Differential Calculus 201-SN2-RE • CEGEP, Montreal
Corrected exercises: L'Hôpital's rule and indeterminate forms (201-SN2-RE)
Here are fifteen corrected exercises on indeterminate forms and L'Hôpital's rule, as the differential calculus course 201-SN2-RE (formerly 201-NYA) requires them. The chapter comes at its natural place: the differentiation rules have just been established, and the first thing you do with them is use them to compute limits that algebra cannot resolve.
Exercise 0.1 opens the set with twelve limits to compute directly with L'Hôpital's rule, as in textbook drill lists: algebraic 00 forms, with a root, trigonometric, exponential and logarithmic, two successive differentiations for 1−cos3xx2, ∞∞ forms between exponential, power and logarithm, then the forms 0⋅∞, ∞−∞, 1∞ with (cosx)x21 and 00, each with its value to find and checked on the spot.
Part A sorts and equips: recognizing a form, stating the rule and its hypotheses, rewriting a product or a difference as a quotient, handling transcendental functions, going through the logarithm for the exponential forms. Part B puts it all to work: growth rates, oblique asymptotes, differentiable extension, and a physics problem where the limit without air resistance gives back free fall. Part C takes on the classics: the three ways the rule fails, the pocket-sized expansion, the order of contact, the catenary and continuous interest.
The thread of the set: L'Hôpital's rule is not a rule for computing limits, it is a cure for one specific pathology. Two moves follow from that and come back from one exercise to the next. Check the indeterminate form BEFORE every differentiation, because applied to a healthy limit the rule gives a result that has nothing to do with it. And ask yourself whether the limit is not, in disguise, a derivative you already know, in which case applying the rule would be circular.
Self-checking setType your answers and check them question by question: the page tells you right or wrong before you open the solution. With an account, every answer right on the first try earns points, and your right answers stay filled in when you come back.
•Indeterminate forms: 00, ∞∞, 0⋅∞, ∞−∞, 00, 1∞, ∞0. Everything else is settled by substitution.
•L'Hôpital's rule: if the form is 00 or ∞∞, if f and g are differentiable near a with g′=0, and if limg′f′ EXISTS, then limgf=limg′f′.
•Differentiate the top and the bottom SEPARATELY: this is not the quotient rule. And check the form again before every new round.
•Product 0⋅∞: move to the denominator the factor whose derivative complicates the expression. Difference ∞−∞: common denominator, factoring or conjugate.
•Exponential forms: set y=fg, compute limlny=glnf, then conclude limy=eL. Never forget the last step.
•A derivative in disguise, limx→ax−af(x)−f(a)=f′(a), is read off the table without any computation, and L'Hôpital's rule would be circular on it.
•Growth rates: lnx≪xp≪bx for all p>0 and b>1. Between two exponentials, the larger base wins.
•Oblique asymptote: a=limxf(x), then b=lim(f(x)−ax), both limits being almost always indeterminate.
•Three ways to fail: the rule goes in circles, the quotient of derivatives has no limit, or every round makes things worse. Remedies: algebra, squeezing, change of variable.
•Order of contact: lim(x−a)nf−g=C=0 gives the order n, which is the order of the first derivatives that stop agreeing.
Calculations: limits to resolve with L'Hôpital's rule
Exercise 0.1: Applying L'Hôpital's rule: twelve direct calculations
For each limit, name the indeterminate form obtained by substitution, apply L'Hôpital's rule as many times as necessary, then give the value of the limit.
One method for all twelve lines: substitute first and name the form; if it is not 00 or ∞∞, rewrite it as a quotient (move a factor down for 0⋅∞, common denominator for ∞−∞, logarithm for the exponential forms); differentiate the numerator and the denominator SEPARATELY; substitute again, and start over only if the form is still indeterminate.
a) limx→2x3−8x4−16.
b) limx→4x−42x+1−3.
c) limx→0sin5xtan2x.
d) limx→0sin2xe3x−e−x.
e) limx→1x2−1lnx.
f) limx→01−cos3xx2.
g) limx→+∞x2+4e3x.
h) limx→+∞3xlnx.
i) limx→1(1−x)tan(2πx).
j) limx→0(ex−11−x1).
k) limx→0(cosx)x21.
l) limx→0+x1+lnx3.
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Answers
a)34x at 2; 38≈2.667
b)2x+11 at 4; 31
c)5cos(5x)2sec2(2x) at 0; 52
d)2cos2x3e3x+e−x at 0; 2
e)2x21 at 1; 21
f)9cos3x2 at 0, after two rounds; 92
g)29e3x, after two rounds; +∞
h)3x3; 0
i)cot(2πx)1−x; π2≈0.637
j)x(ex−1)x−ex+1, two rounds; −21
k)lny→−21; e−21≈0.607
l)lny→3; e3≈20.086
The move that decides everything happens BEFORE you differentiate: substitute and name the form. Only 00 and ∞∞ allow the rule; the five other forms are first rewritten as a quotient, and the check is done again before EVERY new differentiation.
a)
Form 00. Differentiate: 3x24x3=34x→38≈2.667.
b)
Form 00. Differentiate: 122x+12=2x+11→31≈0.333. Pitfall: forgetting the factor 2 from the inner derivative, which gives 61.
c)
Form 00. Differentiate: 5cos(5x)2sec2(2x)→52.
d)
Form 01−1=00. Differentiate: 2cos2x3e3x+e−x→23+1=2. Pitfall: (e−x)′=−e−x, and the minus sign of the difference turns it into a plus.
e)
Form 00, since ln1=0. Differentiate: 2xx1=2x21→21.
f)
Form 00. Differentiate: 3sin3x2x, still 00; differentiate again: 9cos3x2→92≈0.222. Pitfall: stopping after the first round, or forgetting the 3 at each differentiation of the cosine.
g)
Form ∞∞. Differentiate: 2x3e3x, still ∞∞; differentiate again: 29e3x→+∞. The exponential beats any power.
h)
Form ∞∞. Differentiate: 31x−32x1=x313→0. The logarithm loses against any positive power, even x31.
i)
Form 0⋅∞. Turn the tangent into a cotangent: cot(2πx)1−x, of the form 00. Differentiate: −2πcsc2(2πx)−1→π2≈0.637. Pitfall: the factor 2π from the inner derivative.
j)
Form ∞−∞. Common denominator: x(ex−1)x−ex+1, of the form 00. Differentiate: ex−1+xex1−ex, still 00; differentiate again: 2ex+xex−ex→−21.
k)
Form 1∞. Set y=(cosx)x21, so lny=x2ln(cosx), of the form 00. Differentiate: 2x−tanx, still 00; differentiate again: 2−sec2x→−21. Therefore y→e−21≈0.607. Pitfall: answering −21, the limit of the logarithm and not that of y.
l)
Form 00, since lnx→−∞ makes the exponent tend to zero. Set lny=1+lnx3lnx, of the form ∞∞. Differentiate: x1x3=3. Therefore y→e3≈20.086. Pitfall: believing that a 00 form is always worth 1.
