Cubic function cube function cube coefficient Chapter 13 Cubic Functions: Local Analysis Input-Output Pairs, 210 – Local I-O Rule Near ∞, 212 – Local Graph Near ∞, 213 – Local Features Near ∞, 214 – Addition Formula For Cubes, 216 – Local I-O Rule Near x0 , 219 – Local Coefficients Near x0 , 221 – Local Graph Near x0 , 225 – Local Features Near x0 , 226. Cubic functions are the result of adding-on a quadratic function to a cube function, that is a power function with exponent +3, or, the other way around, adding on a cube function to a quadratic function. Either way, cubic functions are specified by a global input-output rule of the form CU BICa,b,c,d x −−−−−−−−−−−−−→ CU BICa,b,c,d (x) = ax3 + bx2 + cx + d where CU BICa,b,c,d is the name of the cubic function and where a, b, c, d stand for the four bounded numbers that are needed to specify the cubic function CU BICa,b,c,d . In order to facilitate our investigation of cubic functions, it is necessary to begin by introducing some language special to cubic functions. Given the cubic function CU BICa,b,c,d , that is the function specified by the global input-output rule CU BICa,b,c,d x −−−−−−−−−−−−−→ CU BICa,b,c,d (x) = ax3 + b2 x + cx + d • The given signed number a is called the cube coefficient of the cubic function CU BICa,b,c,d and ax3 , that is the cube coefficient multiplied by 209 210 cube term square coefficient square term linear coefficient linear term constant coefficient constant term CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS three copies of the input, is called the cube term of the cubic function CU BICa,b,c,d . • The given signed number b is called the square coefficient of the cubic function CU BICa,b,c,d and bx2 , that is the square coefficient multiplied by two copies of the input, is called the square term of the cubic function CU BICa,b,c,d • The given signed number c is called the linear coefficient of the cubic function CU BICa,b,c,d and cx1 , that is the linear coefficient multiplied by one copy of the input, is called the linear term of the cubic function CU BICa,b,c,d • The given signed number d is called the constant coefficient of the cubic function CU BICa,b,c,d and dx0 , the constant coefficient multiplied by no copy of the input, is called the constant term of the cubic function CU BICa,b,c,d . In other words, the constant term is the same as the constant coefficient and what words we will use will depend on what viewpoint we will be taking. EXAMPLE 1. Given the function cubic function T AT A−3,+5,−2,+4 , that is the function specified by the global input-output rule T AT A−3,+5−2,+4 x −−−−−−−−−−−−−−−−−→ T AT A−3,+5,−2,+4 (x) = −3x3 + 5x2 − 2x + 4 is the cubic function whose • cube term is (−3)x3 , that is the cube coefficient −3 multiplied by three copies of the input x • square term is (+5)x2 , that is the square coefficient +5 multiplied by two copies of the input x • linear tern is (−2)x, that is the linear coefficient −2 multiplied by one copy of the input x • constant term is +4, that is the constant coefficient +4 multiplied by no copy of the input x. In other words, the constant term is the same as the constant coefficient. 13.1 Input-Output Pairs Given the cubic function CU BICa,b,c,d , that is the function specified by the global input-output rule CU BIC x −−−−−−−−−−→ CU BIC(x) = ax3 + bx2 + cx + d and given an input x0 , in order to get the output CU BIC(x0 ), we proceed as follows. 