Prascius 1 Steven Prascius Mrs. Tallman AP Calculus 3 March 2014 Relationship between the Derivative and the Integral The fundamental Theorem of Calculus relates two very important aspects of Calculus together: The derivative and the integral. Both the derivative and integral are central parts of Calculus with nearly all parts of Calculus using them in some way. Because nearly all parts of Calculus relate to the derivative and the integral it is important to understand their properties. One part of the Fundamental Theorem of Calculus is the derivative. The derivative is the instantaneous rate of change of any function f(x), with respect to the x-value that corresponds to that point f(x). For example, if given a function showing the relationship between distance and time the derivative would be the instantaneous rate of change of distance over time at any given x-value of f(x), or in other words would be the exact velocity at that given time. The derivative of a function can numerically be found by taking the limit of the average rate of change over the interval from c as x approaches c. The derivative can be found graphically by finding the slope of function. The second part of the Fundamental Theorem of Calculus is the integral. The integral can either be a definite integral or an indefinite integral. The indefinite integral for a function, f(x), is simply the opposite of the derivative or the antiderivative. In other words the indefinite integral is the value of a function before a derivative is taken. For example, if given the value of the derivative of function f’(x) the indefinite integral would be equal to the original function f(x). The definite integral, however, relates to finding the area under the curve of a given function for Prascius 2 𝑏 a set interval. The notation for a definite integral is ∫𝑎 𝑓(𝑥) ∗ 𝑑𝑥 where a and b are the start and end points of an interval and f(x) is the function. The actual order of a and b is important 𝑏 𝑎 𝑏 because ∫𝑎 𝑓(𝑥) ∗ 𝑑𝑥 does not equal∫𝑏 𝑓(𝑥) ∗ 𝑑𝑥. The integral of ∫𝑎 𝑓(𝑥) ∗ 𝑑𝑥 is the same as 𝑎 ∫𝑏 𝑓(𝑥) ∗ 𝑑𝑥 but negative. This can be seen when solving the integrals. The integral of 𝑎 𝑏 ∫𝑏 𝑓(𝑥) ∗ 𝑑𝑥 is g(a) – g(b) whereas the integral of ∫𝑎 𝑓(𝑥) ∗ 𝑑𝑥 is g(b) – g(a) (with g(x) being the integral of f(x)) which shows that the integrals produce the same numerical values but just have a different sign. Since the integral is the opposite of the derivative integrating cancels out differentiation. If given the derivative of a function, taking the integral would result in getting the original function. For example, if a function shows the relationship of velocity and time taking the derivative would give a graph of acceleration over time whereas the integral would give a graph of distance over time. Another example can be seen when considering a function of acceleration over time. The derivative of this function would be the instantaneous rate of change of acceleration over time whereas the integral would be velocity over time. The opposite nature of the integral and derivative can also be seen when determining the units of a given graph. The units of the derivative of any given graph can be found by dividing the dependent variable, f(x), by the independent variable x of a graph. For example, if given a graph of distance (feet) over time (seconds) the derivative would be in feet per second because the dependent variable feet is divided by the independent variable seconds. The units of the integral, however, are found by multiplying the dependent variable by the independent variable. If given a graph of velocity (feet/second) over time (seconds) the integral would be in feet because the dependent Prascius 3 variable feet per second is multiplied by the independent variable seconds which cancels out the seconds leaving only feet as the unit. Relating to the graphs of integrals and derivatives are critical points. A critical point is a point on a graph where the derivative is zero or undefined. These critical points can be local maximums, local minimums, global maximums, global minimums, or points of inflection on the original function. Local max and mins are the max and mins of a certain portion of a function whereas the global max and mins are the max and mins for the entire function. Points of inflection are spots on a function where the function changes concavity, or the direction the function faces. These critical points give important information regarding the appearance of the original function and can be found using derivatives. The max and mins are found by taking the derivative of the original function and finding