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LQWHJUDO&$/& V�&DOFXOXV�,�6XUYLYDO�*XLGH E\�.UL VWD�.L QJ�RI� LQWHJU DO&$/ &�FRP �����LQWHJUDO&$/&� $OO�5LJKWV�5HVHUYHG� Disclaimer This e-book is presented solely for educational purposes. While best efforts have been used in preparing this e-book, the author makes no representations or warranties of any kind and assumes no liabilities of any kind with respect to the accuracy or completeness of the contents. The author shall not be held liable or responsible to any person or entity with respect to any loss or incidental or consequential damages caused, or alleged to have been caused, directly or indirectly, by the information contained herein. Every student and every course is different and the advice and strategies contained herein may not be suitable for your situation. This e-book is intended for supplemental use only. You should always seek help FIRST from your professor and other course material regarding any questions you may have. Introduction Author’s Note As a third grader, I learned my multiplication tables faster than anyone in my class. I was allowed to skip all of seventh-grade math and go straight to eighth-grade (something I think most people would pay a lot of money for, considering how much math sucks for pretty much everyone). As a junior, I finished all the math courses my high school was offereing. It wouldn’t be conceited to say that math was a subject that came easier to me than it did to others. Compared to my classmates, I was always good at it. What can I say? I got my butt kicked by every science class I ever took, but I was always ahead of the curve when it came to math. I guess it’s just the way my brain works. And yet, despite the fact that it’s always been easier for me, I’ve struggled with all kinds of math concepts soooooo many times, and often remember feeling totally and completely lost in math classes. You know that feeling when you’re reading through an example in your textbook, hoping with desperation that it will show you how to do the problem you’re stuck on? You hang in there for the first few steps, and you’re like, “Okay awesome! I’m getting this!” And then by about the fourth step, you start to lose track of their logic and you can’t for the life of you figure out how they got from Step 3 to Step 4? It’s the worst feeling. This is the point where most people give up completely and just resign themselves to failing the final exam. I’ve seen this same reaction in many of the students I tutored in calculus while I was in college. As hard as they tried to understand, the professor and the textbook just didn’t make sense, and they’d end up feeling overwhelmed and defeated before they’d ever really gotten started. I wasn’t a math major in college, but I spent a lot of time tutoring calculus students, and I’ve come to the conclusion that for most people, the way we teach math is fundamentally wrong. First, there’s a pretty good chance that you won’t ever actually use what you learn in calculus. Algebra? Definitely. Basic geometry? Probably. But calculus? Not so much. Second, even if it is worthwhile to learn this stuff, trying to teach us how to work through problems with proofs that are supposed to illustrate how the original formulas are derived, just seems ridiculous. In my experience, most students get the most benefit out of understanding the basic steps involved in completing the problem, and leaving it at that. Get in, get out, escape with your life, and hopefully your G.P.A. still intact. Sure, there’s a lot to be said for going more in depth with the material, and I’d love to help you do that if that’s your goal. For most people though, a basic understanding is sufficient. My greatest hope for this e-book and for integralCALC.com is that they’ll help you in whatever capacity you need them. If you’re shooting for a C+, let’s get you a C+. I don’t want to waste your time trying to give you more than you need. That being said though, most of the students I tutored who came in shooting for a C+ came out with something closer to a B+ or an A-. If you want an A, attaining it is easier than you think. No matter what your skill level, or the final grade you’re shooting for, I hope that this e- book will help you get closer to it, and better yet, save you some stress along the way. Remember, if there’s anything I can ever do for you, please contact me at integralCALC.com. Words of Wisdom There are two pieces of advice I’d like to give you before we get started. 1. Stay Positive More than anything, you have to stay positive. Don’t defeat yourself before you even get started. You’re smarter than you think, and calculus is easier than you think it is. Don’t panic. Half of the people I’ve tutored over the years needed a personal calculus cheerleader more than they needed a tutor. They’d gingerly proceed through a new problem… “Is this right? Then if I… am I still doing it right?” They’d doubt themselves at every step. And I would just stand behind them and say “Yeah, it’s right, you’re doing great, you’ve got it, you’re right,” until they’d solved the problem without my help at all. So many students let themselves get worked up and freaked out the moment something starts to get difficult. It’s understandable, but the more you can fight the fear that starts to creep in, the better off you’ll be. So take a deep breath. It’s going to be okay. 2. Use Your Calculator (Or Don’t) Your calculator can be your greatest ally, but it can also be your worst enemy. As calculators have gotten more powerful, students have come to rely on them more and more to solve their problems on both homework and exams. Instead of relying on my calculator to solve problems outright, I like to use it as a double- check system. If you never learn how to do the problem without your calculator, you won’t know if what your calculator tells you is correct. Nor will you be able to show any work if you’re required to do so on an exam, which could cost you big points. Learning the calculus itself means you’ll be able to show your work when you need to, and you’ll actually understand what you’re doing. Once you solve a problem, you should know how to punch in the equation so that you can look at the graph or solution to verify that the answer you got is the same one your calculator gives back to you. What You Won’t Find I’m not here to replace your textbook. Because this is a quick-reference guide, you won’t find chapter introductions full of calculus history you don’t care about. I’m also not here to replace your professor, nor do I expect that you’re particularly excited about learning calculus. If you are excited about calculus, that’s awesome! So am I. But if you’re not, this is the place to be, because, at least in this e-book, you won’t find pointless tangents where I geek out hard core and get really excited about proofs, and you just get bored and confused. The purpose of this e-book is to serve as a supplement to the rest of your course material, not to completely replace your professor or your textbook. Even though I’ve tried to cover the most common introductory calculus topics in enough detail that you could get by with just this e-book, neither of us can predict whether your professor will ask you to solve a problem with a different method on a test, or a specific problem not covered here. The last thing I want is for you to think that this e-book is a replacement for going to class, miss that information, and then do poorly on the test because you didn’t get all the instructions. What You Will Find This e-book should give you the most crucial pieces of information you’ll need for a real understanding of how to solve most of the problems you’ll encounter. I don’t want to be your textbook, which is why this e-book is only about thirty pages long. I want this to be your quick reference, the thing you reach for when you need a clear understanding in only a few minutes. For a specific list of topics covered in this e- book, please refer to the Table of Contents. (Clickable) Table of Contents I. Foundations of Calculus A. Functions 1. Vertical Line Test 2. Horizontal Line Test 3. Domain and Range 4. Independent/Dependent Variables 5. Linear Functions a. Slope-Intercept Form b. Point-Slope Form 6. Quadratic Functions a. The Quadratic Formula b. Completing the Square 7. Rational Functions a. Long Division B. Limits 1. What is a Limit? 