211 13.1. INPUT-OUTPUT PAIRS i. We read the global input-output rule: The output of CU BICa,b,c,d is obtained by multiplying a by 3 copies of the input, adding b multiplied by 2 copies of the input, adding c multiplied by 1 copy of the input and adding d. ii. We indicate that x is to be replaced by the given input x0 CU BIC x x←x0 −−−−−−−→ CU BIC(x) x←x0 = ax3 + bx2 + cx + d = ax30 + bx20 x←x0 + cx + d iii. When we are given specific numbers for a, b, c, d and for x0 , we can then identify the specifying-phrase ax30 + bx20 + cx0 + d to get the specific value of the output CU BICa,b,c,d (x0 ). EXAMPLE 2. Given the function T HORA specified by the global input-output rule T HORA x −−−−−−−−→ T HORA(x) = −42.17x3 − 32.67x2 − 52.39x + 71.07 and given the input −3, in order to get the input-output pair, we proceed as follows. i. We read the global input-output rule: “The output of T HORA is obtained by multiplying −32.67 by 2 copies of the input, adding −52.39 multiplied by 1 copy of the input, and adding +71.07” ii. We indicate that x is to be replaced by the given input −3 x x←−3 T HORA −−−−−−−−→ T HORA(x) x←−3 = −42.17x3 − 32.67x2 − 52.39x + 71.07 x←−3 which gives us the following specifying-phrase = (−42.17)(−3)3 + (−32.67)(−3)2 + (−52.39)(−3) + (+71.07) iii. We identify the specifying-phrase = +1138.59 − 294.03 + 157.17 + 71.07 = +1072.80 iv. Altogether, depending on the circumstances, we can then write any of the following: T HORA −3 −−−−−−−−→ +1072.80 T HORA(−3) = +1072.80 (−3, +1072.80) is an input-output pair for T HORA . 212 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS LOCAL ANALYSIS NEAR INFINITY Doing local analysis means working in a neighborhood of some given input and thus counting inputs from the given input since it is the center of the neighborhood. When the given input is ∞, counting from ∞ means to set x ← large and to compute with powers of large in descending order of sizes. NOTE. As it happens, the powers in global input-output rules are usually given in descending order of exponents which, when x is large, is in descending order of sizes. However, this is not an obligation and, when the powers in a global input-output rule are not given in descending order of exponents, in order to work in a neighborhood of ∞, the powers must be rearranged in descending order of exponents so as to be in descending order of sizes. 13.2 Local Input-Output Rule Near Infinity Given a cubic function CU BIC, we look for a function whose input-output rule will be simpler than the input-output rule of CU BIC but whose local graph near ∞ will still be qualitatively the same as the local graph near ∞ of CU BIC. 1. Given a cubic function CU BICa,b,c that is a function specified by the global input-ouput rule CU BICa,b,c,d x −−−−−−−−−−−−−→ CU BICa,b,c,d (x) = ax3 + bx2 + cx + d where a, b, c, d are bounded, when the input is large, the cube term of CU BICa,b,c,d is the principal term near ∞ of the output, because when the input is near ∞: • The bounded number a multiplied by three copies of a large input gives a result that is large, while • A bounded number multiplied by two copies of a large input will also be large but not as large and thus, regardless of its sign, will not change the size of the result which which will remain large • A bounded number multiplied by one copy of a large input will also be large but not as large and thus, regardless of its sign, will not change the size of the result which which will remain large and • adding the constant which is also bounded will even less change the size from being large. 13.3. LOCAL GRAPH NEAR ∞ 213 2. However, even though, for large inputs, the quadratic part of CU BIC is “too small to matter here”, it is not 0 and so we cannot write that CU BICa,b,c,d (x) is equal to the cube term ax3 and, in mathematics, we do want to write equalities, if only because they are easier to work with. So we will use the symbol +[...] to mean “plus something too small to matter here” and we will write CU BICa,b,c,d x|x near ∞ −−−−−−−−−−−→ CU BICa,b,c,d (x)|x near ∞ = ax2 + [...] which we will of course call the approximate local input-output rule near ∞ of the cubic function CU BICa,b,c,d . EXAMPLE 3. Given the cubic function M OAN+93.37−21.74,+31.59.