at what x-values the derivative is equal to zero. Once the x-values are determined the slope of the derivative is then looked at to determine if it is positive or negative. If the slope of the derivative is negative where the critical point is the point is a maximum, and if the slope is positive where the critical point is the point is a minimum. Points of inflection are found by taking both the first and second derivatives of the original function and then finding at what x-values the second derivative is equal to zero. These values correspond to where the points of inflections are on a graph. The signs of the first and second derivative also give important information about the original function. The sign of the first derivative determines whether the original function is increasing or decreasing. If the first derivative is positive (above the x-axis) the original function is increasing. This makes sense because the first derivative is the rate of change of the function and if the rate of change is positive then the function must be increasing. Because of this is makes sense that when the first derivative is negative (below the x-axis) the original function is Prascius 4 decreasing. When the first derivative is zero it shows that the original function has either a max or min at that point. The sign of the second derivative on the other hand determines the concavity of the original function. If the second derivative is positive then the original function is concave upwards and if the second derivative is negative then the original function is concave downwards. If the second derivative is zero it shows that there is a point of inflection on the original function at that point. Even though the second derivative is used to determine the concavity and locations of the points of inflection on the original function, the first derivative can determines these things to. The concavity of the original function can be determined by examining the slope of the first derivative. If the slope of the first derivative is positive then the original function is concave up and if the slope of the first derivative is negative then the original function is concave down. This makes sense because the second derivative is the rate of change of the first derivative so if the slope of the first derivative is positive then the second derivative is positive giving the original function an upward concavity with the same going for a negative slope. The points of inflection of the original function can be determined by finding the max and mins of the first derivative. These max and mins of the first derivative give the location of the points of inflection because they are where the slope of the derivative changes which causes a change in concavity of the original function which is what a point of inflection is. An example of using critical points and the signs of the first and second derivative to find information about the original function can be seen when considering figure 1. Prascius 5 Figure 1. Graph of f’(x) Figure 1 shows the derivative of the function f(x) in the interval from negative 5 to 5. By considering the derivative of the original function the local maximums and minimums of the original function can be found. The local maximums of f(x) occur when the derivative is zero and has a negative slope (which shows the function is concave down) and the minimums occur when the derivative is zero and has a positive slope. By looking at the derivative it is clear that the local maximums of f(x) must occur when x is 4 and -3 because that is where the derivative is zero and where the slope of the derivative is negative. Also, it is clear that the absolute minimum for f(x) must occur when x is 1 because that is where the derivative is zero and has a positive slope. This minimum is the absolute minimum on the graph because it is the only place a min occurs. The derivative of the original function can also be used to find the points of inflection of f(x). The points of inflections occur when the first derivative has a slope of zero. By looking at the graph it is clear that the points of inflection for f(x) must occur when x=-4,-1, and 2 because that is where the slope of the derivative is zero and also where the f(x) changes Prascius 6 concavity because of the change in direction of slope. Finally, the concavity of the original function f(x) can be found by looking at the sign of the slope of the first derivative. The original function is concave up from negative 5 to negative 4 and from negative 1 to 2 because that is where the slope of the derivative is positive. Also, f(x) has a