2. When Does a Limit Exist? a. General vs. One-Sided Limits b. Where Limits Don’t Exist 3. Solving Limits Mathematically a. Just Plug It In b. Factor It c. Conjugate Method 4. Trigonometric Limits 5. Infinite Limits C. Continuity 1. Common Discontinuities a. Jump Discontinuity b. Point Discontinuity c. Infinite/Essential Discontinuity 2. Removable Discontinuity 3. The Intermediate Value Theorem II. The Derivative A. The Difference Quotient 1. Secant and Tangent Lines 2. Creating the Derivative 3. Using the Difference Quotient B. When Derivatives Don’t Exist 1. Discontinuities 2. Sharp Points 3. Vertical Tangent Lines C. On to the Shortcuts! 1. The Derivative of a Constant 2. The Power Rule 3. The Product Rule 4. The Quotient Rule 5. The Reciprocal Rule 6. The Chain Rule D. Common Operations 1. Equation of the Tangent Line 2. Implicit Differentiation a. Equation of the Tangent Line b. Related Rates E. Common Applications 1. Speed/Velocity/Acceleration 2. L’Hopital’s Rule 3. Mean Value Theorem 4. Rolle’s Theorem III. Graph Sketching A. Critical Points B. Increasing/Decreasing C. Inflection Points D. Concavity E. - and -Intercepts F. Local and Global Extrema 1. First Derivative Test 2. Second Derivative Test G. Asymptotes 1. Vertical Asymptotes 2. Horizontal Asymptotes 3. Slant Asymptotes H. Putting It All Together IV. Optimization V. Essential Formulas Foundations of Calculus Functions Vertical Line Test Most of the equations you’ll encounter in calculus are functions. Since not all equations are functions, it’s important to understand that only functions can pass the Vertical Line Test. In other words, in order for a graph to be a function, no completely vertical line can cross its graph more than once. This graph does not pass the Vertical Line Test because a vertical line would intersect it more than once. Passing the Vertical Line Test also implies that the graph has only one output value for for any input value of . You know that an equation is not a function if can be two different values at a single value. You know that the circle below is not a function because any vertical line you draw between and will cross the graph twice, which causes the graph to fail the Vertical Line Test. You can also test this algebraically by plugging in a point between and for , such as . At , can be both and . Since a function can only have one unique output value for for any input value of , the graph fails the Vertical Line Test and is therefore not a function. We’ve now proven with both the graph and with algebra that this circle is not a function. Horizontal Line Test The Horizontal Line Test is used much less frequently than the vertical line test, despite the fact that they’re very similar. You’ll recall that any function passing the Vertical Line Test can only have one unique output of for any single input of . This graph passes the Horizontal Line Test because a horizontal line cannot intersect it more than once. Contrast that with the Horizontal Line Test, which says that no value corresponds to two different values. If a function passes the Example Determine algebraically whether or not is a function. Plug in for and simplify. Horizontal Line Test, then no horizontal line will cross the graph more than once, and the graph is said to be “one-to-one.” This graph does not pass the Horizontal Line Test because any horizontal line between and would intersect it more than once. Domain and Range Think of the domain of a function as everything you can plug in for without causing your function to be undefined. Things to look out for are values that would cause a fraction’s denominator to equal and values that would force a negative number under a square root sign. The range of a function is then any value that could result for from plugging in every number in the domain for . Independent and Dependent Variables Your independent variable is , and your dependent variable is . You always plug in a value for first, and your function returns to you a value for based on the value you gave it for . Remember, if your equation is a function, there is only one possible output of for any input of . Linear Functions You’ll need to know the formula for the equation of a line like the back of your hand (actually, better than the back of your hand, because who really knows what the back of their hand looks like anyway?). You have two options about how to write the equation of a line. Both of them require that you know at least two of the following pieces of information about the line: 1. A point 2. Another point 3. The slope, 4. The y-intercept, If you know any two of these things, you can plug them into either formula to find the equation of the line. Slope-Intercept Form The equation of a line can be written in slope- intercept form as , where is the slope of the function and is the -intercept, or the point at which the graph crosses the -axis and where . The slope, represented by , is calculated using two points on the line, and , and the equation you use to calculate is To find the slope, subtract the -coordinate in the first point from the -coordinate in the second point in the numerator, then subtract the -coordinate in the first point from the - coordinate in the second point in the denominator. Example Describe the domain and range of the function In this function, cannot be equal to , because that value causes the denominator of the fraction to equal . Because setting equal to is the only way to make the function undefined, the domain of the function is all . Point-Slope Form The equation of a line can also be written in point-slope form as In this form, is one point on the line, and is the other. Just as with slope- intercept form, is still the slope of the function. To use this form, find the same way you did in slope-intercept form, then simply plug in your two points to the point- slope formula. Quadratic Functions Quadratic Functions are functions of the specific form As long as you have an term and an term and a constant, the coefficients , and can be any number. The Quadratic Formula The Quadratic Formula can be used to factor and solve for the roots of a quadratic function. To use it, plug , and into the Quadratic Formula, here: If any terms in your quadratic function are negative, make sure to keep the negative sign when plugging into the formula. For example, If is negative in your quadratic function, you’ll end up with – for the first term in the numerator of the Quadratic Formula, which would make that term positive. You should also remember that in order for this formula to work, must be greater than or equal to , because you can’t take the square root of a negative number. If you do end up with a negative number inside the radical, then there are no real solutions to your quadratic function. Example Find the equation of the line in point- slope form that passes through the points and . We start by finding the slope. Now plug in the slope and either one of the points into the formula. Even though we could, simplifying any further would take this out of point slope form, so we leave it as is. Example Find the equation of the line in slope- intercept form that passes through the points and . We start by finding the slope. Now we can plug in our slope and either one of our points to the formula and solve for . Multiply every term by to cancel out the denominator of the fraction. Subtract from both sides. Divide by to solve for . For the final answer, plug and back into the formula, leaving and as variables. Since you always get a fraction with a plus or minus sign in the