies \[ f(x_2)-y_1=y_2-y_1 =L\Delta x- c{\Delta
x}\] and \[ f(x_2)-y_1=L(\Delta x)- c{\Delta x}\] and hence \[
f(x_2)=y_1+L(\Delta x)+\mbox{an error}\] where the error is
$-c{\Delta x}$ and its magnitude \[|c\cdot \Delta x| \le |\Delta x|
\cdot \frac12\cdot 10^{-k} \le\frac12\cdot 10^{-n} \cdot \frac12\cdot
10^{-k}\]
The last inequality provides information about the error behavior in
the approximation of $y=f(x_2)$ by the linear function $y= y_1+L(\Delta x)=
y_1+m_{ski}(x_2-x_1)$. Since $x_2$ is arbitrary, the letter which plays it
role is not important. It can be replaced. In particular, $x_2$ in the
above exposition can be replaced by a number $x$.
Theorem: [Consequences of a Non-Zero Slope]
If the slope $m=f'(x_1)=L$ of $f(x)$ at $x=x_1$ is nonzero, then there
exist a $\delta>0$ such that the sign of $f(x)-f(x_1)$ equals the sign
of $L\cdot(x-x_1)$ whenever $|x-x_1| \le \delta$.
Proof: In the previous discussion, choose $k$ such
$\frac1210^{-k} < |L|$ and let $\delta=\frac1210^{-n}$.
This theorem implies if $m=f'(x_1)\ne0$ then no interior maximum nor
minimum can occur at $x=x_1$. Finding all solutions $x=a$ of the equation
$f'(x)=0$ identifies locations $x=a$ at which interior maximums and
minimums might be found. The latter can also occur at points where the
slope or derivative $f'(x)$ is not defined. The points $x$ where
-
$f(x)$ is undefined, and
-
$f'(x)$ is zero or undefined
are called \em critical points. \rm On finite and infinite intervals,
the maximums and minimums of functions $f(x)$ are located
-
at critical points inside that interval, and/or
-
at included endpoints.
So finding the critical points locates some, if not all, of the
maximums and minimums. This an extremum, that is, a maximum and minimum
locating principle for functions.
Rules For Differentiation
A calculus course may ask for the computation of slope $m_{ski}=L$ by
evaluating the limit directly. The rules and properties of limits suggest
how, at least in the simpler cases. Then the course may introduce rules
for differentiation. These rules for differentiation are based on or
justified by the rules and properties of limits. Differentiation rules
say how to compute formulas for $f'(x_1)$ in a routine mechanical manner
from formulas for $f(x)$, at least when the formula for $f(x)$ is simple
enough. The proof, justification and further explanation of rules for
differentiation may be found in a calculus course or book.
Algebraic Evaluation of Limits
The repetitive nature of the examples in this section
is deliberate. It emphasizes the algebraic way of writing and
thinking.
-
[Play
Video] 4.5 minutes: Algebraic View of Limits. Example
involving sums and quotients.
-
[Play
Video] 2.5 minutes: Derivative of a Linear Expression
cx+d via Limits.
-
[Play
Video] 2.3 minutes: Derivative as a Limit of a Quotient.
First pass at finding the derivative or slope of f(x) = x2.
Algebraic View.
-
[Play
Video] 2.25 minutes: Second pass at finding the derivative or
slope of f(x) = x2 at two values of x. Numerical
Examples of Limit Evaluation to suggest a pattern.
-
[Play
Video] 3.75 minutes: Third pass at finding the derivative or
slope of f(x) = x2. Back to the algebraic view and a
conclusion.
Remark: Many students survive
high school math courses without mastering the algebraic way of writing
and thinking. But mastery of the latter is necessary for comprehension
of the algebraic computations and reasoning in calculus. I have known
students, who obtained excellent marks in high school mathematics, to
say that the algebraic way of writing and thinking was strange to them
before taking calculus. The assumption that students have mastered the
algebraic thought cannot yet be made in a calculus course. Thus
examples to help with this mastery may be needed.
Consider the function y = f(x) =
x2. We will compute the slope, that is the derivative of
this function at x = 2, x = 3, x = 5 and x =
a. Look for a pattern in the following arithmetic
computations.
Example 1. Let $x=2$. Then with $x_1=x=2$ and $x_2=x_1+\delta x =x
+\delta x$, we have \begin{eqnarray*} \Delta y &=&f(x_2) -f(x_1)
\\ &=&f(x+\Delta x) -f(x) \\ &=&f(2+\Delta x)- f(2) \\
&=&(2+\Delta x)^2 -2^2 \\ &=&(2^2+2(2)\Delta x+(\Delta
x)^2) -2^2 \\ &=&2(2)\Delta x+(\Delta x)^2 \end{eqnarray*} Of
course $2(2)=4$, but for the sake of pattern recognition and emphasis, we
keep the arithmetic expression $2(2)$ to the end of the calculation. Now
\begin{eqnarray*} \mbox{A}&=&\frac{2(2)\Delta x+(\Delta
x)^2)}{\Delta x} \\ &=&2(2)+(\Delta x) \end{eqnarray*} This
implies \[ \lim_{\Delta x \to 0}\mbox{A} =\lim_{\Delta x \to 0}
2(2)+(\Delta x)= 2(2) =4 \] Example 2. Let $x=3$. Then
\begin{eqnarray*} \Delta y &=&f(x+\Delta x) -f(x) \\
&=&f(3+\Delta x)- f(3) \\ &=&(3+\Delta x)^2 -3^2 \\
&=&(3^2+2(3)\Delta x+(\Delta x)^2) -3^2 \\ &=&2(3)\Delta
x+(\Delta x)^2 \end{eqnarray*} Therefore \begin{eqnarray*}
\mbox{A}&=&\frac{2(3)\Delta x+(\Delta x)^2)}{\Delta x} \\
&=&2(3)+(\Delta x) \end{eqnarray*} This implies \[ \lim_{\Delta x
\to 0}\mbox{A} =\lim_{\Delta x \to 0}2(3)+(\Delta x)= 2(3) =6 \]
Example 3. Let $x=5$. Then \begin{eqnarray*} \Delta y
&=&f(x+\Delta x) -f(x) \\ &=&f(5+\Delta x)- f(5) \\
&=&(5+\Delta x)^2 -5^2 \\ &=&(5^2+2(5)\Delta x+(\Delta
x)^2) -5^2 \\ &=&2(5)\Delta x+(\Delta x)^2 \end{eqnarray*}
Therefore we expect \begin{eqnarray*} \mbox{A}&=&\frac{2(5)\Delta
x+(\Delta x)^2)}{\Delta x} \\ &=&2(5)+(\Delta x) \end{eqnarray*}
The last equality suggests that \[ \lim_{\Delta x \to 0}\mbox{A}
=\lim_{\Delta x \to 0}2(5)+(\Delta x) = 2(5) =10 \]
[Play
Video] 2.25 minutes: Derivative as a Limit of a Quotient.