−71.09 , that is the function specified by the global input-ouput rule M OAN x −−−−−−−→ M OAN (x) = +93.37x3 − 21.74x2 + 31.59x − 71.09 we can write M OAN x|x near ∞ −−−−−−−−→ M OAN (x)|x near ∞ = +93.37x3 + [...] In other words, we have: THEOREM 1 (Approximation Near ∞). Near ∞ the output of a cubic function is principally its cube term. 13.3 Local Graph Near Infinity We get the qualitative local graph near ∞ as follows: i. We use the Approximation Near ∞ Theorem to get the approximate local input-output rule near ∞ ii. We normalize it so that, depending on the sign of the coefficient, we get the local input-output rule of either the cube function or the opposite cube function, iii. We draw the corresponding local graph near ∞.. EXAMPLE 4. Given the cubic function ALM A−38.38,−21.36,−45.78,+53.20 , find its local graph near ∞. ALBA−21.36,−45.78,+53.20 is specified by the global input-output rule: ALM A x −−−−−−−→ ALM A(x) = −38.38x3 − 21.36x2 − 45.78x + 53.20 214 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS i. The approximate local input-output rule near ∞ is: ALM A x|x near ∞ −−−−−−−−−−→ ALM A(x)|x near ∞ = −38.38x+3 + [...] ii. We normalize ALM A ALM A∗ x|x near ∞ −−−−−−−−−−→ ALM A(x)|x near ∞ = −x+3 + [...] Output Ruler +∞ ) iii. The local graph near ∞ of ALM A is: ( Screen –∞ –∞ 13.4 ) ) +∞ Input Ruler Local Features Near Infinity Once we have the local graph of the function CU BIC near ∞, we can “read” the local features off the local graph near ∞ as in Chapter 4. This is a good way to proceed but not in the long run because it is too slow. And, in fact, once we have a mental picture of the two possible qualitative local graphs near ∞, in order to decide which of the two is the actual case in the instance, we need only know what the place of the local graph is and this is given by THEOREM 2 (Height-sign Near ∞). Given the function CU BICa,b,c,d : • W hen Sign a = +, Height-sign CU BIC |near ∞ = (+, −) • W hen Sign a = −, Height-sign CU BIC |near ∞ = (−, +) And of course we also have the other two local features near ∞: THEOREM 3 (Slope-sign Near ∞). Given the function CU BICa,b,c,d : • When Sign a = +, Slope-sign CU BIC |near x0 = (, ) • When Sign a = −, Slope-sign CU BIC |near x0 = (, ) (Keep in mind that the feature signs near ∞ are coded while facing ∞ and not while facing 0.) 215 13.4. LOCAL FEATURES NEAR ∞ THEOREM 4 (Concavity-sign Near ∞). Given the function CU BICa,b,c,d : • W hen Sign a = +, Concavity-sign CU BIC |near ∞ = (∪, ∩) • W hen Sign a = −, Concavity-sign CU BIC |near ∞ = (∩, ∪) EXAMPLE 5. Given the cubic function M AON−38.82,+34.54,−40.38,−94.21 , that is the function specified by the global input-output rule M AON x −−−−−−−−−−→ M AON (x) = −38.82x3 + 34.54x2 − 40.38x − 94.21 we find its local features near ∞ as follows. i. The local features near ∞ according to the Local Features Theorem are: • Height-sign |x near ∞ = (−, +) • Slope-sign |x near ∞ = (−, −) • Concavity-sign |x near ∞ = (−, +) which, translated back into our language, gives • Height-sign |x near ∞ = (−, +) • Slope-sign |x near ∞ = (, ) • Concavity-sign |x near ∞ = (∪, ∩) ii. Should we want to check that the Local Features Theorem gave us the correct information, we would get the normalized approximate local input-output rule near ∞ M AON ∗ x|x near ∞ −−−−−−−−−−−→ M AON ∗ (x)|x near ∞ = −x3 + [...] Output Ruler ) +∞ Screen ( and then the local graph near ∞ from which we get the following local features – + –∞ –∞ ) ) +∞ Input Ruler which are the same as those that were given by the Local Features Theorem keeping in mind that the local graph near ∞ is viewed here by Mercator rather than by Magellan. LOCAL ANALYSIS NEAR A FINITE INPUT Doing local analysis means working in a neighborhood of some given input and thus counting inputs from the given input since it is the center of the neighborhood. When the given input