Check: on the calculator, evaluate the original expression very close to the point, for example at a+0.001, or for a large value of x; the number displayed must approach the limit you found. For the exponential forms, convergence is slow: check the limit of lny instead.
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Part A: the basics (/50)
Exercise 1: Indeterminate, determinate, or a derivative in disguise?
Before differentiating anything, you have to sort. A limit can be DETERMINATE, and be obtained by plain substitution; INDETERMINATE, and call for a tool; or be nothing more than a DERIVATIVE in disguise, that is, the limit limx→ax−af(x)−f(a)=f′(a) written backwards.
That third case is the most interesting one in the course: you recognize it, you read the answer in the table of derivatives, and there is nothing to compute.
a) Compute limx→0x1+x−1 by recognizing it as a derivative at a point. Which function, at which point?
b) Do the same for limx→2x−2x5−32 and for limh→0hsin(6π+h)−21.
c) Among these four limits, which ones are indeterminate? limx→0x2+3x+1, limx→0+xlnx, limx→∞7x3−42x3+x, limx→0x1−cosx. Conclude for those that are not.
d) Compute the two that remain, with the appropriate method.
e) A student writes: “the limit is indeterminate, so it does not exist”. Refute this, and propose the correct wording.
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Answers
a)21, the derivative of 1+x at 0
b)80 and 23
c)Only the third and the fourth are indeterminate
d)72 and 0
e)“Indeterminate” describes the FORM, not the limit: it says that work is needed
a)
You recognize x−0f(x)−f(0) with f(x)=1+x and f(0)=1. The limit is therefore f′(0). Now f′(x)=21+x1, so f′(0)=21. No manipulation, no differentiation of the quotient: the table of derivatives has already done the work.
b)
First limit: x−2x5−25 is the difference quotient of f(x)=x5 between 2 and x, so the limit is f′(2)=5×24=80. Second: hsin(6π+h)−sin6π is the difference quotient of the sine at 6π, so the limit is cos6π=23≈0.866. The signal to remember: a − followed by the value of the function at the point, divided by the distance to the point, almost always announces a derivative.
c)
x2+3x+1 at 0 equals 31 by substitution: DETERMINATE. xlnx at 0+ gives 0+−∞, which is not an indeterminate form: the limit is −∞. The other two are indeterminate: ∞∞ for the third, 00 for the fourth. Watch the trap in the second one: 00 is indeterminate, but 0nonzero never is.
d)
limx→∞7x3−42x3+x is settled by ALGEBRA, factoring x3 out of the top and the bottom: the limit is 72. L'Hôpital's rule would give the same result in three differentiations, which would be a waste. limx→0x1−cosx is indeed 00; differentiating top and bottom, 1sinx→0. The limit is 0, and the example shows that an indeterminate form can perfectly well have a finite limit, zero included.
e)
The sentence confuses the FORM and the LIMIT. “Indeterminate” describes the expression obtained by substitution, not the behaviour of the function: it only means that substitution is not enough to conclude, and that one more tool is needed. The three limits limx→0xx2=0, limx→0xx=1 and limx→0x3x=∞ are all of the form 00 and have three different behaviours: that is exactly what the word “indeterminate” describes. Correct wording: “substitution gives the indeterminate form 00, so the indeterminate form must be resolved”, then you state the result. A limit can also fail to exist, like limx→0sinx1, but that is not the same thing, and it has to be proved.
Exercise 2: L'Hôpital's rule, its hypotheses, and the circular argument it hides
RULE. If limx→ag(x)f(x) has the form 00 or ∞∞, if f and g are differentiable near a except possibly at a, if g′ is never zero there, and if limx→ag′(x)f′(x) exists, then limx→ag(x)f(x)=limx→ag′(x)f′(x).
You differentiate the NUMERATOR and the DENOMINATOR separately. This is not the quotient rule.
a) Compute limx→0x2e2x−1−2x, stating the form obtained BEFORE each differentiation.
b) A student computes limx→1x+1x2+3 with L'Hôpital's rule and finds 12x=2. Where is the mistake, and what is this limit really?
c) Another one computes limx→0xex−1 by applying the QUOTIENT rule to the expression. Explain the confusion.
d) A third one, for limx→0xsin3x, applies L'Hôpital's rule and gets 3cos3x→3. The result is right. Why is this reasoning nevertheless CIRCULAR?
e) State, in one sentence, the rule of conduct that these three cases impose.
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Answers
a)2, after two differentiations
b)No indeterminate form: the limit is 2 by substitution, the student's result is right BY CHANCE
c)The quotient rule differentiates the EXPRESSION, L'Hôpital's rule differentiates top and bottom SEPARATELY
d)The derivative of the sine was established from this very limit
e)Check the indeterminate form before EVERY differentiation, and ask where the derivative being used comes from
a)
At x=0: the numerator equals 1−1−0=0 and the denominator 0: form 00, the rule applies. Differentiate: 2x2e2x−2, which is still 00 at 0: CHECK, and start over. 24e2x→24=2. The limit is 2. The move you must never skip is the intermediate check: you may apply the rule again as many times as the indeterminate form PERSISTS, but only once you have made sure of it.
b)
The mistake is to apply the rule without checking for an indeterminate form. At x=1, the numerator equals 4 and the denominator 2: the form is 24, perfectly determinate, and since the function is continuous at 1, the limit is obtained by substitution: it is 2. The student also finds 2, but through wrong reasoning: it is a coincidence, and the same procedure on limx→1x+3x2+3 would give 12=2 instead of 1. A method that lands on the right answer by chance is worth zero marks.
c)
The quotient rule is used to DIFFERENTIATE a function that is a quotient; L'Hôpital's rule is used to compute a LIMIT of a quotient, and it requires differentiating the top and the bottom SEPARATELY. The two have neither the same purpose nor the same result: here the quotient rule would give x2xex−(ex−1), which is the derivative of the function, not its limit at 0. The confusion comes from the fact that both statements talk about “differentiating a quotient”; the cure is to ask yourself each time what you are looking for, a derivative function or a limit value.
d)
Because the derivative of the sine was ESTABLISHED from the limit limx→0xsinx=1, proved by the Squeeze Theorem in the chapter on limits. Using (sinu)′=cosu to prove again a limit of this family assumes what you want to prove. The result, 3, is indeed correct; it is the PROOF that is flawed. The proper write-up sets u=3x and invokes the special limit: xsin3x=3⋅3xsin3x→3×1=3. The same warning applies to limx→0xex−1 and limx→0xln(1+x), which ARE the derivatives that were used to build the table.
e)
The rule of conduct comes in two steps. First: CHECK the indeterminate form before every differentiation, never just once at the start. Second: before applying the rule, ask yourself whether the limit is not itself the derivative that was used to establish the derivative you are about to use; if so, conclude directly from the definition or from the special limit, without going through L'Hôpital's rule.