numerator, the Quadratic Formula produces two solutions, which you then use to factor your polynomial. If your solutions are and , your factors will always be and . Completing the Square This method is another option you can use to find the solutions of a quadratic function, if you can’t easily factor it. Since it’s very much a step-by-step process, the easiest way to explain this method is to use an example, so let’s do it. Let’s say we have the function The first thing we want to do is set the function equal to . Next, we’ll take one half of the coefficient on the term and square it. We then add and subtract our result back into the function, so that we don’t change the value of the function. Now we factor the quantity in parentheses and consolidate the constants. Now add to both sides to move the constant to the right side. Take the square root of both sides to eliminate the exponent on the left. Don’t forget to add the positive/negative sign in front of the square root on the right side. Finally, add to both sides of the equation to solve it for . This is the same process you’ll follow each time you use this method to solve for the roots of a quadratic function. Rational Functions A rational function is a quotient of two polynomials (a fraction with polynomials in both the numerator and denominator). While polynomials themselves are defined for all values of , rational functions are undefined where the denominator of the function is equal to . Long Division Believe it or not, long division is a skill you’ll use semi-frequently in calculus. It’s just like the long division you learned in fifth grade, except that instead of just numbers, this time you’ll be dividing polynomials. Example Use long division to convert First, we should keep the following in mind: Example Factor Plug for , for and for into the Quadratic Formula. Simplify to find your solutions. Use the solutions to factor your function. Limits What is a Limit? The limit of a function is the value the function approaches at a given value of , regardless of whether the function actually reaches that value. For an easy example, consider the function When , . Therefore, is the limit of the function at , because is the value that the function approaches as the value of gets closer and closer to . I know it’s strange to talk about the value that a function “approaches.” Think about it this way: If you set in the function above, then . Similarly, if you set , then . You can begin to see that as you get closer to , whether you’re approaching it from the side or the side, the value of gets closer and closer to . .0000 .0000 In this simple example, the limit of the function is clearly because that is the actual value of the function at that point; the point is defined. However, finding limits gets a little trickier when we start dealing with points of the graph that are undefined. In the next section, we’ll talk about when limits do and do not exist, and some more creative methods for finding the limit. When Does a Limit Exist? General vs. One-Sided Limits When you hear your professor talking about limits, he or she is usually talking about the general limit. Unless a right- or left-hand limit is specifically specified, you’re dealing with a general limit. The general limit exists at the point if 1. The left-hand limit exists at , 2. The right-hand limit exists at , and 3. The left- and right-hand limits are equal. These are the three conditions that must be met in order for the general limit to exist. The general limit will look something like this: You would read this general limit formula as “The limit of of as approaches equals .” Left- and right-hand limits may exist even when the general limit does not. If the graph approaches two separate values at the point as you approach from the left- and right-hand side of the graph, then separate left- and right-hand limits may exist. Left-hand limits are written as Divisor Numerator Dividend Denominator ________ | -( ) -( To start our long division problem, we determine what we have to multiply by (in the divisor) to get (in the dividend). Since the answer is , we put that on top of our long division problem, and multiply it by the divisor, to get , which we then subtract from the dividend. We bring down from the dividend and repeat the same steps until we have nothing left to carry down from the dividend. Our original problem reduces to: The negative sign after the indicates that we’re talking about the limit as we approach from the negative, or left-hand side of the graph. Right-hand limits are written as The positive sign after the 2 indicates that we’re talking about the limit as we approach 2 from the positive, or right-hand side of the graph. In the graph below, the general limit exists at because the left- and right- hand limits both approach . On the other hand, the general limit does not exist at because the left-hand and right-hand limits are not equal, due to a break in the graph. Left- and right-hand limits are equal at , but not at . Where Limits Don’t Exist We already know that a general limit does not exist where the left- and right-hand limits are not equal. Limits also do not exist whenever we encounter a vertical asymptote. There is no limit at a vertical asymptote because the graph of a function must approach one fixed numerical value at the point for the limit to exist at . The graph at a vertical asymptote is increasing and/or decreasing without bound, which means that it is approaching infinity instead of a fixed numerical value. In the graph below, separate right- and left- hand limits exist at but the general limit does not exist at that point. The left-hand limit is , because that is the value that the graph approaches as you trace the graph from left to right. On the other hand, the right-hand limit is , since that is the value that the graph approaches as you trace the graph from right to left. The general limit does not exist at or at . Where there is a vertical asymptote at , the left-hand limit is , and the right-hand limit is . However, the general limit does not exist at the vertical asymptote because the left- and right-hand limits are unequal. Solving Limits Mathematically Just Plug It In Sometimes you can find the limit just by plugging in the number that your function is approaching. You could have done this with our original limit example, . If you just plug into this function, you get , which is the limit of the function. Below is another example, where you can simply plug in to the function to solve for the limit. Factor It When you can’t just plug in the value you’re evaluating, your next approach should be factoring. Example Plug in for and simplify. Conjugate Method This method can only be used when either the numerator or denominator contains exactly two terms. Needless to say, its usefulness is limited. Here’s an example of a great, and common candidate for the Conjugate Method. In this example, the substitution method would result in a in the denominator. We also can’t factor and cancel anything out of the fraction. Luckily, we have the Conjugate Method. Notice that the numerator has exactly two terms, and . Conjugate Method to the rescue! In order to use it, we have to multiply by the conjugate of whichever part of the fraction contains the two terms. In this case, that’s the numerator. The conjugate of two terms is those same two terms with the opposite sign in between them. Notice that we multiply both the numerator and denominator by the conjugate, because that’s like multiplying by , which is useful to us but still doesn’t change the value of the original function. Remember, if none of these methods work, you can always go back to the method we were using originally, which is to plug in a number very close to the value you’re evaluating and solve for the limit that way. Trigonometric Limits Trigonometric limit problems revolve around three formulas: Simplify and cancel the . Since we’re evaluating at , plug that in for and solve. Example