is x0 , we localize at x0 , that is we set x = x0 + h where h is small and we compute with powers of h in descending order of sizes. (See Section 2.7 Analysis Near Finite Inputs. EXAMPLE 6. Given the input +2, then the location of the number +2.3 relative to +2 is +0.3: 216 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS addition formula for cubes +2 ( +0.3 0 Neighborhood of +2 Input Ruler ) +3 +2 +1 0 13.5 +2.3 = +2 +0.3 Addition Formula For Cubes In order to get the local input-output rule of a given cubic function near a given finite input x0 , we need first to get an addition formula to give us (x0 + h)3 in terms of x0 and h and which we will call the addition formula for cubes. We prefer to establish it here, ahead of time, rather than in the midst of the developing the local input-output rule. There are two approaches. 1. The computational approach. We “just” multiply three copies of (x0 + h): a. We begin by multiplying two copies of (x0 + h): x0 + h x0 + h x20 x20 + h2 + x0 h x0 h + 2x0 h + h2 b. We multiply x20 + 2x0 h + h2 , the result of the multiplication of two copies of (x0 + h), by a third copy of (x0 + h): x20 + 2x0 h + h2 x0 + h x20 h 2x20 h + + 2x0 h2 x 0 h2 + h3 x30 + 3x20 h 2. The graphic approach. + 3x0 h2 + h3 +h We go back to the real world and to the definition of double multiplication in terms of the volume of a rectangle so that (x0 + h)3 is the volume of a x0 + h by x0 + h by x0 + h cube: x0+h x0 + x0+h x30 (x0+h)3 217 13.5. ADDITION FORMULA FOR CUBES What we then do is to get this volume by starting with an x0 by x0 by x0 cube, the initial cube, and then augment the sides of the initial cube by h and see how the volume increases. For the sake of clarity, we will augment the cube one step at a time: x0 i. The sides of the initital cube are equal to x0 and the volume of the initial cube is therefore x30 : ii. We now augment the sides of the initial cube by h in each dimension which adds three x0 + h by x0 + h by h slabs to the initial cube: x0 x0 x0 x0 h x0 h x0 x0 x0 h iii. We glue the three slabs to the initial cube which, however, leaves three grooves: h iv. We fill the three grooves with three x0 by h by h rods: h x0 h h x0 x0 h h 218 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS v. We glue the three rods in the three grooves which leaves a hole in the corner: vi. We complete the enlargement of the initial cube by adding one h by h by h cube to fill the indentation in the corner: vii. Altogether, the volume of the enlarged cube, whose side is x0 + h is therefore: x30 + 3x20 h + 3x0 h + h2 + h3 h h h h x0 h x0 h h x0 3. Contrary to what one might think at first, the graphic approach is greatly preferable because it has three major advantages over the computational approach: i. The terms in the sum automatically come in order of diminishing sizes. Indeed, since x0 is finite and h is small, • all three dimensions of the “initial cube” are finite, say “in the ones”, so x30 is also finite or “in the ones”, • two dimensions of the “slabs” are finite, say “in the ones”, but the third dimension is small, say “in the tenths”, so the volume of the slabs is small: since x0 is “in the ones” and h is “in the tenths”, then 3x20 h will also be “in the tenths”, • one dimension of the “rods” is finite, say “in the ones”, but the other two dimensions are small, say “in the tenths”, so the volume of the rods is smaller: since x0 is “in the ones” and h is “in the tenths”, then 3x0 h2 will be “in the hunfredths”, • all three dimensions of the “little cube” are small so that the volume of the little cube is even smaller than the volume of the slabs: if h is “in the tenths”, then h3 will be “in the thousandths”. ii. If all we need is only a particular one of the terms, and this will very 13.6. LOCAL I-O RULE NEAR X0 219 often be the case, we can get it straight from the