Higher-Order Derivatives: Notation, Patterns, Examples

#Calculus
TL;DR
Higher-order derivatives are what you get by differentiating again and again: f′′f'', f′′′f''', up to f(n)f^{(n)}. This guide covers the notation, the nth-derivative patterns, their meaning in motion, and six worked examples.
BT
Bhanzu TeamLast updated on October 9, 202615 min read

What Are Higher-Order Derivatives?

Higher-order derivatives are the derivatives you get by differentiating a function more than once: the second derivative is the derivative of the first, the third is the derivative of the second, and so on. Each one measures how the previous one changes. The first derivative is order 1, the next is order 2, and the nth derivative is order nn.

Formally, start from a function ff with first derivative f′f', the ordinary derivative of a function. For each whole number n≥2n \geq 2, the nth derivative is defined step by step:

f(n)(x)=ddx[f(n−1)(x)]f^{(n)}(x) = \frac{d}{dx}\left[f^{(n-1)}(x)\right]

The nth derivative exists at xx only when f(n−1)f^{(n-1)} exists near xx and is itself differentiable at xx. Order 0 is the function itself, so f(0)=ff^{(0)} = f. The order-2 case has its own page on the second derivative; this page is about the whole ladder, order 3 and beyond included.

How Do You Write Higher-Order Derivatives?

You write higher-order derivatives with primes for low orders and a bracketed number for high orders. Four notations are in common use:

Notation

Second

Third

nth

Where you see it

Prime (Lagrange)

f′′(x)f''(x)

f′′′(x)f'''(x)

f(n)(x)f^{(n)}(x)

School and university calculus

Leibniz

d2ydx2\frac{d^2y}{dx^2}

d3ydx3\frac{d^3y}{dx^3}

dnydxn\frac{d^ny}{dx^n}

Physics, differential equations

Dot (Newton)

s¨\ddot{s}

s⋯\overset{\cdots}{s}

rarely used

Time derivatives in mechanics

Operator

D2fD^2 f

D3fD^3 f

DnfD^n f

Differential equations

Two details trip people up. In the Leibniz form, the 2 sits on the dd in the numerator but on the xx in the denominator, because the expression means "apply ddx\frac{d}{dx} twice" and the bottom records dxdx used twice. And the brackets in f(4)f^{(4)} are not decoration: f4(x)f^{4}(x) usually means [f(x)]4\left[f(x)\right]^4, a power.

This article uses the prime and bracket form throughout: f′′f'', f′′′f''', then f(4)f^{(4)}, f(5)f^{(5)} and f(n)f^{(n)}.

How Do You Find Higher-Order Derivatives?

You find a higher-order derivative by differentiating, simplifying, and differentiating again, as many times as the order asks. There is no new rule to learn; the power rule, the chain rule and the product rule are simply applied repeatedly.

  1. Find f′f' with the usual rules.

  2. Simplify f′f' fully. Expand, cancel and collect terms before you differentiate again.

  3. Differentiate the simplified result to get f′′f'', then repeat.

  4. Look for a pattern after three or four rounds, if the question asks for f(n)f^{(n)}.

Step 2 decides how long the work takes. Differentiating an unsimplified f′f' multiplies the number of terms at every round.

How Do You Find The Second Derivative Of Parametric Equations?

For a curve given by x=x(t)x = x(t) and y=y(t)y = y(t), as in parametric equations, the first derivative is dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}. The second derivative differentiates that result with respect to tt, then divides by dxdt\frac{dx}{dt} again:

d2ydx2=ddt(dydx)dxdt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}}

For x=t2x = t^2 and y=t3y = t^3 with t≠0t \neq 0:

dydx=3t22t=3t2\frac{dy}{dx} = \frac{3t^2}{2t} = \frac{3t}{2}

d2ydx2=322t=34t\frac{d^2y}{dx^2} = \frac{\frac{3}{2}}{2t} = \frac{3}{4t}

How Do You Find Higher Derivatives Of Implicit Equations?