Multiply the numerator and denominator by the conjugate. Example Just plugging in would give us a nasty result. Therefore, we’ll try factoring instead. Cancelling from the top and bottom of the fraction leaves us with something that is much easier to evaluate: Now the problem is simple enough that we can just plug in the value we’re approaching. When solving trigonometric limit problems, our goal is to reduce our problem to a simple combination involving nothing but these formulas and simple constants. Here’s an example. Infinite Limits Infinite limits exist when we can plug in a number for that causes the denominator of a rational function in lowest terms to equal . Here is an example of a rational function in lowest terms, which means that we cannot factor and cancel anything in the fraction. We can see that setting gives in the denominator, which means that we have a vertical asymptote at , and therefore an infinite limit at that point. Now that we’ve established that this is a rational function in lowest terms and that a vertical asymptote exists, all that’s left to determine is whether the limit at approaches positive or negative infinity. In order to do that, simply plug in a number very close to 1. If our result is positive, the limit will be . If the result is negative, the limit is . We can see that the result will be very large and positive, so we know that the limit of this function at is . Continuity I would give you the definition of continuity, but I think it’s confusing. Plus, you should have some intuition about what it means for a graph to be continuous. Basically, a function is continuous if there are no holes, breaks, jumps, fractures, broken bones, etc. in its graph. You can also think about it this way: A function is continuous if you can draw the entire thing without picking up your pencil. Let’s take some time to classify the most common types of discontinuity, or what makes a function not continuous. As it turns out, we can now easily evaluate our entire problem with the three fundamental trigonometric limit formulas, without making the denominator . Example Since we have exactly two terms in the numerator, we’re actually going to borrow the Conjugate Method for the first step of this problem. Applying the identity to the numerator gives Notice now that we can factor out , which is one of our three fundamental formulas. Common Discontinuities Jump Discontinuity You’ll usually encounter jump discontinuities with piecewise-defined functions. “A piece- wahoozle whatsit?” you ask? Exactly. A piecewise-defined function is a function for which different parts of the domain are defined by different functions. One example that’s often used to illustrate piecewise- defined functions is the cost of postage at the post office. Here’s how the cost of postage might be defined as a function, as well as the graph of this function. They tell us that the cost per ounce of any package lighter than pound is cents per ounce, that the cost of every ounce from pound to anything less than pounds is cents per ounce, etc. A piecewise-defined function Every break in this graph is a point of jump discontinuity. You can remember this by imagining yourself walking along on top of the first segment of the graph. In order to continue, you’d have to jump up to the second segment. Point Discontinuity Point discontinuity exists when there is a hole in the graph at one point. You usually find this kind of discontinuity when your graph is a fraction like this: In this case, the point discontinuity exists at , where the denominator would equal . This function is defined and continuous everywhere, except at . The graph of a point discontinuity is easy to pick out because it looks totally normal everywhere, except for a hole at a single point. Infinite/Essential Discontinuity You’ll see this kind of discontinuity called both infinite discontinuity and essential discontinuity. In either case, it means that the function is discontinuous at a vertical asymptote. Vertical asymptotes are only points of discontinuity when the graph exists on both sides of the asymptote. The first graph below shows a vertical asymptote that makes the graph discontinuous, because the function exists on both sides of the vertical asymptote. The vertical asymptote in the second graph below is not a point of discontinuity, because it doesn’t break up any part of the graph. A vertical asymptote at that makes the graph discontinuous A vertical asymptote at that does not make the graph discontinuous Removable Discontinuity Discontinuity is removable if you can easily plug in the holes in its graph by redefining the function. When you can’t easily plug in the holes because the gaps are bigger than a single point, you’re dealing with nonremovable discontinuity. Point discontinuity is removable, because you can easily patch the hole. Let’s take the function from the Point Discontinuity section: If we add another piece to this function as follows, we “plug” the hole and the function becomes continuous: Jump and infinite discontinuities are always nonremovable, because the gaps are large. The Intermediate Value Theorem Similarly to the definition of continuity, the definition of the Intermediate Value Theorem is absolutely more harmful than helpful. So instead, consider the following graph: The Intermediate Value Theorem This theorem is fairly ridiculous because it doesn’t tell us anything that we don’t already know. All it says is that, when we look at a continuous function on a closed interval between (blue) and (purple), there will be a point in between them, which we’ll call (orange). must be between and and must be between and . Looking at the graph, isn’t that obvious? Values may or may not exist below and above depending on the graph, but must exist. The Derivative The derivative of a function is written as , and read as “ prime of .” By definition, the derivative is the slope of the original function. Let’s find out why. The Difference Quotient I should warn you that this is one of those dumb things you have to learn to do before you learn how to do it the real way. If you can believe this, your professor will actually have the nerve to require you on a test to find the derivative using this method, even though you could just use the shortcuts that we’re going to learn later. Unbelievable, I know. But since our goal is just to get you a good grade, and not to make a big scene, we’ll learn how to find derivatives the long way first, then we’ll learn the shortcuts and things will end up better in the end. I promise. For now, the long way… Secant and Tangent Lines A tangent line is a line that juuussst barely touches the edge of the graph, intersecting it at only one specific point. Tangent lines look very graceful and tidy, like this: A tangent line A secant line, on the other hand, is a line that runs right through the middle of a graph, sometimes hitting it at multiple points, and looks generally meaner, like this: A secant line It’s important to realize here that the slope of the secant line is the average rate of change over the interval between the points where the secant line intersects the graph. The slope of the tangent line instead indicates an instantaneous rate of change, or slope, at the single point where it intersects the graph. Creating the Derivative If we start with a point, on a graph, and move a certain distance, , to the right of that point, we can call the new point on the graph . Connecting those points together gives us a secant line, and we can use the slope equation to determine that the slope of the secant line is which, when we simplify, gives us I bet your heart just skipped a beat out of pure excitement. No? Strange… The point of all this nonsense is that, if I take my second point and start moving it slowly left, closer to the original point, the slope of the secant line becomes closer to the slope of the tangent line at the original point. As the secant line moves closer and closer to the tangent line, the points where the line intersects the graph get closer together, which eventually reduces to . Running through this exercise allows us to realize that if I reduce to and the distance between the two secant points becomes nothing, that the slope of the secant line is now exactly the same as the slope of the tangent line. In fact, we’ve just changed the secant line into the tangent line entirely. That is how we create the formula above, which is the very definition of the derivative, which is why the definition of the derivative is the slope of the function at a single point. Using the Difference Quotient To find the derivative of a function using the difference quotient, follow these steps: 1. Plug in for every in your original function. 