Exercise 3: The forms 0·∞ and ∞ − ∞: turn everything into a quotient
The rule handles ONLY the forms 00 and ∞∞. The other indeterminate forms are brought back to these by rewriting.
For a product 0⋅∞, move one of the two factors to the denominator: uv=1/vu. For a difference ∞−∞, use a common denominator, factor, or multiply by the conjugate.
a) Compute limx→0+xlnx. Two rewritings are possible: try both and say which one works.
b) Compute limx→∞x(2π−arctanx).
c) Compute limx→1(lnx1−x−11).
d) Compute limx→∞(x−x2−4x). Why is L'Hôpital's rule the wrong tool here?
e) Sum up in one sentence the criterion that decides which factor to move in a product.
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Answers
a)0; only the rewriting x−1/2lnx works
b)1
c)21
d)2; the conjugate is faster and safer
e)Move down the factor whose derivative COMPLICATES the expression, keep on top the one it simplifies
a)
Form 0⋅(−∞). First rewriting, 1/lnxx: the derivative of the denominator is −x(lnx)21, and the quotient of derivatives becomes −2xx(lnx)2, worse than at the start. Second rewriting, x−1/2lnx, of the form +∞−∞: differentiate, −21x−3/21/x=−2x1/2→0. The limit is 0. The logarithm SIMPLIFIES when differentiated, the root does not: the logarithm is the one to keep on top.
b)
Form ∞⋅0, since arctanx→2π. Move the factor x down: 1/x2π−arctanx, of the form 00. Differentiate: −x21−1+x21=1+x2x2→1. The limit is 1, which can also be read this way: the gap between arctanx and its asymptote decreases like x1.
c)
Form ∞−∞, both terms diverging at 1. Use a common denominator: (x−1)lnx(x−1)−lnx, of the form 00. Differentiate: lnx+xx−11−x1=xlnx+x−1x−1, still 00. Differentiate again: lnx+1+11→21. The limit is 21. Going to a common denominator is compulsory: differentiating each term separately makes no sense, the rule is about a QUOTIENT.
d)
Form ∞−∞. The conjugate: x−x2−4x=x+x2−4xx2−(x2−4x)=x+x2−4x4x. Dividing top and bottom by x, the denominator tends to 2 and the limit is 2. L'Hôpital's rule would be the wrong tool for two reasons: you would first have to rewrite the difference as a quotient, which is already the conjugate's job; and differentiating a square root gives back a square root, so that the expression never simplifies and the rule goes in circles. Practical rule: faced with a difference of two roots, or of a root and a polynomial, ALWAYS try the conjugate first.
e)
The criterion: move to the denominator the factor whose derivative COMPLICATES the expression, and keep on top the one whose derivative simplifies it. A logarithm simplifies when differentiated, and so does a power; an exponential and a root do not. When in doubt, try, and give up as soon as the quotient of derivatives is heavier than the original.
Exercise 4: Transcendental functions at work: exponential, logarithm and arctangent
The previous chapter gave the derivatives of the transcendental functions. These four limits put them all to use, and each one asks you to count the rounds before concluding.
a) Compute limx→0x3arctanx−x.
b) Compute limx→0x2ln(1+x)−x.
c) Compute limx→∞x2(e1/x−1−x1).
d) Compute limx→∞ln(x3+x)ln(x2+1).
e) Each of the first three limits is negative or positive, and that sign means something precise. What do they say about the graph of each function relative to its tangent line at 0?
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Answers
a)−31
b)−21
c)21
d)32
e)Negative sign: the curve lies BELOW its tangent line. Positive sign: above it
a)
Form 00. Differentiate: 3x21+x21−1=3x2(1+x2)−x2=3(1+x2)−1→−31. Simplifying ALGEBRAICALLY after the first differentiation saves two rounds of the rule: it always pays to check whether the quotient of derivatives simplifies before differentiating again.
b)
Form 00. Differentiate: 2x1+x1−1=2x(1+x)−x=2(1+x)−1→−21. Same remark: the simplification falls into place by itself.
c)
Form ∞⋅0. Set u=x1, which tends to 0+: the expression becomes u2eu−1−u, of the form 00. Differentiate: 2ueu−1, still 00; differentiate again: 2eu→21. The change of variable is safer here than moving a factor down directly, because it replaces a limit at infinity by a limit at zero, where forms are easier to read.
d)
Form ∞∞. Differentiate: x3+x3x2+1x2+12x=(x2+1)(3x2+1)2x(x3+x)=(x2+1)(3x2+1)2x2(x2+1)=3x2+12x2→32. You could also conclude without differentiating: ln(x2+1)∼2lnx and ln(x3+x)∼3lnx, so the quotient tends to 32. Both routes are accepted; the second is faster and more robust.
e)
Each limit compares a function with its linear approximation at 0, that is, with its TANGENT LINE. For the arctangent, arctanx−x≈−3x3: the gap is negative for x>0 and positive for x<0, so the curve crosses its tangent line, the sign of an INFLECTION point at 0. For the logarithm, ln(1+x)−x≈−2x2: the gap is negative on BOTH sides, so the curve stays below its tangent line, which corresponds to a graph that is concave down. For the exponential, eu−1−u≈+2u2: the curve stays ABOVE its tangent line, concave up. An indeterminate limit of this kind therefore gives more than a number: it tells you on which side of its tangent line the curve lies, and how fast it moves away from it. That is exactly the information you will use in the chapter on curve sketching.
Exercise 5: The three exponential forms: go through the logarithm
A limit of the form f(x)g(x) can be indeterminate in three ways: 00, 1∞ and ∞0. None of them can be handled directly.