First pass at finding the derivative or slope of f(x) = x2.
Algebraic View.
[Play
Video] 2.25 minutes: Second pass at finding the derivative or
slope of f(x) = x2 at two values of x. Numerical
Examples of Limit Evaluation to suggest a
pattern.
[Play
Video] 3.75 minutes: Third pass at finding the derivative or slope
of f(x) = x2. Back to the algebraic view and a
conclusion.
The Common Algebraic Pattern
The three examples follow the same pattern. We will rewrite the above
calculations with the letter $a$ replacing the numbers $2$, $3$ and/or
$5$ above, to emphasize the pattern. In the rewrite below, note that the
role of $a$ below could be played or assumed by each of the numbers $2$,
$3$ or $5$ above, another number or another letter!
Example n. Let $x=a$. Then as before \begin{eqnarray*} \Delta y
&=&f(x+\Delta x) -f(x) \\ &=&f(a+\Delta x)- f(a) \\
&=&(a+\Delta x)^2 -a^2 \\ &=&(a^2+2a\Delta x+(\Delta
x)^2) -a^2 \\ &=&2a\Delta x+(\Delta x)^2 \end{eqnarray*}
Therefore \begin{eqnarray*} \mbox{A}&=&\frac{2a\Delta x+(\Delta
x)^2)}{\Delta x} \\ &=&2(a)+(\Delta x) \end{eqnarray*} This
implies \[ \lim_{\Delta x \to 0}\mbox{A}=\lim_{\Delta x \to
0}2(a)+(\Delta x) = 2a \] Note that in the limit calculation, the
variable $a$ is held constant while $\Delta x \to 0$.
Now we can replace $a$ in the above pattern by $x$. This yields \[
f'(x)=\lim_{\Delta x \to 0}\mbox{A} = \cdots = \lim_{\Delta x\to0}
2x+(\Delta x) =2x \] The $\cdots$ indicates reasoning similar or
identical to that has gone before.
Remark - technical. The ratio $\mbox{A}=\frac{f(x_1+\Delta
x)-f(x_1)}{\Delta x}$ is not defined at $\Delta x =0$ as division by zero
is not defined. But the algebraic manipulations above shows that
$\lim_{\Delta x \to 0} $A does exist - at least for the simple case
treated.
[Play
Video] 2.25 minutes: Derivative of x3
algebraically via Limits.
Recapitulation
In the absence of units, the slope of the ski could be the finite number
L with the following arithmetic property:
For each whole number $k > 0$, there exist an $n>0$ such that
\[\left|L-\frac{\Delta y}{\Delta x} \right| \le \frac12\cdot 10^{-k}\] IF
$|\Delta x| \le \frac12\cdot 10^{-n}$.
When the latter occurs, we may write\[L=f'(x_1)=L=
\lim_{\mbox{ $\Delta x \to 0$}}\mbox{A}= \lim_{ \Delta x \to
0}\frac{f(x_1+\Delta x)-f(x_1)}{\Delta x} \]
The above limit L, if such a finite limit exists, is taken as the
definition of the slope to curve at or above the point x =
x1. This mathematical definition or convention provides
the computational answer to the two questions:
-
what is the slope of a curve $y=f(x)$ at a point $(x_1,y_1)=
(x_1,f(x_1))$?
-
what is the slope of a curve $y=f(x)$ at the point on it
determined by x=x1$?
Both questions have the same answer. The limit based definition of the
slope to the curve $y=f(x)$ depends only on the arithmetic properties of
the expression \[ \frac{\Delta y}{\Delta x} =\frac{f(x_2)-f(x_1)}{x_2-x_1}
\] The mathematical definition of the derivative or slope for function
$f(x)$ at a point $x_1$ is given by taking the slope to be the finite
limiting value $L$ of the expression $\frac{\Delta y}{\Delta x}$ as
$\Delta x\to 0$ approaches zero --- provided such a limiting value exists.
When this limit exists, the slope or derivative to $y=f(x)$ at $x=x_1$ is
said to be defined. It involves no explicit physical ideas --- this limit
can be computed without drawing a diagram and without imagining a short ski
placed on a curve. The latter are just motivations, important ones, for the
very computational and more precise, mathematical definition.
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