L'Hôpital's Rule: Conditions, Forms and Examples

#Calculus
TL;DR
L'Hôpital's rule turns a 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} limit into the limit of f′(x)g′(x)\frac{f'(x)}{g'(x)}. This guide states the exact conditions, converts the other indeterminate forms and shows where the rule fails.
BT
Bhanzu TeamLast updated on October 11, 202614 min read

What Is L'Hôpital's Rule?

L'Hôpital's rule is a theorem that evaluates a limit of a quotient f(x)g(x)\frac{f(x)}{g(x)} that takes the indeterminate form 00\frac{0}{0} or ∞∞\frac{\infty}{\infty}, by replacing the quotient with f′(x)g′(x)\frac{f'(x)}{g'(x)}, the derivative of the top over the derivative of the bottom. If the new limit exists, the original limit has the same value. That is the whole answer to the Quora question "What is L'Hopital's Rule?", but the conditions matter as much as the formula.

Here is the precise statement. Let ff and gg be differentiable on an open interval II containing aa, except possibly at aa itself, and suppose g′(x)≠0g'(x) \neq 0 for every xx in II with x≠ax \neq a. Suppose also that either

lim⁡x→af(x)=0 and lim⁡x→ag(x)=0,orlim⁡x→a∣g(x)∣=∞.\lim_{x \to a} f(x) = 0 \text{ and } \lim_{x \to a} g(x) = 0, \quad \text{or} \quad \lim_{x \to a} |g(x)| = \infty.

If lim⁡x→af′(x)g′(x)=L\lim_{x \to a} \frac{f'(x)}{g'(x)} = L, where LL is a real number, ∞\infty or −∞-\infty, then

lim⁡x→af(x)g(x)=L.\lim_{x \to a} \frac{f(x)}{g(x)} = L.

  • f(x)f(x) and g(x)g(x) are the numerator and denominator, each a function you can differentiate near aa.

  • f′(x)f'(x) and g′(x)g'(x) are their derivatives, taken separately. This is not the quotient rule.

  • aa is the point being approached. The same statement holds for one-sided limits (x→a+x \to a^{+} or x→a−x \to a^{-}) and for x→∞x \to \infty or x→−∞x \to -\infty, with II replaced by an interval on that side.

  • LL is the value the derivative ratio approaches, and the conclusion only follows when that limit exists.

The forms 00\frac{0}{0} and ∞∞\frac{\infty}{\infty} are two of the seven indeterminate forms. The other five (such as 0⋅∞0 \cdot \infty and 1∞1^{\infty}) are rewritten into one of these two before the rule applies, as shown further down.

What Are The Exact Conditions For Using L'Hôpital's Rule?

You can use L'Hôpital's rule only when all four conditions hold. Two Quora questions, "When is L'Hôpital's rule not applicable?" and "Why can't L'Hôpital's rule be used for limits which aren't in indeterminate form?", come down to this checklist:

  1. The form is 00\frac{0}{0} or ∞∞\frac{\infty}{\infty}. Substitute first. Anything else is either already an answer or must be rewritten.

  2. Both functions are differentiable near aa (they need not be defined at aa).

  3. g′(x)≠0g'(x) \neq 0 near aa, except possibly at aa.

  4. The limit of f′(x)g′(x)\frac{f'(x)}{g'(x)} exists, as a number or as ±∞\pm\infty.

Condition 1 is the one people skip. A Physics Forums student asked "Why is 0/-2 not an indeterminate form?" after expecting to use the rule on lim⁡x→2ln⁡(x−1)x2−x−4\lim_{x \to 2} \frac{\ln(x - 1)}{x^2 - x - 4}. Substitution gives ln⁡1−2=0−2=0\frac{\ln 1}{-2} = \frac{0}{-2} = 0, a finished answer. A form like 0−2\frac{0}{-2} or 53\frac{5}{3} carries complete information, so differentiating changes the problem into a different one with a different answer.