The method is always the same, in three steps. Set y=f(x)g(x) and write lny=g(x)lnf(x), which is a 0⋅∞ form you already know; compute limlny=L; conclude limy=eL.
a) Compute limx→0+(tanx)x, naming the form.
b) Compute limx→∞(x−1x+2)x.
c) Compute limx→0+(x1)sinx.
d) A student writes: “the base tends to 1, and 1 raised to any power is 1, so the limit in b) is 1.” Refute this by computation.
e) Another one correctly finds limlny=0 in a) and answers 0. What is the right answer, and which step was skipped?
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Answers
a)1, form 00
b)e3≈20.09, form 1∞
c)1, form ∞0
d)The base tends to 1 but the exponent tends to infinity: their tug of war is settled by the logarithm
e)The limit is e0=1: the return to the exponential was forgotten
a)
Form 00, since tanx→0+ and x→0+. Set y=(tanx)x, so lny=xln(tanx), of the form 0⋅(−∞). Move a factor down: 1/xln(tanx), of the form +∞−∞. Differentiate: −x21tanx1+tan2x=−tanxx2(1+tan2x). Since tanx∼x near 0, this behaves like −x→0. Therefore lny→0 and y→e0=1.
b)
Form 1∞, the base tending to 1 and the exponent to infinity. Set lny=xlnx−1x+2, of the form ∞⋅0. Move a factor down: 1/xln(x+2)−ln(x−1), of the form 00. Differentiate: −x21x+21−x−11=−x21(x+2)(x−1)−3=(x+2)(x−1)3x2→3. Therefore lny→3 and y→e3≈20.09.
c)
Form ∞0, since x1→+∞ and sinx→0. Set lny=sinx⋅lnx1=−sinxlnx. Since sinx∼x, this behaves like −xlnx, whose limit is 0. Therefore y→e0=1. You could also write 1/sinx−lnx and differentiate, but recognizing sinx∼x shortens everything.
d)
The reasoning confuses a base EQUAL to 1 with a base that TENDS to 1. If the base were exactly 1, the power would be 1 whatever the exponent. But here the base is 1+x−13, so it exceeds 1 by a little, and that excess is raised to the power x, which tends to infinity. Two opposite tendencies fight it out, and the outcome depends on their RATES: that is exactly what the word “indeterminate” describes. The computation settles it: the limit is e3≈20.09, twenty times the announced answer. An immediate counterexample to convince yourself: (1+x1)x→e, not 1.
e)
The right answer is 1, and the skipped step is the last one: the method computes the limit of the LOGARITHM of the expression, not that of the expression. You must therefore go back to the exponential, y=elny→e0=1. The mistake is all the easier to make because the auxiliary variable y often vanishes from the paper; the cure is to write it explicitly on the first line, “let y=…”, and to finish with “therefore y→eL”. A marker takes off one or two marks for this omission, which turns e3≈20 into 3 in case b).
Part B: problems and reasoning (/50)
Exercise 6: Growth rates: the hierarchy that decides the shape of a curve
At infinity, the functions that diverge do not all do so at the same rate. The hierarchy is established once and for all with L'Hôpital's rule, and it is then used without computing anything again.
The rule: the LOGARITHM is beaten by any power, and any power is beaten by any exponential with base greater than 1.
a) Prove that limx→∞x(lnx)2=0.
b) Compute limx→∞x3e−x and limx→∞2xx.
c) Rank by growth at infinity: lnx, x, xlnx, x2, 2x, ex. Justify the two least obvious comparisons.
d) Beyond which value of x does ex>x3 hold for good? Solve to within 0.01.
e) What do the two limits in b) say about the shape of the graphs of x3e−x and 2xx?
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Answers
a)0, after two applications of the rule
b)0 in both cases
c)lnx<x<xlnx<x2<2x<ex
d)For x>4.54 approximately
e)Both curves rise, reach a maximum, then come back down towards the axis
a)
Form ∞∞. Differentiate: 12lnx⋅x1=x2lnx, still ∞∞. Differentiate again: 12/x=x2→0. The limit is 0. The mechanism is clear: each differentiation lowers the power of the logarithm by one notch without touching the x at the bottom, so the logarithm always runs out in the end. The same reasoning gives limxp(lnx)n=0 for all n and p>0.
b)
x3e−x=exx3, form ∞∞. Three successive differentiations give ex3x2, then ex6x, then ex6→0. Each round lowers the degree of the polynomial by one while the exponential stays itself: it always wins. For 2xx: 2x=exln2, whose derivative is 2xln2, so the quotient of derivatives is 2xln21→0. The base 2 is smaller than e, but that changes nothing: any exponential with base greater than 1 beats any power.
c)
In order: lnx<x<xlnx<x2<2x<ex. The two least obvious comparisons are the following. First x against xlnx: the quotient is xlnxx=xlnx1→0, so xlnx wins, even though it contains the logarithm, because the logarithm is multiplied by a whole x. Next 2x against ex: ex2x=(e2)x with e2≈0.736<1, so this quotient tends to 0: between two exponentials, the larger base wins, and no derivative is needed.
d)
You are looking for where ex=x3, that is, taking the logarithm, where x=3lnx. The function h(x)=x−3lnx gives h(4)=4−4.159=−0.159 and h(5)=5−4.828=+0.172: there is a root between 4 and 5. Refining, h(4.53)=−0.0022 and h(4.54)=+0.0012: the root is approximately 4.54. Beyond it, the exponential wins for good. Check: e4.54=93.7 and 4.543=93.6, almost equal. This figure is worth remembering: the exponential's victory over the cube does not start at infinity, it starts before 5.
e)
Both functions are 0 at 0, positive afterwards, and tend to 0 at infinity by b). A continuous positive function that starts at zero and comes back to it must reach a MAXIMUM somewhere: both curves rise, peak, then come back down and flatten onto the x-axis, which is a horizontal asymptote. The derivative locates the peak: for x3e−x, it is x2e−x(3−x), so the maximum is at x=3, where the function equals 27e−3≈1.34. This is how comparing growth rates pays off in graphical information: without it, you would not know whether the curve comes back down to the axis or shoots off to infinity.
Exercise 7: Oblique asymptotes of transcendental functions
A curve has the oblique asymptote y=ax+b at +∞ when a=limx→∞xf(x) exists and is finite and nonzero, and b=limx→∞(f(x)−ax) exists and is finite.
Both limits are almost always indeterminate: this is the most common use of L'Hôpital's rule in a function analysis.
a) For f(x)=xe1/x, compute a=limx→∞xf(x).
b) Compute b=limx→∞(xe1/x−x), then give the asymptote.
c) For g(x)=xarctanx, find the oblique asymptote at +∞.
d) Find the one at −∞. Do the two answers have the same y-intercept?
e) Does the graph of f lie above or below its asymptote at +∞? Justify by pushing the computation one step further.