2. Plug your answer from Step in for in the difference quotient. 3. Plug your original function in for in the difference quotient. 4. Put in the denominator. 5. Expand all terms and collect like terms. 6. Factor out in the numerator, then cancel it from the numerator and denominator. 7. Plug in the number your function is approaching and simplify. Example Find the derivative of at When Derivatives Don’t Exist Before we jump into finding derivatives with the shortcuts, let’s talk about instances when the derivative doesn’t exist. When the derivative doesn’t exist at a point in the graph, we say that the original function is not differentiable there. Discontinuities A derivative cannot exist at a point of discontinuity in a function. This does not mean that the function is not differentiable at other points in its domain, only that the function is not differentiable at the specific point of discontinuity. Sharp Points If a graph contains a sharp point (A.K.A. a cusp), the function is not differentiable at that point. You’re most likely to find sharp points in your function if it contains absolute values or if it’s a piecewise-defined function. A cusp in the graph of Vertical Tangent Lines Since the slope of a vertical line is undefined, and a tangent line represents the slope of the graph, a tangent line by definition cannot be vertical, so the derivative cannot be a perfectly vertical line. On to the Shortcuts! Finally, we’ve gotten to the point where things start to get easier. We’ve moved past the Difference Quotient, which was cumbersome and tedious and generally not fun. You’re about to learn several new derivative tricks that will make this whole process a whole lot easier. Aren’t you excited?! The Derivative of a Constant The derivative of a constant (a term with no variable attached to it) is always . Remember that the graph of any constant is a perfectly horizontal line. Remember also that the slope of any horizontal line is . Because the derivative of a function is the slope of that function, and the slope of a horizontal line is , the derivative of any constant must be . The Power Rule The Power Rule is the tool you’ll use most frequently when finding derivatives. The rule says that for any term of the form , the derivative of the term is To use the Power Rule, multiply the variable’s exponent, , by its coefficient, , then subtract from the exponent. If there is no coefficient (the coefficient is ), then the exponent will become the new coefficient. After replacing with in , plug it your answer for . Then plug in as-is for . Put in the denominator. Expand all terms. Collect similar terms together then factor out of the numerator and cancel it from the fraction. For , plug in the number you’re approaching, in this case . Then simplify and solve. The Product Rule If a function contains two variable expressions that are multiplied together, you cannot simply take their derivatives separately and then multiply the derivatives together. You have to use the Product Rule. Here is the formula: If a function then To use the Product Rule, multiply the first function by the derivative of the second function, then add the derivative of the first function times the second function to your result. The Quotient Rule Just as you must always use the Product Rule when two variable expressions are multiplied, you must use the Quotient Rule whenever two variable expressions are divided. Here is the formula: If a function then The Reciprocal Rule The Reciprocal Rule is very similar to the Quotient Rule, except that it can only be used with quotients in which the numerator is exactly . It says that if Example Find the derivative of Based on the Quotient Rule formula, we know that is the numerator and therefore and that is the denominator and therefore that . is , and is . Plugging all of these components into the Quotient Rule gives Simplifying the result gives us our final answer: Example Find the derivative of The two functions in this problem are and . It doesn’t matter which one you choose for and . Let’s assign to and to . The derivative of is . The derivative of is . According to the Product Rule, Simplifying the result gives us our final answer: Example Find the derivative of Applying Power Rule gives the following: Simplify to solve for the derivative. then Given as your numerator and anything at all as your denominator, the derivative will be the negative derivative of the denominator divided by the square of the denominator. The Chain Rule The Chain Rule is often one of the hardest concepts for calculus students to understand. It’s also one of the most important, and it’s used all the time, so make sure you don’t leave this section without a solid understanding. If you go through the example and you’re still having trouble, please e-mail me for help at integralCALC@gmail.com. You should use Chain Rule anytime your function contains something more complicated than a single variable. The Chain Rule says that if your function takes the form then The Chain Rule tells us how to take the derivative of something where one function is “inside” another one. It seems complicated, but applying the Chain Rule requires just two simple steps: 1. Take the derivative of the “outside” function, leaving the “inside” function completely alone. 2. Multiply what you got in Step by the derivative of the “inside” function. Common Operations Equation of the Tangent Line You’ll see it written different ways, but the most understandable tangent line formula I’ve found is function, , untouched. Taking the derivative of using the Power Rule gives Plugging back in for gives us Step of Chain Rule tells us to take our result from Step and multiply it by the derivative of the “inside” function. Our “inside” function is , and its derivative is Multiplying the result from Step by the derivative of our inside function, , gives: Simplifying the result gives us our final answer: Example Find the derivative of In this example, the “outside” function is . is representing , but we leave that part alone for now because Step of Chain Rule tells us to take the derivative of the outside function while leaving the inside Example Find the derivative of Applying the Reciprocal Rule gives When a problem asks you to find the equation of the tangent line, you’ll always be asked to evaluate at the point where the tangent line intersects the graph. In order to find the equation of the tangent line, you’ll need to plug that point into the original function, then substitute your answer for . Next you’ll take the derivative of the function, plug the same point into the derivative and substitute your answer for . Implicit Differentiation Implicit Differentiation allows you to take the derivative of a function that contains both and on the same side of the equation. If you can’t solve the function for , implicit differentiation is the only way to take the derivative. On the left sides of these derivatives, instead of seeing or , you’ll find instead. In this notation, the numerator tells you what function you’re deriving, and the denominator tells you what variable is being derived. is literally read “the derivative of with respect to .” One of the most important things to remember, and the thing that usually confuses students the most, is that we have to treat as a function and not just as a variable like . Therefore, we always multiply by when we take the derivative of y. To use implicit differentiation, follow these steps: 1. Differentiate both sides with respect to . 