Take lim⁡x→0cos⁡xx+1\lim_{x \to 0} \frac{\cos x}{x + 1}. Substitution gives 11=1\frac{1}{1} = 1. Differentiating top and bottom anyway gives lim⁡x→0−sin⁡x1=0\lim_{x \to 0} \frac{-\sin x}{1} = 0, which is wrong. The rule's proof uses the fact that ff and gg both start from zero (or both blow up); without that, the derivatives describe how fast each part changes, not what their ratio is.

How Do You Use L'Hôpital's Rule Step By Step?

The method is four steps, and the first one is not differentiating:

  1. Substitute. Confirm the limit really is 00\frac{0}{0} or ∞∞\frac{\infty}{\infty}.

  2. Differentiate the numerator and the denominator separately. Write f′(x)g′(x)\frac{f'(x)}{g'(x)}, using the derivative of a function rules for each part on its own.

  3. Simplify the new quotient if you can (cancel, combine, rewrite trig).

  4. Substitute again. A number or ±∞\pm\infty is the answer. If you get 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} again, return to step 2; if you get a different form, stop and rethink.

A short example shows the rhythm:

lim⁡x→0tan⁡3xx(00)\lim_{x \to 0} \frac{\tan 3x}{x} \quad \left(\frac{0}{0}\right)

=lim⁡x→03sec⁡23x1= \lim_{x \to 0} \frac{3\sec^2 3x}{1}

=3⋅1=3= 3 \cdot 1 = 3

Why Does L'Hôpital's Rule Work?

L'Hôpital's rule works because near a point where f(a)=g(a)=0f(a) = g(a) = 0, each function behaves like its tangent line, so the ratio of the functions behaves like the ratio of the tangent slopes. Physics Forums threads titled "How Does L'Hopital's Rule Intuitively Explain Limits?" and "Proof of the L'Hôpital Rule for the Indeterminate Form" ask for exactly these two levels: the picture and the proof.

The picture. If ff and gg are differentiable at aa with f(a)=g(a)=0f(a) = g(a) = 0, then for xx near aa:

f(x)≈f′(a)(x−a),g(x)≈g′(a)(x−a)f(x) \approx f'(a)(x - a), \qquad g(x) \approx g'(a)(x - a)

f(x)g(x)≈f′(a)(x−a)g′(a)(x−a)=f′(a)g′(a)\frac{f(x)}{g(x)} \approx \frac{f'(a)(x - a)}{g'(a)(x - a)} = \frac{f'(a)}{g'(a)}

The factor x−ax - a, which is the source of both zeros, cancels. Both graphs pass through the same point on the axis, and the rule compares how steeply they leave it.

The proof sketch. The full proof uses Cauchy's extension of the mean value theorem: if ff and gg are continuous on [a,x][a, x], differentiable on (a,x)(a, x), and g′≠0g' \neq 0 there, then some cc between aa and xx satisfies

f(x)−f(a)g(x)−g(a)=f′(c)g′(c).\frac{f(x) - f(a)}{g(x) - g(a)} = \frac{f'(c)}{g'(c)}.

That extension is proved by applying Rolle's theorem to h(t)=(f(x)−f(a))g(t)−(g(x)−g(a))f(t)h(t) = \big(f(x) - f(a)\big)g(t) - \big(g(x) - g(a)\big)f(t).

For the 00\frac{0}{0} case, set f(a)=g(a)=0f(a) = g(a) = 0, so the left side is just f(x)g(x)\frac{f(x)}{g(x)}. As x→a+x \to a^{+}, the point cc is squeezed toward aa, so f(x)g(x)=f′(c)g′(c)\frac{f(x)}{g(x)} = \frac{f'(c)}{g'(c)} approaches LL. The left-hand limit uses the same argument, mirrored. The ∞∞\frac{\infty}{\infty} case needs a longer argument with the same theorem, and the hypothesis g′≠0g' \neq 0 is exactly what keeps the denominator g(x)−g(a)g(x) - g(a) from being zero.

How Do You Handle The ∞/∞ Form?