When yy is defined by an equation such as x2+y2=25x^2 + y^2 = 25, use implicit differentiation for y′y', then differentiate y′y' again, remembering that yy is still a function of xx. Substituting y′y' back in tidies the answer, and Example 6 below works through it.

What Patterns Do The Nth Derivatives Follow?

Many common functions produce a clean formula for the nth derivative, because their derivatives repeat, scale or shrink in a predictable way. Spotting the pattern after three or four rounds turns a 50th-derivative question into a one-line answer.

Function

nth derivative f(n)(x)f^{(n)}(x)

Why the pattern holds

eaxe^{ax}

aneaxa^n e^{ax}

Each round multiplies by aa

axa^x (with a>0a > 0)

(ln⁡a)n,ax(\ln a)^n,a^x

Each round multiplies by ln⁡a\ln a

sin⁡x\sin x

sin⁡(x+nπ2)\sin\left(x + \frac{n\pi}{2}\right)

Each round shifts the wave a quarter period

cos⁡x\cos x

cos⁡(x+nπ2)\cos\left(x + \frac{n\pi}{2}\right)

Same quarter-period shift

sin⁡(ax)\sin(ax)

ansin⁡(ax+nπ2)a^n\sin\left(ax + \frac{n\pi}{2}\right)

Shift plus a factor of aa from the chain rule

1x\frac{1}{x}

(−1)n,1⋅2⋅3⋯nxn+1(-1)^n,\frac{1\cdot 2\cdot 3\cdots n}{x^{n+1}}

The power drops and the sign flips each round

ln⁡x\ln x

(−1)n−1,1⋅2⋯(n−1)xn(-1)^{n-1},\frac{1\cdot 2\cdots (n-1)}{x^n} for n≥1n \geq 1

After one round it becomes 1x\frac{1}{x}

xmx^m, mm a whole number

00 once n>mn > m

Each round lowers the degree by 1

The numerator 1⋅2⋅3⋯n1\cdot 2\cdot 3\cdots n in the 1x\frac{1}{x} row is nn factorial: 11, 22, 66, 2424, 120120 for n=1n = 1 to 55.

Two patterns deserve a closer look:

  • The sine cycle has length 4. The derivatives of sin⁡x\sin x run cos⁡x\cos x, −sin⁡x-\sin x, −cos⁡x-\cos x, sin⁡x\sin x, then repeat. So for any order, divide nn by 4 and read the remainder: remainder 1 gives cos⁡x\cos x, remainder 2 gives −sin⁡x-\sin x, remainder 3 gives −cos⁡x-\cos x, remainder 0 gives sin⁡x\sin x.

  • Polynomials run out. A polynomial of degree mm has a constant mth derivative and a zero derivative from order m+1m + 1 on. For x6x^6, f(4)(x)=360x2f^{(4)}(x) = 360x^2 and f(7)(x)=0f^{(7)}(x) = 0.

What About The Nth Derivative Of A Product?

A product such as x2exx^2 e^x has its own pattern, given by the general Leibniz rule. It extends the product rule to order nn with binomial coefficients:

(fg)(n)=∑k=0n(nk)f(n−k),g(k)(fg)^{(n)} = \sum_{k=0}^{n} \binom{n}{k} f^{(n-k)},g^{(k)}

For order 2 that reads (fg)′′=f′′g+2f′g′+fg′′(fg)'' = f''g + 2f'g' + fg''. The full rule, with its proof by induction, is a topic of its own.

What Do Derivatives Above Order Two Tell You?

Derivatives above order two describe how the shape of a graph is changing, and together they fix the function near a point. A Quora thread asks exactly this: what information do derivatives above order two give? The answer comes in three layers.

  • Order 2 is shape. The sign of f′′f'' says whether the graph bends upward or downward, which is how the second derivative test separates a minimum from a maximum.