2. Whenever you encounter , treat it as a variable just like , and multiply that term by . 3. Move all terms involving to the left side and everything else to the right. 4. Factor out on the left and divide both sides by the other left-side factor so that is the only thing remaining on the left. Example Find the derivative of Our first step is to differentiate both sides with respect to . Treat as a variable just like , but whenever you take the derivative of a term that includes , multiply by . You’ll need to use the Product Rule for the right side, treating as one function and as another. Finally, insert both and into the tangent line formula, along with for , since this is the point at which we were asked to evaluate. You can either leave the equation in this form, or simplify it further, as follows: Example Find the equation of the tangent line at to the graph of First, plug in to the original function. Next, take the derivative and plug in . Equation of the Tangent Line You may be asked to find the tangent line equation of an implicitly-defined function. Just for fun, let’s pretend you’re asked to find the equation of the tangent line of the function in the previous example at the point . You’d pick up right where you left off, and plug in this point to the derivative of the function. Related Rates Related Rates are an application of implicit differentiation, and are usually easy to spot. They ask you to find how quickly one variable is changing when you know how quickly another variable is changing. To solve a related rates problem, complete the following steps: 1. Construct an equation containing all the relevant variables. 2. Differentiate the entire equation with respect to (time), before plugging in any of the values you know. 3. Plug in all the values you know, leaving only the one you’re solving for. 4. Solve for your unknown variable. Example How fast is the radius of a balloon increasing when the radius is 100 centimeters, if air is being pumped into the spherical balloon at a rate of 400 cubic centimeters per second. In this example, we’re asked to find the rate of change of the radius, given the rate of change of the volume. The formula that relates the volume and radius of a sphere to one another is simply the formula for the volume of a sphere: Before doing anything else, we use implicit differentiation to differentiate both sides with respect to . Example (continued) Now that you’ve found the slope of the tangent line at the point , plug the point and the slope into Point-Slope Form: You could leave the equation as it is above, or simplify it as follows: Move all terms that include to the left side, and everything else to the right side. Factor out on the left, then divide both sides by . Dividing the right side by 3 to simplify gives us our final answer: Common Applications Speed/Velocity/Acceleration A common application of derivatives is the relationship between speed, velocity and acceleration. In these problems, you’re usually given a position equation in the form “ ” or “ ”, which tells you the object’s distance from some reference point. This equation also accounts for direction, so the distance could be negative, depending on which direction your object moved away from the reference point. Average speed of the object is Average velocity of the object is To find velocity, take the derivative of your original position equation. Speed is the absolute value of velocity. Velocity accounts for the direction of movement, so it can be negative. It’s like speed, but in a particular direction. Speed, on the other hand, can never be negative because it doesn’t account for direction, which is why speed is the absolute value of velocity. To find acceleration, take the derivative of velocity. Example Suppose a particle is moving along the -axis so that its position at time is given by the formula Compute its velocity and acceleration as functions of . Next, decide in which direction (left or right) the particle is moving when and whether its velocity and speed are increasing or decreasing. To find velocity, we take the derivative of the original position equation. To find acceleration, we take the derivative of the velocity function. To determine the direction of the particle at , we plug into the velocity function. Because is positive, we can Now we plug in everything that we know. Keep in mind that is the rate at which the volume is changing, is the rate at which the radius is changing, and is the length of the radius at a specific moment. Our problem tells us that the rate of change of the volume is 400, and that the length of the radius at the specific moment we’re interested in is 100. Solving for gives us Therefore, we know that the radius of the balloon is increasing at a rate of centimeters per second. L’Hopital’s Rule L’Hopital’s Rule is used to get you out of sticky situations with indeterminate limit forms, such as or . If you plug in the number you’re approaching to the function for which you’re trying to find the limit and your result is one of the indeterminate forms above, you should try applying L’Hopital’s Rule. To use it, take the derivatives of the numerator and denominator and replace the original numerator and denominator with their derivatives. Then plug in the number you’re approaching. If you still get an indeterminate form, continue using L’Hopital’s Rule until you can use substitution to get a prettier answer. is our final answer. However, if plugging in had resulted in another indeterminate form, we could have applied another round of L’Hopital’s Rule, and another and another, until we were able to plug in the number we’re approaching to get an answer that was not indeterminate. Mean Value Theorem This theorem guarantees that, at some point on a closed interval, the tangent line to the graph will be parallel to the line connecting the endpoints of that interval. The Mean Value Theorem is the following: Example Pretend that we drive from Florida to California in exactly hours, from time to time , and travel a distance of miles. If describes the distance we’ve traveled at time , then the Mean Value Theorem tells us that Example If we try plugging in for , we get the indeterminate form , so we know that this is a good candidate for L’Hopital’s Rule. The derivative of our numerator is . The derivative of our denominator is . To use L’Hopital’s Rule, we take those derivatives and plug them in for the original numerator and denominator. If we now try plugging in the number we’re approaching, we get a clear answer. conclude that the particle is moving in the positive direction (toward the right). To determine whether velocity is increasing or decreasing, we plug 1 into the acceleration function, because that will give us the rate of change of velocity, since acceleration is the derivative of velocity. Since acceleration is negative at , velocity must be decreasing at that point. Since the velocity is positive and decreasing at , that means that speed is also decreasing at that point. Rolle’s Theorem Rolle’s Theorem is a specific instance of the Mean Value Theorem. Like the Mean Value Theorem, Rolle’s Theorem applies to a function on a closed interval, . If and are both equal to , meaning that the interval starts and ends on the -axis, then the derivative, or slope of the function, at some point in the interval must be equal to . Rolle’s Theorem - At some point between and , the slope of the derivative must be equal to and the derivative must be parallel to the - axis. Graph Sketching Graph sketching is not very hard, but there are a lot of steps to remember. Like anything, the best way to master it is with a lot of practice. When it comes to sketching the graph, if possible I absolutely recommend graphing the function on your calculator before you get started so that you have a visual of what your graph should look like when it’s done. You certainly won’t get all the information you need from your calculator, so unfortunately you still have to learn the steps, but your calculator is still a good double-check system. Our strategy for sketching the graph will include the following steps: 1. Find critical points. 