You handle ∞∞\frac{\infty}{\infty} exactly like 00\frac{0}{0}: differentiate top and bottom separately and take the limit again. The form appears most often in limits at infinity, where it answers the question of which function grows faster.

lim⁡x→∞ln⁡xx=lim⁡x→∞1x12x=lim⁡x→∞2x=0\lim_{x \to \infty} \frac{\ln x}{\sqrt{x}} = \lim_{x \to \infty} \frac{\frac{1}{x}}{\frac{1}{2\sqrt{x}}} = \lim_{x \to \infty} \frac{2}{\sqrt{x}} = 0

Results like this build the growth ladder that the rule proves rung by rung. For large xx:

ln⁡x≪xp≪ex(p>0)\ln x \ll x^{p} \ll e^{x} \qquad (p > 0)

Each function on the left is eventually negligible compared with the one on its right, so the quotient (left over right) tends to 00. That single line explains why a logarithmic-time algorithm beats a polynomial one for large inputs, and why exponential growth overwhelms any power.

How Do You Convert The Other Indeterminate Forms?

You convert every other indeterminate form into 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} first, because L'Hôpital's rule applies only to quotients. The Physics Forums question "When to use e and ln in limits, applying L'Hôpital's rule twice?" is about the exponent forms in the last row below.

Form

Example

Rewrite

Then

0⋅∞0 \cdot \infty

xln⁡xx \ln x as x→0+x \to 0^{+}

ln⁡x1x\frac{\ln x}{\frac{1}{x}}

∞∞\frac{\infty}{\infty} type, apply the rule

∞−∞\infty - \infty

1x−1sin⁡x\frac{1}{x} - \frac{1}{\sin x} as x→0x \to 0

sin⁡x−xxsin⁡x\frac{\sin x - x}{x \sin x} (common denominator)

00\frac{0}{0}, apply the rule

1∞1^{\infty}, 000^{0}, ∞0\infty^{0}

(1+3x)x\left(1 + \frac{3}{x}\right)^{x}, xxx^{x}, x1xx^{\frac{1}{x}}

Let yy be the expression and take ln⁡y\ln y

ln⁡y\ln y is a 0⋅∞0 \cdot \infty product; find its limit MM, then y→eMy \to e^{M}

The logarithm step works because the natural logarithm turns a power into a product, ln⁡(uv)=vln⁡u\ln\left(u^{v}\right) = v \ln u, and because ete^{t} is continuous, so the limit can pass through it at the end. Two quick results from this row:

  • lim⁡x→0+xx=1\lim_{x \to 0^{+}} x^{x} = 1, because ln⁡y=xln⁡x→0\ln y = x \ln x \to 0.

  • lim⁡x→∞x1x=1\lim_{x \to \infty} x^{\frac{1}{x}} = 1, because ln⁡y=ln⁡xx→0\ln y = \frac{\ln x}{x} \to 0.

Can You Apply L'Hôpital's Rule More Than Once?

Yes. You can apply L'Hôpital's rule as many times as the result stays 00\frac{0}{0} or ∞∞\frac{\infty}{\infty}, but you must substitute and check the form before every round. For instance, lim⁡x→0x−sin⁡xx3\lim_{x \to 0} \frac{x - \sin x}{x^3} takes three rounds:

lim⁡x→0x−sin⁡xx3=lim⁡x→01−cos⁡x3x2=lim⁡x→0sin⁡x6x=lim⁡x→0cos⁡x6=16\lim_{x \to 0} \frac{x - \sin x}{x^3} = \lim_{x \to 0} \frac{1 - \cos x}{3x^2} = \lim_{x \to 0} \frac{\sin x}{6x} = \lim_{x \to 0} \frac{\cos x}{6} = \frac{1}{6}

Each of the first three quotients is 00\frac{0}{0}; the fourth is not, and that is where you stop. When a limit needs many rounds, a Taylor series usually gets there faster: x−sin⁡x=x36−⋯x - \sin x = \frac{x^3}{6} - \cdots, so the answer 16\frac{1}{6} is visible at once.

When Does L'Hôpital's Rule Fail Or Loop?