picture without having to go through the whole multiplication. iii. Later on, when we shall need formulas for (x0 + h)4 , (x0 + h)5 , etc, not only will the length of the computational approach get very rapidly out of hand but, as we shall see, since we will never need more than the first two or three terms of the result, the computational approach will also become more and more inefficient. On the other hand, even though we will not be able to draw pictures as we have been able to do so far, one can extend the patterns we have found so far in the graphic approach and the graphic approach will thus survive. In any case, we have THEOREM 5 (Addition Formula For Cubes). (x0 + h)3 = x30 + 3x20 h + 3x0 h2 + h3 13.6 Local Input-Output Rule Near A Finite Input Since x0 is given for the duration of the local investigation and since it is therefore h that will be the actual input, we will think in terms of a local function, that is of a function which returns for h the same output that the given global function would return for x = x0 + h. In order to get the input-output rule of the local function function when the given function is a cubic function, we proceed just as we did in the case of quadratic functions: i. We replace x by x0 + h (where h is small) in the global inputoutput rule, ii. We use the Addition Formula For Squares to compute (x0 + h)2 , iii. We use the Multiplication Theorem to compute with h. More precisely, given the cubic function CU BICa,b,c,d , that is the function specified by the global input-output rule CU BIC x −−−−−−−−−−→ CU BIC(x) = ax3 + bx2 + cx + d and given a finite input x0 , 220 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS i. We localize the function CU BIC at the given input x0 , that is we count inputs from the given imput x0 instead of from the origin of the input ruler. In other words, we use the location of x in relation to the given input x0 , that is we replace in the global input-output rule x by x0 + h, (where h is small). CU BICa,b,c,d x|x←x0 +h −−−−−−−−−→ CU BICa,b,c,d (x)|x←x0 +h = ax3 + bx2 + cx + d x←x0 +h = a[x0 + h]3 + b[x0 + h]2 + c[x0 + h] + d ii. Using the Addition Formula Theorems, we get h i h i h i = a x30 + 3x20 h + 3x0 h2 + h3 + b x20 + 2x0 h + h2 + c x0 + h + d = ax30 + 3ax20 h + 3ax0 h2 + ah3 + bx20 + 2bx0 h + bh2 + cx0 + ch + d iii. We collect terms of like size in order of diminishing sizes: [ ] [ ] [ ] [] = ax30 + bx20 + cx0 + d + 3ax20 + 2bx0 + c h + 3ax0 + b h2 + a h3 We then have: THEOREM 6 (Local Input-Output Rule). Given the cubic function CU BIC specified by the global input output rule CU BIC x −−−−−−−−−−→ CU BIC(x) = ax3 + bx2 + cx + d the local function CU BIC(x0 ) is specified by the local input-output rule CU BIC(x ) 0 h −−−−−−−− → CU BICx0 (h) = [ax 3 0 ] [ ] [ ] [] + bx20 + cx0 + d + 3ax20 + 2bx0 + c h + 3ax0 + b h2 + a h3 BEN EXAMPLE 7. Given the cubic function x −−−−−→ BEN (x) = −2x3 + 3x2 − 5x + 7, and given an input, say x0 = −4, we get the local input-output rule near x0 = −4 by localizing at −4 and then “just” do the computations as follows: BEN −4 + h −−−−−−−−−→ BEN (−4 + h) = −2x3 + 3x2 − 5x + 7x←−4+h 3 2 = −2 − 4 + h + 3 − 4 + h − 5 − 4 + h + 7 221 13.7. LOCAL COEFFICIENTS NEAR X0 and, using the Addition Formula Theorem with x0 = −4, i h i h = −2 (−4)3 + 3(−4)2 h + 3(−4)h2 + h3 + 3 (−4)2 + 2(−4)h + h2 h i −5 −4+h +7 h i h i h i = −2 − 64 + 48h − 12h2 + h3 + 3 + 16 − 8h + h2 − 5 − 4 + h + 7 local local local local constant coefficient linear coefficient quadratic coefficient cubic coefficient = +128 − 96h + 24h2 − 2h3 + 48 − 24h + 3h2 + 20 − 5h + 7 We collect terms of like size in order of diminishing sizes: = [ + 203] + [ − 125]h + [ + 27]h2 + [ − 2]h3 The local function BEN(−4) is therefore specified by the local input-output rule BEN(−4) h −−−−−−−−−−−→ BEN−4 (h) = +203 − 125h + 27h2 − 2h3 13.7 Local Coefficients