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Answers
a)a=1
b)b=1, so y=x+1
c)y=2πx−1
d)y=−2πx−1: yes, the same y-intercept −1
e)Above: the gap is approximately 2x1, positive
a)
xf(x)=e1/x, and x1→0, so a=e0=1. No indeterminate form here: always try substitution before pulling out the rule.
b)
f(x)−x=x(e1/x−1), of the form ∞⋅0. Set u=x1→0+: the expression becomes ueu−1, of the form 00, whose limit is 1, either by L'Hôpital's rule or by recognizing the derivative of the exponential at 0. Therefore b=1 and the asymptote is y=x+1. Notice that here, recognizing the derivative, as in exercise 1, spares you any differentiation.
c)
xg(x)=arctanx→2π, so a=2π. Next g(x)−2πx=x(arctanx−2π), of the form ∞⋅0. This is the opposite of the limit computed in exercise 3b, which was 1: so b=−1 and the asymptote at +∞ is y=2πx−1.
d)
At −∞, arctanx→−2π, so a=−2π. Then g(x)+2πx=x(arctanx+2π): moving a factor down, 1/xarctanx+2π, of the form 00, whose differentiation gives −x211+x21=−1+x2x2→−1. The asymptote is therefore y=−2πx−1. Both y-intercepts are −1: that is to be expected, since g is EVEN, and the reflection in the y-axis swaps the two asymptotes. A free check: when a function is even, its two oblique asymptotes are symmetric, so they have opposite slopes and the same y-intercept.
e)
Compute the gap f(x)−(x+1)=x(e1/x−1)−1. With u=x1, this reads ueu−1−u, which tends to 0, confirming the asymptote. To know the SIGN of this gap, push one step further: you know from exercise 4c that u2eu−1−u→21, so eu−1−u≈2u2 and the gap is approximately 2u=2x1, POSITIVE for x>0. The curve therefore lies ABOVE its asymptote and approaches it from above, the gap still being 0.005 at x=100. This is the information missing from most papers: finding the asymptote does not tell you from which side the curve approaches it, and a sketch on the wrong side loses a mark.
Exercise 8: Five statements to correct
Each of the following five sentences has been heard in tutoring sessions. Say what is wrong with it, then write the correct version. Naming the rule that is broken is worth half the marks.
a) “The form is indeterminate, so the limit does not exist.”
b) “L'Hôpital's rule means differentiating the quotient, then substituting.”
c) “Once you have applied the rule, you can apply it again as many times as you like.”
d) “limx→0xsinx=1 is proved by L'Hôpital's rule in one line.”
e) “limx→∞(1+x2)x=1, because the base tends to 1.”
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Answers
a)False: “indeterminate” describes the form, not the limit
b)False: you differentiate the top and the bottom SEPARATELY
c)False: only as long as the indeterminate form PERSISTS, which you check at every round
d)False: it is circular, the derivative of the sine comes from this limit
e)False: the limit is e2≈7.39
a)
FALSE. “Indeterminate” describes the FORM obtained by substitution, not the behaviour of the function. The limits of xx2, xx and x3x at 0 are all of the form 00 and are 0, 1 and +∞ respectively: that is precisely why the form determines nothing. Correct version: “substitution gives an indeterminate form, so the indeterminate form must be resolved”.
b)
FALSE, and it is the most costly confusion of the chapter. The quotient rule is used to differentiate a FUNCTION that is a quotient; L'Hôpital's rule is used to compute a LIMIT, and it requires differentiating the numerator and the denominator SEPARATELY, which does not produce the same expression at all. Correct version: “replace gf by g′f′, never by g2f′g−fg′”.
c)
FALSE. You may apply the rule again as long as the indeterminate form PERSISTS, and you must check it before every round. Applied to a determinate form, it gives a result that has nothing to do with it: on limx→0x2+2x+1, which is 21, one round of the rule would give 2x1, which blows up at 0. Correct version: “check the form at every step, and stop as soon as it is no longer indeterminate”.
d)
FALSE, and the error is one of logic rather than computation. The result is right, but the proof assumes the derivative of the sine is known, and that derivative was established FROM this very limit, by the Squeeze Theorem. You cannot prove a statement by relying on a consequence of that statement. Correct version: “this limit is proved by a geometric squeeze; L'Hôpital's rule recovers it, but does not prove it”.
e)
FALSE. The base tends to 1 but the exponent tends to infinity: this is the indeterminate form 1∞, and the two tendencies fight it out. The logarithm computation gives lny=xln(1+x2), whose limit is 2, so the limit sought is e2≈7.39. Correct version: “a base that TENDS to 1 is not a base EQUAL to 1; the form 1∞ is handled through the logarithm”. It is the same error as believing that a number very close to 1 raised to a huge power stays close to 1, whereas an interest rate of two percent compounded a hundred times multiplies the capital by more than seven.
Exercise 9: Extend by continuity, then differentiate the extension
A function that is undefined at a but whose limit at a exists can be EXTENDED by continuity: set f(a)=limx→af(x). The next question, which is the question of differential calculus, is whether the extension is DIFFERENTIABLE at a, and that is decided by a second indeterminate limit, the limit of the difference quotient.
a) Extend f(x)=xex−1 at 0.
b) Is the extension differentiable at 0? Compute f′(0) from the definition.
c) Do the same for g(x)=xsinx: value at 0, then g′(0).
d) The function h(x)=xlnx, extended by h(0)=0, is it differentiable at 0? Conclude.
e) Check the result of b) numerically by comparing f(0.1) with 1+20.1.
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Answers
a)f(0)=1
b)Yes, f′(0)=21
c)g(0)=1 and g′(0)=0
d)No: the difference quotient is lnx, which tends to −∞
e)f(0.1)=1.0517 against 1.05: the gap is 1.7×10−3
a)
The limit limx→0xex−1 has the form 00; it is the derivative of ex at 0, so it equals 1. Set f(0)=1, and the function so extended is continuous on all of R.
b)
By definition, f′(0)=limx→0x−0f(x)−f(0)=limx→0xxex−1−1=limx→0x2ex−1−x. This limit has the form 00; differentiate: 2xex−1, still 00; differentiate again: 2ex→21. The extension is therefore DIFFERENTIABLE at 0, with f′(0)=21. Notice that you CANNOT get this result by differentiating the expression xex−1 and then substituting 0: that derivative is not defined at 0. Only the definition works at the point where the pieces are joined.