L'Hôpital's rule fails when its conditions break, and it loops when differentiating keeps reproducing the same shape. A Quora question asks "Can all limits be calculated using L'Hopital's Rule?" The answer is no, and these four situations are why:

  • The form is not indeterminate. The rule gives a wrong answer, as the cos⁡xx+1\frac{\cos x}{x + 1} example showed.

  • The derivative ratio has no limit. For lim⁡x→∞x+sin⁡xx\lim_{x \to \infty} \frac{x + \sin x}{x}, the rule gives 1+cos⁡x1\frac{1 + \cos x}{1}, which oscillates forever. The rule simply says nothing here. Algebra settles it: x+sin⁡xx=1+sin⁡xx→1\frac{x + \sin x}{x} = 1 + \frac{\sin x}{x} \to 1. A failed rule does not mean a missing limit.

  • The rule loops. For lim⁡x→∞x2+1x\lim_{x \to \infty} \frac{\sqrt{x^2 + 1}}{x}, one round gives xx2+1\frac{x}{\sqrt{x^2 + 1}} and the next gives back x2+1x\frac{\sqrt{x^2 + 1}}{x}. Dividing top and bottom by xx instead gives 1+1x2→1\sqrt{1 + \frac{1}{x^2}} \to 1. The same loop happens with ex−e−xex+e−x\frac{e^{x} - e^{-x}}{e^{x} + e^{-x}}, which algebra (divide by exe^{x}) sends to 11.

  • The reasoning would be circular. Using the rule on lim⁡x→0sin⁡xx\lim_{x \to 0} \frac{\sin x}{x} needs the derivative of sin⁡x\sin x, and that derivative is proved from this very limit. The standard limits are proved geometrically instead.

I'll admit the third case surprised me the first time: nothing in the statement warns that the rule can be technically valid and still useless. The hypotheses guarantee a correct answer when the new limit exists; they never promise the new limit is easier.

Examples Of L'Hôpital's Rule

Example 1

Evaluate lim⁡x→1ln⁡xx−1\lim_{x \to 1} \dfrac{\ln x}{x - 1}.

Substitution gives ln⁡10=00\frac{\ln 1}{0} = \frac{0}{0}. Differentiate top and bottom separately.

lim⁡x→11x1\lim_{x \to 1} \frac{\frac{1}{x}}{1}

=11=1= \frac{1}{1} = 1

Final answer: 11

Example 2

Evaluate lim⁡x→01−cos⁡xx2+x\lim_{x \to 0} \dfrac{1 - \cos x}{x^2 + x}.

Substitution gives 00\frac{0}{0}, so one round of the rule is allowed:

lim⁡x→0sin⁡x2x+1\lim_{x \to 0} \frac{\sin x}{2x + 1}

A common next move is to keep going, since the first round worked. Differentiate again:

lim⁡x→0cos⁡x2=12\lim_{x \to 0} \frac{\cos x}{2} = \frac{1}{2}

That answer is wrong. Check with a small input: at x=0.01x = 0.01 the original expression is 0.00005000.0101≈0.00495\frac{0.0000500}{0.0101} \approx 0.00495, nowhere near 12\frac{1}{2}. The second round was illegal because sin⁡x2x+1\frac{\sin x}{2x + 1} is not indeterminate at 00. Substitute instead of differentiating:

lim⁡x→0sin⁡x2x+1=01=0\lim_{x \to 0} \frac{\sin x}{2x + 1} = \frac{0}{1} = 0

Final answer: 00

Example 3

Evaluate lim⁡x→∞x2ex\lim_{x \to \infty} \dfrac{x^2}{e^{x}}.

This is ∞∞\frac{\infty}{\infty}. Apply the rule, check, and apply it again.

lim⁡x→∞2xex(∞∞)\lim_{x \to \infty} \frac{2x}{e^{x}} \quad \left(\frac{\infty}{\infty}\right)

=lim⁡x→∞2ex= \lim_{x \to \infty} \frac{2}{e^{x}}

=0= 0

Final answer: 00 (the exponential outgrows the square)

Example 4

Evaluate lim⁡x→0+xln⁡x\lim_{x \to 0^{+}} x \ln x.