Near A Finite Input When looking only for one of the local features, instead of computing the whole local input-ouput rule, we will only compute the single term of the local input-ouput rule that controls the local feature. More precisely, given a function CU BIC specified by the global inputoutput rule: CU BIC x −−−−−−−−−−→ CU BIC(x) = ax3 + bx2 + cx + d and whose local input-output rule near x0 is therefore CU BIC(x0 ) h −−−−−−−−−−−−→ CU BIC(x0 )|x←x0 +h [ ] [ ] [ ] [] = ax30 + bx20 + cx0 + d + 3ax20 + 2bx0 + c h + 3ax0 + b h2 + a h3 we will say that • ax30 + bx20 + cx0 + d is the local constant coefficient, [ ] • [3ax + 2bx + c] is the local linear coefficient, • [3ax + b] is the local quadratic coefficient. • [a] is the local cubic coefficient. 2 0 0 0 and we will now investigate how to get just a single one of the local coefficients without getting the whole local input-output rule. At first, getting 222 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS just this one single term rather than the whold local input-output rule will look more difficult than getting the whole local input-output rule but, with a little bit of practice, writing less and less each time, this will soon get easy. We begin by writing CU BICa,b,c,d x|x←x0 +h −−−−−−−−−→ CU BICa,b,c,d (x)|x←x0 +h = ax3 + bx2 + cx + d x←x0 +h = a[x0 + h]3 + b[x0 + h]2 + c[x0 + h] + d a. To find the local constant coefficient, we proceed as follows: i. Since the Addition Formula for Cubes is: (x0 + h)3 = x30 + 3x20 h + 3x0 h2 + h3 the contribution of a[x0 + h]3 to the local constant term will be a · x30 h0 ii. Since the Addition Formula for Squares is: (x0 + h)2 = x20 + 2x0 h + h2 the contribution of b[x0 + h]2 to the local constant term will be b · x20 h0 iii. The contribution of c[x0 + h] to the constant term will be c · x0 h0 iv. The contribution of d to the local constant term will be d · h0 Altogether, the contributions to the local constant term add up to: a · x30 h0 + b · x20 h0 + c · x0 h0 + d · h0 = ax30 h0 + bx20 h0 + cx0 h0 + dh0 [ ] = ax30 + bx20 + cx0 + d h0 and therefore the local constant coefficient is: ax30 + bx20 + cx0 + d b. To find the local linear coefficient, we proceed as follows i. Since the Addition Formula for Cubes is: (x0 + h)3 = x30 + 3x20 h + 3x0 h2 + h3 the contribution of a[x0 + h]3 to the local linear term will be a · 3x20 h ii. Since the Addition Formula for Squares is: (x0 + h)2 = x20 + 2x0 h + h2 the contribution of b[x0 + h]2 to the local linear term will be b · 2x0 h 223 13.7. LOCAL COEFFICIENTS NEAR X0 iii. The contribution of c[x0 + h] to the local linear term will be c · h iv. The contribution of d to the local linear term will be nothing. Altogether, the linear term adds up to: a · 3x20 h + b · 2x0 h + c · h = 3ax0 h2 + 2bx0 h + ch [ ] = 3ax20 + 2bx0 + c h and therefore the local linear coefficient is: 3ax20 + 2bx0 + c c. To find the local square coefficient, we proceed as follows: i. Since the Addition Formula for Cubes is: (x0 + h)3 = x30 + 3x20 h + 3x0 h2 + h3 the contribution of a[x0 + h]3 to the local square term will be a · 3x0 h2 ii. Since the Addition Formula for Squares is: (x0 + h)2 = x20 + 2x0 h + h2 the contribution of b[x0 + h]2 to the local square term will be b · h2 iii. The contribution of c[x0 + h] to the local square term will be nothing iv. The contribution of d to the local square term will be nothing. Altogether, the square term adds up to: a · 3x0 h2 + b · h2 = 3ax0 h2 + bh2 [ ] = 3ax0 + b h2 and therefore the local square coefficient is: 3ax0 + b d. To find the local cube coefficient we proceed as follows: i. Since the Addition Formula for Cubes is: (x0 + h)3 = x30 + 3x20 h + 3x0 h2 + h3 the contribution of a[x0 + h]3 to the local cube term will be a · h3 local cube coefficient 224 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS ii. Since the Addition Formula