2. Determine where is increasing and decreasing. 3. Find inflection points. 4. Determine where is concave up and concave down. 5. Find - and -intercepts. 6. Plot critical points, possible inflection points and intercepts. 7. Determine behavior as approaches positive and negative infinity. 8. Draw the graph with the information we just gathered. Critical Points Critical points occur at -values where the function’s derivative is either equal to zero or undefined. Critical points are the only points at which a function can change direction, and also the only points on the graph that can be maxima or minima of the function. Example Find the critical points of Take the derivative and simplify. You can move the in the denominator of the fraction into the numerator by changing the sign on its exponent from to . The Mean Value Theorem therefore implies that there was an instantaneous velocity of exactly miles/hour at least once during the trip. Increasing/Decreasing A function that is increasing (moving up as you travel from left to right along the graph), has a positive slope, and therefore a positive derivative. An increasing function Similarly, a function that is decreasing (moving down as you travel from left to right along the graph), has a negative slope, and therefore a negative derivative. A decreasing function Based on this information, it makes sense that the sign (positive or negative) of a function’s derivative indicates the direction of the original function. If the derivative is positive at a point, the original function is increasing at that point. Not surprisingly, if the derivative is negative at a point, the original function is decreasing there. We already know that the direction of the graph can only change at the critical points that we found earlier. As we continue with our example, we’ll therefore plot those critical points on a wiggle graph to test where the function is increasing and decreasing. Example (continued) Determine where is increasing and decreasing First, we create our wiggle graph and plot our critical points, as follows: -----------------------|--------------------|----------------- Next, we pick values on each interval of the wiggle graph and plug them into the derivative. If we get a positive result, the graph is increasing. A negative result means it’s decreasing. The intervals that we will test are: , and . To test , we’ll plug into the derivative, since is a value in that range. Using Power Rule to take the derivative gives Moving the back into the denominator by changing the sign on its exponent gives Now set the derivative equal to and solve for . Inflection Points Inflection points are just like critical points, except that they indicate where the graph changes concavity, instead of indicating where the graph changes direction, which is the job of critical points. We’ll learn about concavity in the next section. For now, let’s find our inflection points. In order to find inflection points, we first take the second derivative, which is the derivative of the derivative. We then set the second derivative equal to zero and solve for . There is no solution to this equation, but we can see that the second derivative is undefined at . Therefore, is the only possible inflection point. Concavity Concavity is indicated by the sign of the function’s second derivative, . The function is concave up everywhere the second derivative is positive, and concave down everywhere the second derivative is negative. The following graph illustrates examples of concavity. From , the graph is concave down. Think about the fact that a graph that is concave down looks like a frown. Sad, I know. The inflection point at which the graph changes concavity is at . On the range , the graph is concave up. It looks like a smile. Ah… much better. is concave down on the range and concave up on the range . We can use the same wiggle graph technique, along with the possible inflection point we just found, to test for concavity. Example (continued) We’ll start with the first derivative, and then take its derivative to find the second derivative. Now set the second derivative equal to zero and solve for . To test , we’ll plug into the derivative. To test , we’ll plug into the derivative. Now we plot the results on our wiggle graph, and we can see that is Increasing on , Decreasing on and Increasing on . -----------------------|--------------------|----------------- - and -Intercepts To find the points where the graph intersects the and axes, we can plug into the original function for one variable and solve for the other. Local and Global Extrema Maxima and Minima (these are the plural versions of the singular words maximum and minimum) can only exist at critical points, but not every critical point is necessarily an extrema. To know for sure, you have to test each solution separately. Minimums exist at as well as . Based on the -values at those points, the global minimum exists at , and a local minimum exists at . If you’re dealing with a closed interval, for example some function on the interval to , then the endpoints and are candidates for extrema and must also be tested. We’ll use the First Derivative Test to find extrema. First Derivative Test Remember the wiggle graph that we created from our earlier test for increasing and decreasing? Example (continued) To find -intercepts, plug in for . Immediately we can recognize there are no -intercepts because we can’t have a result in the denominator. Let’s plug in for to try for - intercepts. Multiply every term by to eliminate the fraction. Since there are no solutions to this equation, we know that there are no - intercepts either for this particular function. Example (continued) Since our only inflection point was at , let’s go ahead and plot that on our wiggle graph now. --------------------------|----------------------- As you might have guessed, we’ll be testing values is the following intervals: and To test , we’ll plug into the second derivative. To test , we’ll plug into the second derivative. Now we can plot the results on our wiggle graph --------------------------|----------------------- We determine that is concave down on the interval and concave up on . Based on the positive and negative signs on the graph, you can see that the function is increasing, then decreasing, then increasing again, and if you can picture a function like that in your head, then you know immediately that we have a local maximum at and a local minimum at . You really don’t even need the silly First Derivative Test, because it tells you in a formal way exactly what you just figured out on your own: 1. If the derivative is negative to the left of the critical point and positive to the right of it, the graph has a local minimum at that point. 