positive slope from -5 to -3 and from -1 to -4 because that is where the derivative is positive which gives the original function a positive slope because the derivative is the slope of the original function The Fundamental Theorem of Calculus gives the relationship between the derivative and integral. The fundamental theorem of calculus comes in two forms which both relate integrals and derivatives to one another. The first part of the Fundamental Theorem of Calculus is an 𝑏 algebraic method for calculating definite integral and states ∫𝑎 𝑓(𝑥)𝑑𝑥 = g(b) – g(a) where g’(x) = f(x). This part of the theorem explains how a definite integral is found and states the derivative of the integral of f(x) is equal to the original function f(x). In order to calculate a definite integral the antiderivative g(x) of the original function must be found. One the antiderivative is found the limits a and b are then substituted into g(x) as g(b) and g(a) and then subtracted giving the value of the definite integral. This part of the Fundamental Theorem of Calculus can be applied to the function found in figure 1. If we are given function g which is equal to g(x) = 𝑥 ∫1 𝑓 ′ (𝑡)𝑑𝑡 and we have to find g(3) using the function in figure 1 we would find the definite integral of f’(x) from 1 to 3. When you take an integral of a derivative you get the original function f(x) so we are left with g(x) = f(x) integrated from 1 to 3. So to find g(3) we substitute the limits into f(x) and subtract them and get f(3)-f(1) = 3.9-3=0.9. The second part of the Fundamental Theorem of Calculus is the derivative of an integral form. This part of the theorem states that if the function is continuous on a closed interval [a,b] Prascius 7 𝑥 then g(x) = ∫𝑎 𝑓(𝑡)𝑑𝑡 ,when x is between a and b, is continuous on the closed interval [a,b] and differentiable on the open interval (a,b) , and g’(x) = f(x). This theorem states that the derivative of an integral is equal to the original function and that the derivative can be found by substituting x for t in the function f(t) and then multiplying the now f(x) by the derivative of x. This theorem is used when there is a variable for one of the limits of a definite integral. This theorem works because the constant limit becomes zero because its derivative is zero leaving only the variable part of the limit. This part of the Fundamental Theorem of Calculus can also be shown in an 𝑥 example from figure 1. If we were again given g(x) = ∫1 𝑓 ′ (𝑥)𝑑𝑥 and the function f’(x) and had to find g’(3) we would use this second part of the Fundamental Theorem. We would begin by integrating g(x) which would give us g(x) = f(x) because an integral of a derivative is just the original function. We would then take the derivative of both sides giving us g’(x) = f’(x) and plug in 3 as our x-value and look at the graph of f’(x) to determine what that is equal to. When looking at the graph it is clear that f’(3) and g’(3) are equal to 1. Going off this example is finding g’’(3) given the same information. Since g’(x) = f’(x) we would take the second derivative giving us g’’(x) = f’’(x) where would then plug in 3 as x to find g’’(3). Since the function in figure 1 is f’(x) we must find the slope or rate of change at x=3 to find out what g’’(3) equals. By finding the slope between the points (2,2) and (4,0) we come up with a slope of -1 which is what g’’(3) is equal to. Yet another example of how the second part of the Fundamental Theorem of Calculus is used can be see when considering the function of w(x) = 𝑔(𝑥) ∫1 𝑓(𝑡)𝑑𝑡 and the values found in table 1. If we had to find the value of w’(3) we would use Derivative of the Integral Form of the Fundamental Theorem because the upper limit of the function is a variable and the lower limit is a constant. When we solve for w’(3) we start by taking the derivative of w(x) which comes out to w’(x) = f(g(x))*g’(x) and then plug in 3 as x Prascius 8 and solve for w’(3) which comes out to be w’(3)=f(4)*2=-1*2=-2. So for this example w’(3) = 2. Another theorem relating to integrals and derivatives is the Intermediate Value Theorem. The theorem states that if a function is continuous for all x-values in the closed interval [a,b] and y is a number between f(a) and f(b) there is a number x = c in the interval (a,b) for which f(c) = y. This theorem basically means that given a y-value in the interval a to b there is a x-value that corresponds with that y-value which can be seen in figure 2 below Figure 2. Representation of the Intermediate Value Theorem An example of the Intermediate Value Theorem can be seen when considering table 1 below. Prascius 9 Table 