Calculus I

Framework and Overview of Main Concepts


This document provides an overview of the framework of Calculus I.  You will work through the details in the text, in class notes, and in communication with the instructor.

If you have already had Calculus I, this document should provide a brief review of the main topics.

If you are just starting Calculus I, you should read over this document, though you will probably not understand much of it. 

If you are reviewing for a test, this document is a good place to start.


Topics


The Idea of the Derivative

We know that to find the average rate of change of a quantity over a time interval we can divide the change in the quantity by the duration of the time interval.

If y(t) is a linear function y(t) = m t + b of clock time, then dy / dt = lim {t -> 0} [ y(t + Dt) - y(t) ] / Dt is easily simplified to give us dy / dt = m. That is, the derivative of a linear function is constant, and is equal to the slope of the graph of that function.

If we interpret y(t) as the depth of water in a uniform cylinder as water flows from a hole at the bottom of the cylinder, then as we have observed through a modeling exercise y(t) is very closely modeled by a quadratic function of clock time.

The Idea of the Integral

We know that to find the change in a quantity over a time interval we can multiply the rate of change in the quantity by the duration of the time interval.

[ r(t1) + r(t2) ] / 2 * (t2 - t1)

Connection between Integral and Derivative

If a function y(t) represents some quantity vs. clock time, then its derivative dy / dt represents the time rate of change of that quantity.

We can find the change in y(t) between two given clock times either by evaluating y(t) at these clock times, or by integrating r(t) between these clock times.

We thus see that the definite integral of r(t) = dy / dt between t = a and t = b is simply equal to y(b) - y(a).

A more familiar way of stating this is to say that is the following:

The above statement is the First Fundamental Theorem of Calculus.

This Theorem tells us that to integrate a function f(t), which for now we can think of as a rate function, we need only find some function F(t) whose derivative is equal to f(t)

For a linear rate of depth change function r(t) = m t + b, a corresponding quantity function is the quadratic function y(t) = 1/2 m t^2 + b t (it is easy to verify that the derivative of y(t) is r(t), so y(t) is an antiderivative of r(t)).

More generally, we can say that if F(t) is an antiderivative of a function f(t), then so is F(t) + c, where c is any constant number. We can furthermore say that the set of all such functions F(t) + c, where c can be any constant number, includes all possible antiderivatives of f(t).

The graphs of a function f(t) and an antiderivative function F(t) are related.

Trapezoidal Approximation Graphs

We can construct an approximation to the graph of a given function by partitioning its domain into trapezoids and labelling information relevant to the interpretation of the graph.

If the function represents a quantity Q(t) which depends on clock time t, then

If the function represents the rate dQ / dt at which some quantity Q changes with respect to clock time, then

Tangent-Line Approximation

If we know the value of a function y(t) at t = t0 and also the value y ' (t) of its derivative at t = t0, then we can estimate y(t) at any t value which is close to t0.

This is easily understood from a graph of y(t) vs. t in the vicinity of t = t0.

Riemann Sums

For a function f(x) which is continuous and increasing on an interval a <= f(t) <= b we form a partition a = t(0) < t(1) < t(2) < . . . < t(n) = b with t(i+1) - t(i) = `dt and approximate the integral int( f(t), t, a, b) by a lower sum and an upper sum. 

The actual integral lies between the lower sum and the upper sum, and as `dt -> 0 the difference between these sums approaches zero. 

The integral is therefore equal to the limiting value of either the lower or the upper sum, and must be equal to F(b) - F(a) for any function F(t) which is an antiderivative of f(t).

Derivatives of Basic Functions

The derivatives of the basic functions are as follows:

The Chain Rule

The derivative of f(g(x)) is the product of the rate at which g(x) changes at x, and the rate at which f(z) changes at z = g(x).

If a function f(z) depends on the value of z(w), which in turn depends on the value of w(v), which in turn depends on v(x), then a change in x causes a change in v which causes a change in w which causes a change in z which causes a change in f.

Derivative of Inverse Functions

If g(x) = f^-1(x), then f(g(x)) = x and f ' (g(x)) = 1.  However, we also have f ' (g(x)) = g ' (x) * f ' (g(x)), so that

Provided we can obtain an expression for f ' (g(x) ) we can thus find the formula for the derivative g ' (x) of the inverse function g(x) = f^-1(x).

Using this technique we find that

Implicit Differentiation

If y is a function of x and g is a function of y, then dg / dx is the derivative with respect to x of the composite function g ( y(x) ). 

This derivative, by the Chain rule, is dg / dx = y ' (x) * g ' ( y (x) ).

A product function of the form f(x) * g(y) can be differentiated with respect to x (recalling that dg / dx = dg / dy * dy / dx, or dg / dx = dg / dy * y ' ) using the product rule

An equation f(x, y) = 0 will often be satisfied by an infinite number of order pairs or points (x, y).

Given an equation of the form f(x, y) = 0, where f(x, y) denotes any expression involving x and y, we can differentiate the equation with respect to x.  The resulting equation will involve the variables x and y and the derivative y ' = dy / dx.   The equation can often be solved for y ' in terms of x and y, especially when y ' appears only as a linear factor of one or more terms of the equation.

L'Hopital's Rule

Often we need to evaluate the limiting value of an expression of the form f(x) / g(x) where both f(x) and g(x) have limiting values 0.

Thus

This is known as l'Hopital's Rule.

This rule is easily adapted to the case where f(x) and g(x) both have infinite limits at x = a (instead of f(x) / g(x) we use [ 1 / f(x) ] / [ 1 / g(x) ], where the numerator and denominator both have limit 0.  It is also easy to adapt to the case where the limits of the two functions are both zero as x -> infinity.

Optimization

A function f(x) which is continuous and twice-differentiable near x = a will have a maximum at x = a under the following conditions:

or

A function f(x) which is continuous and twice-differentiable near x = a will have a minimum at x = a under the following conditions:

or