c)
limx→0xsinx=1, so g(0)=1. Then g′(0)=limx→0xxsinx−1=limx→0x2sinx−x. Form 00; differentiate: 2xcosx−1, still 00; differentiate again: 2−sinx→0. Therefore g′(0)=0: the sinc function has a HORIZONTAL tangent line at 0, which its symmetry already suggested, since a differentiable even function always has a zero derivative at 0.
d)
limx→0+xlnx=0, computed in exercise 3, so the extension h(0)=0 is continuous. But the difference quotient is x−0h(x)−h(0)=xxlnx=lnx, which tends to −∞: the function is NOT differentiable at 0. Its graph has a VERTICAL tangent line there: the curve leaves the origin heading straight down. The lesson matters: continuity of the extension never guarantees its differentiability, and the second computation must be done. Here the difference quotient is not even an indeterminate form, it is read off directly.
e)
f(0.1)=0.1e0.1−1=0.10.105171=1.05171. The linear approximation given by b) is f(0)+f′(0)×0.1=1+0.05=1.05. The gap is 1.7×10−3, that is 0.16%: the agreement confirms that f′(0)=21 and not, say, 1 or 41, which would give 1.10 and 1.025 respectively. This numerical check takes thirty seconds and catches most differentiation errors: whenever you announce a derivative at a point, you can always test it on a small x.
Exercise 10: Problem: falling with air resistance, and the limit without resistance
A skydiver of mass m falling under air resistance proportional to speed reaches, after a time t, the speed v(t)=kmg(1−e−kt/m), where k is the drag coefficient, in kg/s.
Data: m=80 kg, g=9.81 m/s², k=12 kg/s.
a) Compute the terminal speed, reached as t→∞, in m/s.
b) Compute the speed after 3.0 s, in m/s, and compare it with free fall gt.
c) Without air resistance, you expect v=gt. Show that limk→0+v(t)=gt for fixed t. Which form do you get?
d) Push the computation one step further to obtain the approximation v(t)≈gt(1−2mkt) for short times.
e) Apply d) at t=0.50 s and compare with the exact value. Up to what time does the free-fall approximation stay good to within 5%?
Show the solution
Answers
a)65.4 m/s, that is 235 km/h
b)23.7 m/s against 29.4 m/s: 80.5% of free fall
c)Form 00 in the variable k; the limit is indeed gt
d)v(t)≈gt(1−2mkt), from u1−e−u≈1−2u with u=mkt
e)4.72 m/s against 4.73; free fall stays good to within 5% up to about 0.69 s
a)
As t→∞, e−kt/m→0 and v→kmg=1280×9.81=65.4 m/s, that is 235 km/h. This is the terminal speed, at which drag exactly balances the weight: no indeterminate form here, but it sets the scale of the whole problem.
b)
mkt=8012×3.0=0.45, so v(3.0)=65.4(1−e−0.45)=65.4×0.3624=23.7 m/s. Free fall would give gt=9.81×3.0=29.4 m/s: the skydiver is going 20% slower than the model without air resistance predicts, after only three seconds.
c)
For fixed t, let k tend to 0+. The factor kmg diverges and the factor in parentheses tends to 0: form ∞⋅0. Rewrite it as a quotient IN THE VARIABLE k: v=kmg(1−e−kt/m), of the form 00. Differentiate with respect to k, the numerator giving mg⋅mte−kt/m=gte−kt/m and the denominator 1: the quotient tends to gte0=gt. The model with air resistance therefore gives back free fall when the resistance disappears, which is the first check to run on any physics formula. The point of method: the variable of differentiation is k, not t; mixing the two up is the classic error in this kind of exercise.
d)
Start again from 1gte−kt/m obtained in c) and expand the gap to the limit. Setting u=mkt, v=kmg(1−e−u)=gt⋅u1−e−u. Now exercise 4 established that u2eu−1−u→21, which gives here u1−e−u≈1−2u. Hence v(t)≈gt(1−2u)=gt(1−2mkt). The relative correction is therefore 2mkt: it is proportional to time, and smaller the heavier the body.
e)
At t=0.50 s: 2mkt=16012×0.50=0.0375, so v≈9.81×0.50×0.9625=4.72 m/s. The exact value is 65.4(1−e−0.075)=4.726 m/s: the agreement is to within about a thousandth. For free fall alone, without correction, to stay good to within 5%, you need 2mkt<0.05, that is t<122×80×0.05=0.67 s. The exact check gives 0.69 s. In other words, the high-school free-fall formula is only usable for the first two thirds of the first second: after that, the air matters. This is the kind of conclusion that an indeterminate limit lets you put a number on, and that no intuition provides.
Part C: the classics (/50)
Exercise 11: When L'Hôpital's rule goes in circles, refuses to answer, or makes things worse
The rule is not universal. It has three ways of failing, all recognizable in the first rounds, and each one has its remedy.
a) Try limx→∞x+1x2+4 with L'Hôpital's rule. What happens? Then conclude with algebra.
b) Try limx→∞3x+sinx2x+cosx. What does the rule give? Does the limit exist all the same? Which precise hypothesis is violated?
c) Try limx→0+xe−1/x. What happens to the quotient after each differentiation? Find the remedy.
d) Compute limx→0xx+x2sinx1, first with the rule, then correctly.
e) Sum up the three ways of failing and the remedy for each one.
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Answers
a)The rule goes in circles; algebra gives 1
b)The rule gives a quotient with no limit; the true limit is 32
c)Every round makes it worse; the change of variable u=x1 gives 0
d)The rule fails; the limit is 1
e)Going in circles, quotient of derivatives with no limit, getting worse: algebra, squeezing, change of variable
a)
Form ∞∞. Differentiate: 1x2+4x=x2+4x, still ∞∞. Differentiate again: x2+4x1=xx2+4: you are back at the starting point, up to the constant. The rule GOES IN CIRCLES. With algebra, factor x out of the top and the bottom: x(1+x1)x1+x24→1.
b)
Form ∞∞. The rule gives 3+cosx2−sinx, whose numerator oscillates between 1 and 3 and denominator between 2 and 4: this quotient has NO limit at +∞. Yet the limit sought exists: dividing by x, 3+xsinx2+xcosx→32, since the two oscillating terms are bounded and divided by x. The violated hypothesis is the last one in the statement: “IF limg′f′ exists”. The rule is a one-way implication; when the quotient of derivatives has no limit, it says nothing at all, and certainly not that the original limit does not exist.
c)
Form 00, since e−1/x→0 very fast. Differentiate the numerator: (e−1/x)′=x2e−1/x, and the denominator gives 1: the quotient becomes x2e−1/x, where the exponent of x has INCREASED. Every round makes the situation worse, and the rule will never end. The remedy is a CHANGE OF VARIABLE: set u=x1→+∞, and the expression becomes ue−u=euu, which tends to 0 by comparison of growth rates. The limit is 0.