1 Function Values Table 1 shows the functions F and G which are differentiable for all real numbers and where G is strictly increasing. Also, the function H is given by H(x) = F(G(x))-6. The Intermediate Value Theorem can be used to explain why there must be a value r for 1<r<3 such that H(r) =-5. In order to explain this, though, we must first determine if H(x) is continuous to see if the IVT applies. Since functions G and F are differentiable for all real numbers that means that H(x) is continuous and that the IVT applies. Now, the values of H(1) and H(3) must be found. When plugged into the table these values come out to be H(1) =F(G(1))-6=3 and H(3)=F(G(3))-6=-7. Since H(x) is continuous and because -5 is between 3 and -7 there must be a value of r for 1<r<3 such that H(r) = -5. Relating to the Intermediate Value Theorem is the Mean Value Theorem. The Mean Value Theorem states that if f(x) is continuous on the closed interval [a,b] and differentiable on the open interval (a,b) then there exists at least one point, c, in [a,b] where f’(c)= 𝑓(𝑏)−𝑓(𝑎) 𝑏−𝑎 . This basically means that given a continuous function there is a point c that has an instantaneous rate of change, or f’(c), that is equal to the average rate of change from a to b. In order for this theorem to apply, though, the function must be both continuous and differentiable. If the function is both continuous and differentiable then there must be one point c such that its Prascius 10 instantaneous rate of change is equal to the average rate of change from a to b. This theorem is demonstrated in figure 3 below. Figure 3. Mean Value Theorem Figure 3 shows a graph representing the Mean Value Theorem. As seen in the figure point c on the function has an instantaneous rate of change (shown as the tangent line) that is equal to the average rate of change between a and b (shown as the secant line). An example of the Mean Value Theorem can be seen when again considering table 1 and the function H(x). The Mean Value Theorem explains why there must be a value c for 1<c<3 such that H’(c)= -5. As previously mentioned, H(x) is both continuous and differentiable so that the Mean Value applies. Since the Mean Value Theorem applies then f’(c)= out to be -5 = −7−3 3−1 𝐻(𝑏)−𝐻(𝑎) 𝑏−𝑎 which comes or -5 = -5. Since the instantaneous rate of change f’(c) is the same as the average rate of change 𝐻(𝑏)−𝐻(𝑎) 𝑏−𝑎 and the function in continuous and differentiable then there must be a value c for 1<c<3 that corresponds to f’(c). Prascius 11 Another example that can be solved using the values in table 1 is to find an equation for the line tangent to the graph of y =G-1(x) at x = 2 where G-1 is the inverse function of G. In order to find the line tangent to the graph of y =G-1(x) at x = 2 we must first understand the relationship between G-1 and G. Since G-1 is the inverse to G then when G(1) = 2 the inverse G-1 is G-1(2)=1 because the x and the y get switched. When trying to find the line tangent to y =G-1(x) we must find the rate of change at that point which is just the derivative of G-1(2) because that is the slope of the line in the equation. The derivative of an inverse is found with the equation G-1’(x) = 1/(G’(G-1(x)) which comes out to be G-1’(2) = 1/(G’(G-1(2)) or G-1’(x) = 1/(G’(1)) which is equal to 1/5. Now that the slope of 1/5 is found you simply plug it in along with the x and y values into the line equation to get y = 1/5(x-2) +1 which is the equation for the line tangent to the graph of y =G-1(x) at x = 2. The final example involving table 1 is to find H’(3) if H(x) = x B(x) where B(x) = F-1(x). You begin by understanding the relationship between F-1(x) and F(x). Since F-1(x) is the inverse of F(x) when F(1) = 3 the inverse F-1(x) is F-1(3) = 1. You then take the derivative of H(x) which comes out to be H’(x) = 1*F-1(x) + x*F '1 (x) or H’(x) = 1*F-1(x) + x*1/(F’(F-1(x)) if you substitute F-1(x) in for B(x). You then solve for H’(3) by plugging in 3 for x and 1 for F-1(x). This comes out to be H’(3) = 1+ 3*1/(F’(1)) or H’(3) = 1 + ¾ or 1.75. The Fundamental Theorem of Calculus relates the integral and the derivative to each other. These two concepts are crucial to the understanding of Calculus and allow you to solve problems that would be impossible to solve otherwise. Prascius 12 Works Cited Dawkins, Paul. "Pauls Online Notes : Calculus I - The Mean Value Theorem." Pauls Online Notes : Calculus I - The Mean Value Theorem. Http://tutorial.math.lamar.edu/, n.d. Web. 02 Mar. 2014 Bohun, Sean. "Intermediate Value Theorem." Associate Professor Sean Bohun. Associate Professor Sean Bohun, n.d. Web. 02 Mar. 2014.