for Squares is: (x0 + h)2 = x20 + 2x0 h + h2 the contribution of b[x0 + h]2 to the local cube term will be nothing iii. The contribution of c[x0 + h] to the local cube term will be nothing iv. The contribution of d to the local cube term will be nothing. Altogether, the cube term “adds up” to: a · h3 = ah3 [] = a h3 and therefore the local cube coefficient is: a In fact, it is usually better to write only the terms that are relevant to what we want. BEN EXAMPLE 8. Given the cubic function x −−−−−→ BEN (x) = −2x3 + 3x2 − 5x + 7, and given the input −4, find the local square term. We start as usual: BEN −4 + h −−−−−−−−−→ BEN (−4 + h) = −2x3 + 3x2 − 5x + 7x←−4+h 3 2 = −2 − 4 + h + 3 − 4 + h − 5 − 4 + h + 7 now, instead of using the full Addition Formula Theorems, we just pick the h2 terms in each addition formula: h i h i h i = −2 (· · · + 3(−4)h2 + · · · + 3 · · · + h2 − 5 · · · + · · · where 3(−4)h2 are the three rods in the enlarged cube and +h2 is the little square in the enlarged square. So, h i h i h i = −2 · · · − 12h2 · · · + 3 · · · + h2 − 5 · · · + · · · = · · · + 24h2 · · · + · · · + 3h2 + · · · + · · · and, collecting “like” terms, = [ · · · ] + [ · · · ]h + [ + 27]h2 + [ · · · ]h3 So, the quadratic term in the local input-output rule of BEN when x is near −4 is: +27h2 225 13.8. LOCAL GRAPH NEAR X0 13.8 Local Graph Near A Finite Input The local graph of a given cubic function CU BICa,b,c,d near a given input x0 is the graph of the local function CU BIC(x0 ) , that is the graph of the function specified by the local input-output rule of CU BICa,b,c,d near x0 . So, in order to get the local graph of the given cubic function CU BIC near the given input x0 , we: i. Get the local graph of the constant term of CU BIC(x0 ) , ii. Get the local graph of the linear term of CU BIC(x0 ) , iii. Add-on (as we did in Chapter 8) the local graph of the linear term to the local graph of the constant term to get the local graph of the affine part of CU BIC(x0 ) iv. Get the local graph of the square term of CU BIC(x0 ) v. Add-on (as we did in Chapter 8) the local graph of the the local graph of the square term to the local graph of the affine part to get the local graph of CU BIC(x0 ) EXAMPLE 9. Given a cubic function SHIP and given that the local input-output rule of SHIP near the input −4 is SHIP(−4) h− −−−−−−−−−−− → SHIP(−4) (h) = +75 − 29h + 3h2 − 4h3 construct the local graph of SHIP near −4, that is the graph of SHIP(−4) . i. We get the local graph of the constant term of SHIP(−4) : h −−−−−→ +75 Output Ruler Screen +75 0 that is ( ii. We get the local graph of the linear term of SHIP(−4) : –4 ) Input Ruler ) Input Ruler Output Ruler Screen h −−−−−→ −29h that is 0 ( –4 226 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS iii. We get the local graph of the affine part of SHIP(−4) by adding-on the linear term to the constant term: Output Ruler Screen h −−−−−→ +75 − 29h +75 0 that is ( iv. We get the local graph of the square term of SHIP(−4) : Output Ruler –4 ) Input Ruler ) Input Ruler Screen h −−−−−→ +3h 2 0 that is ( v. We get the full local graph of SHIP(−4) by adding-on the square term to the affine part: Output Ruler h −−−−−→ +75 − 29h + 3h2 –4 Screen vi. And +75 0 that is ( since the local graph has concavity, we are done! 13.9 –4 ) Input Ruler Local Features Near A Finite Input Once we have the local graph of the function CU BIC near x0 , we can “read” the local features off the local graph near x0 as in Chapter 4. This is a good way to proceed but not in the long run because it is too slow. Given the cubic function CU BICa,b,c,d , that is the function specified by the global input-output rule CU BIC x −−−−−−−−−−→ CU BIC(x) = ax3 + bx2 + cx + d what controls the local features of CU BIC near x0 are the local coefficients, that is the coefficients in the local input-output rule near x0 CU BIC(x0 ) h −−−−−−−−−−−−→ CU BIC(x0 )|x←x0 +h [ ] [ ] [ ] = ax30 + bx20 + cx0 + d + 3ax20 + 2bx0 + c h + 3ax0 + b h2 + [...] 