d)
Form 00. The rule gives 11+2xsinx1−cosx1, whose term cosx1 oscillates endlessly as x→0: the quotient of derivatives has no limit, and the rule does not conclude. Correctly, simplify FIRST: xx+x2sinx1=1+xsinx1, and since xsinx1≤∣x∣→0 by squeezing, the limit is 1. It is the same way of failing as in b), with the same lesson: simplifying the expression before differentiating is often faster than the rule, and sometimes it is the only way.
e)
The three ways. FIRST, going in circles: the quotient of derivatives gives back the original quotient, as in a); the remedy is algebra, factoring out the dominant term or using the conjugate. SECOND, the quotient of derivatives has no limit, as in b) and d); the remedy is simplifying or squeezing, by isolating the bounded terms. THIRD, getting worse: every round makes the expression heavier, as in c); the remedy is a change of variable, usually u=x1, which turns a limit at 0 into a limit at infinity or the other way round. In all three cases, the alarm signal is the same: if after two rounds the expression is not simpler than at the start, L'Hôpital's rule is not the right tool.
Exercise 12: The pocket-sized expansion: reading the first neglected term in a limit
The linear approximation says that near 0, f(x)≈f(0)+f′(0)x. The next question is: by how much is it off? The answer lies in an indeterminate limit, because if limx→0xnf(x)−f(0)−f′(0)x=C with C nonzero, then the error is approximately Cxn.
Each of these limits produces one line of a small formula sheet that you will use all year.
a) Compute limx→0x2ex−1−x and write the approximation of ex that follows from it.
b) Compute limx→0x3sinx−x and conclude in the same way.
c) Compute limx→0x21+x−1−2x.
d) Compute limx→0x4cosx−1+2x2.
e) Estimate 1.04 with the linear approximation, then correct it with c). Compare with the exact value, 1.019804.
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Answers
a)21, so ex≈1+x+2x2
b)−61, so sinx≈x−6x3
c)−81
d)241
e)1.02 then 1.0198: the correction brings the error down from 2×10−4 to 4×10−6
a)
Form 00. Differentiate: 2xex−1, still 00; differentiate again: 2ex→21. The numerator is therefore approximately 2x2, hence ex≈1+x+2x2. The tangent line at 0 is y=1+x, and the curve moves away from it UPWARDS by about 2x2: the exponential is concave up.
b)
Form 00. Three differentiations: 3x2cosx−1, then 6x−sinx, then 6−cosx→−61. Therefore sinx≈x−6x3. The negative sign says that the sine lies BELOW its tangent line y=x for x>0, which you can see on the graph, and the cube says that the gap is tiny near 0: for x=0.1 rad, the error is only 1.7×10−4. That is why the approximation sinx≈x works so well in physics for small angles.
c)
Form 00. Differentiate: 2x21+x1−21, still 00; differentiate again: 2−41(1+x)−3/2→−81. Therefore 1+x≈1+2x−8x2. The square root is CONCAVE DOWN, it lies below its tangent line, hence the negative sign.
d)
Form 00. Four differentiations: 4x3−sinx+x, then 12x2−cosx+1, then 24xsinx, then 24cosx→241. Therefore cosx≈1−2x2+24x4. After the second differentiation, you could also conclude faster by recognizing x21−cosx→21, a known limit: the quotient was then 121×21=241. Recognizing a limit already established saves two rounds and two chances to get a sign wrong.
e)
Write 1.04=1+0.04. The linear approximation gives 1+20.04=1.02, an error of 1.02−1.019804=1.96×10−4. The correction from c) adds −80.042=−2.00×10−4, which gives 1.019800: the error drops to 4×10−6, FIFTY TIMES smaller. Notice in passing that the predicted correction, 2.00×10−4, reproduces the observed error, 1.96×10−4, almost exactly: that is the best proof that the coefficient −81 is right. A five-line formula sheet, built this way, replaces most of the limit computations of the course and gives the accuracy of each approximation as a bonus.
Exercise 13: The order of contact: how fast two curves pull apart
Two curves that touch at a point can pull apart more or less quickly. They are said to have CONTACT OF ORDER n at a when limx→a(x−a)nf(x)−g(x)=C with C finite and NONZERO.
The higher the order, the longer the curves stick together: the gap behaves like C(x−a)n, so it is divided by 2n when you come twice as close to the point.
a) Find the order of contact of y=sinx and its tangent line y=x at 0, as well as the constant C.
b) Do the same for y=ex and y=1+x.
c) Do the same for y=coshx and y=1+2x2.
d) Compute the three gaps at x=0.20 and rank them. Does the order predict the ranking?
e) How can you recognize the order of contact without computing any limit?
Show the solution
Answers
a)Order 3, C=−61
b)Order 2, C=21
c)Order 4, C=241
d)2.1×10−2, 1.3×10−3 and 6.7×10−5: yes
e)It is the order of the first successive derivatives that stop agreeing
a)
Test increasing powers. With n=1: xsinx−x→0, so C would be zero, which is excluded. With n=2: x2sinx−x→0 as well. With n=3: x3sinx−x→−61, finite and nonzero. The order of contact is therefore 3, with C=−61. The method is always the same: go up in powers until the limit stops being zero.
b)
xex−1−x→0, then x2ex−1−x→21: the order is 2 and C=21. It is the loosest contact of the three, and that is to be expected: the exponential is the only one of the three with no symmetry. The gap sinx−x is an odd function and the gap coshx−1−2x2 an even one, which wipes out every other power; the gap ex−1−x has no such help, and its term in x2 survives.
c)
x2coshx−1−2x2→0, x3coshx−1−2x2→0, and x4coshx−1−2x2→241. The order is 4 and C=241. It is the tightest contact of the three.
d)
At x=0.20: ∣e0.2−1.2∣=∣1.22140−1.2∣=2.14×10−2; ∣sin0.2−0.2∣=∣0.198669−0.2∣=1.33×10−3; ∣cosh0.2−1−0.02∣=∣1.020067−1.02∣=6.7×10−5. The ranking follows the order of contact exactly: the pair of order 2 is the furthest apart, the pair of order 4 the closest, with a factor of about sixteen, then about twenty, from one rung to the next. The predicted values confirm it: 21(0.2)2=2.0×10−2, 61(0.2)3=1.3×10−3 and 241(0.2)4=6.7×10−5.
e)
The order of contact is the FIRST ORDER OF DERIVATIVE at which the two functions stop agreeing at a. For sinx and x: same values at 0, same first derivatives (1 and 1), same second derivatives (0 and 0), but different third derivatives (−1 and 0): order 3. For ex and 1+x: the second derivatives are already 1 and 0: order 2. For coshx and 1+2x2: the third derivatives agree, sinh0=0 and 0, and only the fourth ones differ, cosh0=1 against 0: order 4. The constant follows as well: C=n!f(n)(a)−g(n)(a), which indeed gives −61, 21 and 241. Comparing successive derivatives therefore spares you any limit computation, and it is the fast way to handle this kind of question on the exam.