This is 0⋅(−∞)0 \cdot (-\infty). Rewrite it as a quotient.

lim⁡x→0+ln⁡x1x(−∞∞)\lim_{x \to 0^{+}} \frac{\ln x}{\frac{1}{x}} \quad \left(\frac{-\infty}{\infty}\right)

=lim⁡x→0+1x−1x2= \lim_{x \to 0^{+}} \frac{\frac{1}{x}}{-\frac{1}{x^2}}

=lim⁡x→0+(−x)=0= \lim_{x \to 0^{+}} (-x) = 0

Final answer: 00

Example 5

Evaluate lim⁡x→0(1x−1sin⁡x)\lim_{x \to 0} \left(\dfrac{1}{x} - \dfrac{1}{\sin x}\right).

This is ∞−∞\infty - \infty. Combine over a common denominator, then apply the rule twice, checking the form each time.

lim⁡x→0sin⁡x−xxsin⁡x(00)\lim_{x \to 0} \frac{\sin x - x}{x \sin x} \quad \left(\frac{0}{0}\right)

=lim⁡x→0cos⁡x−1sin⁡x+xcos⁡x(00)= \lim_{x \to 0} \frac{\cos x - 1}{\sin x + x\cos x} \quad \left(\frac{0}{0}\right)

=lim⁡x→0−sin⁡x2cos⁡x−xsin⁡x= \lim_{x \to 0} \frac{-\sin x}{2\cos x - x\sin x}

=02=0= \frac{0}{2} = 0

Final answer: 00

Example 6

Evaluate lim⁡x→∞(1+3x)x\lim_{x \to \infty} \left(1 + \dfrac{3}{x}\right)^{x}.

This is 1∞1^{\infty}. Let y=(1+3x)xy = \left(1 + \frac{3}{x}\right)^{x} and take logarithms.

ln⁡y=xln⁡(1+3x)=ln⁡(1+3x)1x(00)\ln y = x \ln\left(1 + \frac{3}{x}\right) = \frac{\ln\left(1 + \frac{3}{x}\right)}{\frac{1}{x}} \quad \left(\frac{0}{0}\right)

lim⁡x→∞ln⁡y=lim⁡x→∞−3/x21+3/x−1x2\lim_{x \to \infty} \ln y = \lim_{x \to \infty} \frac{\frac{-3/x^2}{1 + 3/x}}{-\frac{1}{x^2}}

=lim⁡x→∞31+3x=3= \lim_{x \to \infty} \frac{3}{1 + \frac{3}{x}} = 3

lim⁡x→∞y=e3≈20.0855\lim_{x \to \infty} y = e^{3} \approx 20.0855

Final answer: e3e^{3}

Where Is L'Hôpital's Rule Used?

L'Hôpital's rule is used wherever a formula breaks at a special value or two quantities race to zero or infinity, which is why the Quora question "What is the significance of l'Hopital's Rule?" has a practical answer:

  • Comparing growth. Computer scientists compare running times such as nln⁡nn \ln n and n2n^2 by the limit of their ratio; the rule shows ln⁡nn→0\frac{\ln n}{n} \to 0, so n2n^2 eventually dominates.

  • Formulas with a removable break. Money deposited continuously at 1 unit per year for tt years, with continuous interest at rate rr, grows to ert−1r\frac{e^{rt} - 1}{r}. At r=0r = 0 the formula reads 00\frac{0}{0}; the rule (differentiating in rr) gives lim⁡r→0tert=t\lim_{r \to 0} t e^{rt} = t, which is exactly what deposits with no interest should give.

  • Continuous compounding. The 1∞1^{\infty} limit lim⁡n→∞(1+rn)n=er\lim_{n \to \infty} \left(1 + \frac{r}{n}\right)^{n} = e^{r} is Example 6 with rr in place of 33. At r=5r = 5% it gives a growth factor of e0.05≈1.0513e^{0.05} \approx 1.0513 per year.