2. If the derivative is positive to the left of the critical point and negative on the right side of it, the graph has a local maximum at that point. As a side note, if it’s positive on both sides or negative on both sides, then the point is neither a local maximum nor a local minimum, and the test is inconclusive. Remember, if you have more than one local maximum or minimum, you must plug in the value of at the critical points to your original function. The values you get back will tell you which points are global maxima and minima, and which ones are only local. For example, if you find that your function has two local maxima, you can plug in the value for at those critical points. If the first returns a - value of and the second returns a -value of , then the first point is your global maximum and the second point is your local maximum. If you’re asked to determine where the function has its maximum/minimum, your answer will be in the form [value]. But if you’re asked for the value at the maximum/minimum, you’ll have to plug in the -value to your original function and state the -value at that point as your answer. Second Derivative Test You can also test for local maxima and minima using the Second Derivative Test if it easier for you than the first derivative test. In order to use this test, simply plug in your critical points to the second derivative. If your result is negative, that point is a local maximum. If the result is positive, the point is a local minimum. If the result is zero, you can’t draw a conclusion from the Second Derivative Test, and you have to resort to the First Derivative Test to solve the problem. Let’s try it. Good news! These are the same results we got from the First Derivative Test! So why did we do this? Because you may be asked on a test to use a particular method to test the extrema, so unfortunately, you should really know how to use both tests. Asymptotes Vertical Asymptotes Vertical asymptotes are the easiest to test for, because they only exist where the function is Example (continued) Our critical points are and . Since the second derivative is negative at , we conclude that there is a local maximum at that point. Since the second derivative is positive at , we conclude that there is a local minimum at that point. undefined. Remember, a function is undefined whenever we have a value of zero as the denominator of a fraction, or whenever we have a negative value inside a square root sign. Consider the example we’ve been working with in this section: You should see immediately that we have a vertical asymptote at because plugging in for makes the denominator of the fraction , and therefore undefined. Horizontal Asymptotes Vertical and horizontal asymptotes are similar in that they can only exist when the function is a rational function. When we’re looking for horizontal asymptotes, we only care about the first term in the numerator and denominator. Both of those terms will have what’s called a degree, which is the exponent on the variable. If our function is the following: then the degree of the numerator is and the degree of the denominator is . Here’s how we test for horizontal asymptotes. 1. If the degree of the numerator is less than the degree of the denominator, then the -axis is a horizontal asymptote. 2. If the degree of the numerator is equal to the degree of the denominator, then the coefficient of the first term in the numerator divided by the coefficient in the first term of the denominator is the horizontal asymptote. 3. If the degree of the numerator is greater than the degree of the denominator, there is no horizontal asymptote. Using the example we’ve been working with throughout this section, we’ll determine whether the function has any horizontal asymptotes. We can use long division to convert the function into one fraction. The following is the same function as our original function, just consolidated into one fraction: We can see immediately that the degree of our numerator is , and that the degree of our denominator is . That means that our numerator is one degree higher than our denominator, which means that this function does not have a horizontal asymptote. Slant Asymptotes Slant asymptotes are a special case. They exist when the degree of the numerator is greater than the degree of the denominator. Let’s take the example we’ve been using throughout this section. First, we’ll convert this function to a rational function by multiplying the first term by . Now that we have a common denominator, we can combine the fractions. We can see that the degree of our numerator is one greater than the degree of our denominator, so we know that we have a slant asymptote. To find the equation of that asymptote line, we divide the denominator into the numerator using long division and we get Right back to our original function! That won’t always happen, our function just happened to be the composition of the quotient and remainder. Whenever we use long division in this way to find the slant asymptote, the first term is our quotient and the second term is our remainder. The quotient is the equation of the line representing the slant asymptote. Therefore, our slant asymptote is the line . Putting It All Together Now that we’ve finished gathering all of the information we can about our graph, we can start sketching it. This will be something you’ll just have to practice and get the hang of. The first thing I usually do is sketch any asymptotes, because you know that your graph won’t cross those lines, and therefore they act as good guidelines. So let’s draw in the lines and . The asymptotes of Knowing that the graph is concave up in the upper right, and concave down in the lower left, and realizing that it can’t cross either of the asymptotes, you should be able to make a pretty good guess that it will look like the following: The graph of In this case, picturing the graph was a little easier because of the two asymptotes, but if you didn’t have the slant asymptote, you’d want to graph - and -intercepts, critical and inflection points, and extrema, and then connect the points using the information you have about increasing/decreasing and concavity. Optimization Optimization is one of the most feared topics for calculus students, but it really shouldn’t be. Optimization only requires a few simple steps, all of which you already know how to do. To solve an optimization problem, you’ll need to: 1. Write an equation in one variable that represents what you’re trying to maximize. 2. Take the derivative, find critical points and draw your wiggle graph. 3. Verify that your solutions are correct based on the real-life situation. Let’s do one of the most common examples. Example: The Open-Top Box I don’t know why this is such a popular optimization example, but I swear it’s in every calculus book ever written. Say you’re given a x piece of paper. You’re told to cut out squares from each corner with side-length , as follows, If we plug into our length, , we get a positive number. However, if we plug into our width, , we get a negative number, so cannot be a solution to our optimization problem. Now we only have to test to make sure it’s a local max. If it is a local max., then is the value of that maximizes the volume of our box. ----------------------------|----------------------- ----------------------------|----------------------- Since our function is increasing to the left of the critical point and decreasing to the right of it, is the value of that maximizes our volume. Multiplying everything together gives Now take the derivative with respect to . Find critical points by setting the equation equal to zero and solving for . Using the Quadratic Formula gives: Our critical points are approximately and . Before we draw our wiggle graph and start testing critical points, we should always test our answers for plausibility. Remember, length, width and height can never be negative. such that folding the sides up will create a box with no top. Your job is to find the value of that maximizes the volume of the box. As soon as you hear volume of a box, you should immediately write down the formula for the volume of a box: Based on the picture we drew of our problem, we already know our length, width and height, so we rewrite the formula as follows: Essential Formulas Foundations of Calculus Laws of Exponents Linear Functions Slope-Intercept Form , where is the slope and is the -intercept Point-Slope Form , where is the slope Slope of a Linear Function Quadratic Functions Quadratic Function Quadratic Formula Derivatives Definition of the Derivative Shortcut Rules The Power Rule The Product Rule The Quotient Rule The Chain Rule Logarithms & Exponentials
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