Exercise 14: Problem: the catenary and the parabola, how far do they look alike?
A flexible cable hanging between two points takes the shape of a CATENARY, yc(x)=acoshax−a, where a is a tension parameter, in metres. Engineers often replace it by the PARABOLA yp(x)=2ax2, which is much handier.
Take a=50.0 m, a common value for a power line, and measure x from the lowest point.
a) Check that both curves pass through the origin with the same tangent line and the same second derivative at 0.
b) Compute limx→0x4yc(x)−yp(x) in terms of a, then its numerical value.
c) What is the order of contact of the two curves at 0?
d) At what distance x from the lowest point does the gap reach 1.0 mm? Check with the exact formula.
e) What does the gap become at x=14.8 m, twice as far? State the engineering rule that follows.
Show the solution
Answers
a)Both are 0, with derivative 0 and second derivative a1
b)24a31, that is 3.33×10−7 m−3
c)Order 4
d)x=7.40 m; the exact formula gives 1.0003 mm
e)16 mm: the gap is multiplied by SIXTEEN when the distance doubles
a)
At 0: yc(0)=acosh0−a=a−a=0 and yp(0)=0. First derivatives: yc′(x)=sinhax, zero at 0, and yp′(x)=ax, zero as well: both curves have the same horizontal tangent line, as expected at the lowest point. Second derivatives: yc′′(x)=a1coshax, which equals a1 at 0, and yp′′=a1 everywhere: same curvature. The parameter a of the catenary is thus chosen precisely so that the parabola has the same curvature at the bottom.
b)
Let u=ax. Then yc−yp=a(coshu−1−2u2) and x4=a4u4, so the quotient equals a31⋅u4coshu−1−2u2, whose limit is 24a31 by exercise 13c. Numerically, 24×5031=3.00×1061=3.33×10−7 m−3.
c)
The limit is finite and nonzero for n=4, and it was zero for n=3: the order of contact is 4. In other words, the two curves share the position, the slope, the curvature AND the rate of change of the curvature at the bottom; they only part ways at the fourth order.
d)
The gap is approximately 24a3x4. Solve 3.00×106x4=1.0×10−3, that is x4=3.00×103 and x=43000=7.40 m. Check with the exact formula, with u=507.40=0.1480: 50(cosh0.1480−1−20.14802)=1.0003×10−3 m, that is 1.0003 mm. The approximation is excellent, to within three ten-thousandths.
e)
The gap varies as the FOURTH POWER of the distance: doubling x multiplies it by 24=16. At x=14.8 m, it is therefore 16 mm. The engineering rule that follows is this one: THE PARABOLA IS AN EXCELLENT APPROXIMATION AS LONG AS THE SPAN STAYS SMALL COMPARED WITH THE PARAMETER a, and it degrades very quickly beyond that. For a power line with a=50 m, the parabola holds to the millimetre over about fifteen metres of total span, to the centimetre over about twenty-six metres, and you need the exact catenary for a suspension bridge or a cable car. The order of contact is therefore not a curiosity: it tells you from which span on the simple model becomes wrong, and it is computed with a single indeterminate limit.
Exercise 15: Problem: from monthly compound interest to continuous interest
A principal P invested at the annual rate r, compounded n times a year, is worth after one year A=P(1+nr)n.
As compounding becomes more and more frequent, n tends to infinity and the base to 1: this is the indeterminate form 1∞.
Data: P=10,000 dollars and r=5.0% per year.
a) Compute the amount after one year with annual, monthly, then daily compounding, to the nearest cent.
b) Prove that limn→∞(1+nr)n=er.
c) Compute the amount with CONTINUOUS compounding, to the nearest cent.
d) How much more does continuous compounding earn than daily compounding? Comment.
e) Redo a) and c) for a rate of 50%. What do you conclude about how much the compounding frequency matters?
Show the solution
Answers
a)10,500.00; 10,511.62; 10,512.67 dollars
b)Through the logarithm: nln(1+nr)→r
c)10,512.71 dollars
d)4 cents: the race stops well before infinity
e)15,000 against 16,487.21 dollars: the frequency matters when the rate is large
a)
Annual, n=1: A=10,000×1.05=10,500.00 dollars. Monthly, n=12: A=10,000(1+120.05)12=10,000×1.0511619=10,511.62 dollars. Daily, n=365: A=10,000(1+3650.05)365=10,512.67 dollars. You can already see that the successive gains run out of steam: 11.62 dollars going from yearly to monthly, then 1.05 dollars going from monthly to daily.
b)
Set y=(1+nr)n, so lny=nln(1+nr), of the form ∞⋅0. Move a factor down by setting u=n1→0+: lny=uln(1+ru), of the form 00. Differentiate with respect to u: 11+rur=1+rur→r. Therefore lny→r and y→er. For r=1, you recognize the very definition of the number e. Without going through the logarithm, no direct computation is possible: this is the textbook case of the form 1∞.
10,512.71−10,512.67=0.04 dollars, that is FOUR CENTS on ten thousand dollars invested for one year. The comment matters as much as the number: the limit er is reached in practice well before infinity, and compounding every second rather than every day earns strictly nothing. The difference between two institutions is therefore never a matter of compounding frequency, but of the posted rate. This is also why financial institutions are required to disclose an EFFECTIVE ANNUAL RATE, which is precisely (1+nr)n−1: it makes offers comparable whatever their frequency.
e)
With r=0.50: annual compounding, 10,000×1.5=15,000 dollars; monthly, 10,000(1+120.5)12=16,320.94 dollars; continuous, 10,000e0.5=16,487.21 dollars. The gap between annual and continuous now reaches 1,487 dollars, nearly 10% of the amount from annual compounding, against barely 13 dollars for a rate of 5%. Conclusion: in the indeterminate form 1∞, everything depends on the DISTANCE from the base to 1. When nr is tiny, the limit is reached almost immediately; when it is not, the compounding frequency changes the result visibly. This is the financial translation of what exercise 5 said mathematically: a base that tends to 1 is not a base equal to 1, and the difference is paid in dollars.
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