  • Derivatives of new functions. Proving limits such as lim⁡x→0ex−1x=1\lim_{x \to 0} \frac{e^{x} - 1}{x} = 1 for a function already known to be differentiable is one line with the rule.

Where Solutions Go Off The Rails

Most marks lost on this topic come from using the rule mechanically: differentiating the wrong thing, at the wrong time, or forgetting what the answer was a limit of.

Mistake 1: Using The Quotient Rule Instead

Where it slips in: The first round, when the expression is a fraction and "derivative of a fraction" triggers a reflex.

Don't do this: Apply the quotient rule to f(x)g(x)\frac{f(x)}{g(x)}. That computes the derivative of the quotient, a different object.

The correct way: Differentiate the numerator alone and the denominator alone, then form f′(x)g′(x)\frac{f'(x)}{g'(x)}. The rusher who sees a fraction and writes f′g−fg′g2\frac{f'g - fg'}{g^2} has done correct calculus on the wrong problem.

Mistake 2: Skipping The Check Between Rounds

Where it slips in: After one successful round, as in Example 2.

Don't do this: Differentiate again without substituting first.

The correct way: Substitute after every round and continue only on 00\frac{0}{0} or ∞∞\frac{\infty}{\infty}. The check between rounds looks skippable, and it is exactly the step that separates 00 from the wrong 12\frac{1}{2} in Example 2.

Mistake 3: Forgetting To Undo The Logarithm

Where it slips in: Exponent forms such as 1∞1^{\infty} and 000^{0}.

Don't do this: Report the limit of ln⁡y\ln y (the 33 in Example 6) as the answer.

The correct way: Finish with y→eMy \to e^{M}, so Example 6 gives e3e^{3}, not 33. The memorizer who learned "take logs, then use the rule" without the reason tends to stop one line early; writing "let y=…y = \ldots" on the first line makes the final step impossible to forget.

Mistake 4: Reading A Failed Rule As A Missing Limit

Where it slips in: Limits like x+sin⁡xx\frac{x + \sin x}{x}, where f′(x)g′(x)\frac{f'(x)}{g'(x)} oscillates.

Don't do this: Conclude "the limit does not exist" because the derivative ratio has no limit.

The correct way: Go back to algebra. The rule is one-directional: when the new limit exists, it gives the answer; when it does not, the rule is silent.

Practice Problems On L'Hôpital's Rule

  1. Evaluate lim⁡x→0e2x−1x\lim_{x \to 0} \dfrac{e^{2x} - 1}{x}.

  2. Evaluate lim⁡x→0x−sin⁡xx3\lim_{x \to 0} \dfrac{x - \sin x}{x^3} without looking back at the repeated-use section.

  3. Evaluate lim⁡x→∞ln⁡xx\lim_{x \to \infty} \dfrac{\ln x}{x}.

  4. Evaluate lim⁡x→0+x2ln⁡x\lim_{x \to 0^{+}} x^2 \ln x.

  5. Evaluate lim⁡x→0+(1x−1ex−1)\lim_{x \to 0^{+}} \left(\dfrac{1}{x} - \dfrac{1}{e^{x} - 1}\right).

  6. Evaluate lim⁡x→0+(1+sin⁡x)1x\lim_{x \to 0^{+}} \left(1 + \sin x\right)^{\frac{1}{x}}.

Answer to Question 1: 22 (one round gives 2e2x2e^{2x} over 11).

Answer to Question 2: 16\frac{1}{6} (three rounds).

Answer to Question 3: 00 (one round gives 1x\frac{1}{x}).

Answer to Question 4: 00 (rewrite as ln⁡xx−2\frac{\ln x}{x^{-2}}; one round gives −x22-\frac{x^2}{2}).

Answer to Question 5: 12\frac{1}{2} (common denominator, then two rounds).

Answer to Question 6: ee (take logs: ln⁡(1+sin⁡x)x→1\frac{\ln(1 + \sin x)}{x} \to 1).