227 13.9. LOCAL FEATURES NEAR X0 1. The local constant term [ax 3 0 ] + bx20 + cx0 + d gives the Height-sign near x0 because it contributes most of the local height since, as long as h remains small, the other two terms of the local input-ouput rule, namely the linear term and the square term are small and therefore contribute very little to the total height and certainly not enough to change the sign of the total local height. The local constant coefficient is therefore what determines the height-sign near any finite input x0 THEOREM 7 (Height-sign Near x0 ). Given the function CU BICa,b,c,d • W hen Local constant coefficient of CU BIC(x0 ) = +, Height-sign CU BIC |near x0 = (+, +) • W hen Local constant coefficient of CU BIC(x0 ) = −, Height-sign CU BIC |near x0 = (−, −) • W hen Local constant coefficient of CU BIC(x0 ) = 0, Height-sign CU BIC|near , x0 depends on the sign of the local linear coefficient of CU BIC(x0 ) 2. The local linear term [3ax 2 0 ] + 2bx0 + c h contibutes most of the local slope because the constant term has no slope and the square term contributes very little to the total slope—as long as h remains small—certainly not enough to change the sign of the total slope. The local linear coefficient is therefore what controls the Slope-sign near any finite input x0 : THEOREM 8 (Slope-sign Near x0 ). Given the function CU BICa,b,c,d • W hen Local linear coefficient of CU BIC(x0 ) = +, Slope-sign CU BIC |near x0 = (, ) • W hen Local linear coefficient of CU BIC(x0 ) = −, Slope-sign CU BIC |near x0 = (, ) • W hen Local linear coefficient of CU BIC(x0 ) = 0, Slope-sign CU BIC|near, x0 depends on the sign of the local square coefficient of CU BIC(x0 ) 228 CHAPTER 13. CUBIC FUNCTIONS: LOCAL ANALYSIS 3. The local square term [3ax 0 ] + b h2 contributes all of the local concavity because neither the constant term nor the linear term have any concavity. The local square term is therefore what controls the Concavity-sign near any finite input x0 : THEOREM 9 (Concavity-sign Near x0 ). Given the function CU BICa, b, c, d • W hen Local square coefficient of CU BIC(x0 ) = +, Concavity-sign CU BIC |near x0 = (∪, ∪) • W hen Local square coefficient of CU BIC(x0 ) = −, Concavity-sign CU BIC |near x0 = (∩, ∩) • W hen Local square coefficient of CU BIC(x0 ) = 0, Concavity-sign CU BIC| , near x0 depends on the sign of the local cube coefficient of CU BIC(x0 ) 4. We look at a couple of examples. EXAMPLE 10. Given the function specified by the global input-ouput rule JIM x −−−−−→ JIM (x) = +2x3 + 3x2 − 36x + 1 and given the input +2, in order to find the slope-sign near +2 we must get the linear term in the local input-ouput rule near +2. Whichever way we proceed, we get the local input-ouput rule of JIM near +2 JIM(+2) h −−−−−−−−→ JIM(+2) (h) = [ ] + [ 0 ]h + [ ]h + [...] 2 Since the linear term vanished, the slope-sign will be given by the square term. After recomputing, we get JIM(+2) h −−−−−−−−→ JIM(+2) (h) = [ ] + [ 0 ]h + [ + 15]h 2 + [...] and therefore, Slope-sign near +2 = (, ). EXAMPLE 11. Given the function specified by the global input-ouput rule KAY x −−−−−→ KAY (x) = +1x3 + 3x2 − 9x + 17 229 13.9. LOCAL FEATURES NEAR X0 and given the input −1, in order to find the concavity-sign near −1 we must get the square term in the local input-ouput rule near −1. Whichever way we proceed, we get the local input-ouput rule of KAY near −1 KAY(−1) h −−−−−−−−→ KAY(−1) (h) = [ ] + [ ]h + [ 0 ]h 2 + [...] Since the square term vanished, the concavity-sign will be given by the cube term. After recomputing, we get KAY(−1) h −−−−−−−−→ KAY(−1) (h) = [ ] + [ ]h + [ 0 ]h + [ + 1]h and therefore, Concavity-sign near −1 = (∩, ∪). 2 3
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