The Short Version

  • L'Hôpital's rule replaces a 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} limit of f(x)g(x)\frac{f(x)}{g(x)} with the limit of f′(x)g′(x)\frac{f'(x)}{g'(x)}, when that limit exists.

  • Substitute before every round, and differentiate the top and bottom separately, never with the quotient rule.

  • Convert 0⋅∞0 \cdot \infty, ∞−∞\infty - \infty and the exponent forms into a quotient first, and exponentiate back at the end.

  • When the derivative ratio oscillates or loops, the rule is silent and algebra or series take over.

  • Johann Bernoulli found the rule in 1694, and l'Hôpital published it in 1696.

A Practical Next Step

Work through Practice Problems 1 to 6. If Problem 5 trips you up, return to Example 5 and combine the fractions before differentiating; if Problem 6 does, reread Mistake 3 and finish with eMe^{M}.

Want a teacher to check your rounds with you? Book a free demo class with a Bhanzu trainer.

Read More

Was this article helpful?

Your feedback helps us write better content

Frequently Asked Questions

How do you pronounce L'Hôpital's rule, and why is it also spelled L'Hospital?
Say "lo-pee-TAHL". In the 17th and 18th centuries the name was spelled l'Hospital, and l'Hôpital wrote it that way himself; modern French replaced the silent s with a circumflex over the o, so both spellings refer to the same rule.
Can you simplify before applying L'Hôpital's rule?
Yes, and you usually should. Cancelling a common factor, pulling out a factor that has a nonzero limit, or rewriting trig often makes the derivatives much shorter. Simplifying between rounds is also allowed.
Is 0∞0^{\infty} an indeterminate form?
No. A positive base approaching 00 raised to a power growing without bound goes to 00, so the form has a definite value and needs no rule.
How do you find lim⁡x→0+(1x)tan⁡x\lim_{x \to 0^{+}} \left(\frac{1}{x}\right)^{\tan x}?
It is ∞0\infty^{0}. Let yy be the expression, so ln⁡y=−tan⁡xln⁡x=−ln⁡xcot⁡x\ln y = -\tan x \ln x = \frac{-\ln x}{\cot x}, an ∞∞\frac{\infty}{\infty} form. One round gives −1x−csc⁡2x=sin⁡2xx→0\frac{-\frac{1}{x}}{-\csc^2 x} = \frac{\sin^2 x}{x} \to 0. So ln⁡y→0\ln y \to 0 and the limit is e0=1e^{0} = 1.
How does L'Hôpital's rule connect to the second derivative?
Apply it in hh to f(x+h)−2f(x)+f(x−h)h2\frac{f(x + h) - 2f(x) + f(x - h)}{h^2}, which is 00\frac{0}{0} as h→0h \to 0. Two rounds give f′′(x+h)+f′′(x−h)2\frac{f''(x + h) + f''(x - h)}{2}, so if f′′f'' is continuous near xx, the limit is f′′(x)f''(x). That is the formula numerical methods use to estimate a second derivative from three function values.
Why does the rule need g′(x)≠0g'(x) \neq 0 near the point?
Because the proof divides by g′(c)g'(c) for points cc arbitrarily close to aa. When g′g' has zeros piling up near aa, there are known counterexamples where f′(x)g′(x)\frac{f'(x)}{g'(x)} has a limit but f(x)g(x)\frac{f(x)}{g(x)} does not.
✍️ Written By
BT
Bhanzu Team
Content Creator and Editor
Bhanzu’s editorial team, known as Team Bhanzu, is made up of experienced educators, curriculum experts, content strategists, and fact-checkers dedicated to making math simple and engaging for learners worldwide. Every article and resource is carefully researched, thoughtfully structured, and rigorously reviewed to ensure accuracy, clarity, and real-world relevance. We understand that building strong math foundations can raise questions for students and parents alike. That’s why Team Bhanzu focuses on delivering practical insights, concept-driven explanations, and trustworthy guidance-empowering learners to develop confidence, speed, and a lifelong love for mathematics.
Related Articles
Book a FREE Demo ClassBook Now →