  • Order 3 is change of shape. f′′′f''' measures how fast the bending itself changes. Where f′′f'' crosses zero and f′′′≠0f''' \neq 0, the graph switches its direction of bending.

  • All orders together are the function. For many functions, the values f(a)f(a), f′(a)f'(a), f′′(a)f''(a), f′′′(a)f'''(a) and onward rebuild ff near aa through the Taylor series, whose coefficient on (x−a)n(x - a)^n is f(n)(a)f^{(n)}(a) divided by nn factorial.

Higher derivatives get harder to picture one by one, and that is honest: almost nobody "sees" a fifth derivative on a graph. Their meaning shows up collectively, in how well a polynomial can copy the function.

What Do Higher-Order Derivatives Mean In Motion?

In motion, higher-order derivatives of position are named one by one. A Quora thread asks how to explain jerk and snap with applications, and the ladder below is the short answer:

Order

Name

Meaning

Units (SI)

0

Position s(t)s(t)

Where the object is

m\text{m}

1

Velocity s′(t)s'(t)

How fast position changes

m/s\text{m/s}

2

Acceleration s′′(t)s''(t)

How fast velocity changes

m/s2\text{m/s}^2

3

Jerk s′′′(t)s'''(t)

How fast acceleration changes

m/s3\text{m/s}^3

4

Snap s(4)(t)s^{(4)}(t)

How fast jerk changes

m/s4\text{m/s}^4

Velocity and acceleration are covered in depth on the velocity and acceleration page. Jerk matters because the body senses a change in force more sharply than a steady force: constant acceleration in a smooth car feels calm, while a sudden change in acceleration feels like a jolt. Snap, also called jounce, appears in the design of smooth motion paths for machines and cameras.

Examples Of Higher-Order Derivatives

These six examples move from a polynomial to an implicit curve.

Example 1

Find f′′′(x)f'''(x), f(4)(x)f^{(4)}(x) and f(5)(x)f^{(5)}(x) for f(x)=2x4−5x3+x−7f(x) = 2x^4 - 5x^3 + x - 7, and evaluate f′′′(1)f'''(1).

f′(x)=8x3−15x2+1f'(x) = 8x^3 - 15x^2 + 1

f′′(x)=24x2−30xf''(x) = 24x^2 - 30x

f′′′(x)=48x−30f'''(x) = 48x - 30

f(4)(x)=48f^{(4)}(x) = 48

f(5)(x)=0f^{(5)}(x) = 0

f′′′(1)=48−30=18f'''(1) = 48 - 30 = 18

Final answer: f′′′(x)=48x−30f'''(x) = 48x - 30, f(4)(x)=48f^{(4)}(x) = 48, f(5)(x)=0f^{(5)}(x) = 0, and f′′′(1)=18f'''(1) = 18.

Example 2

Find f′′(x)f''(x) for f(x)=sin⁡(3x)f(x) = \sin(3x) and show that f′′+9f=0f'' + 9f = 0.

f′(x)=3cos⁡(3x)f'(x) = 3\cos(3x)

f′′(x)=−9sin⁡(3x)f''(x) = -9\sin(3x)

f′′(x)+9f(x)=−9sin⁡(3x)+9sin⁡(3x)=0f''(x) + 9f(x) = -9\sin(3x) + 9\sin(3x) = 0

The chain rule contributes a factor of 3 at each round, so two rounds give 32=93^2 = 9.

Final answer: f′′(x)=−9sin⁡(3x)f''(x) = -9\sin(3x), and f′′+9f=0f'' + 9f = 0 holds for every xx.

Example 3

Find the second derivative of f(x)=x2exf(x) = x^2 e^x.

The tempting shortcut treats the product one factor at a time and multiplies the second derivatives:

(x2)′′⋅(ex)′′=2⋅ex=2ex(x^2)'' \cdot (e^x)'' = 2 \cdot e^x = 2e^x

Test that shortcut on a product whose answer is known: x⋅x=x2x \cdot x = x^2, whose second derivative is 22. The shortcut gives (x)′′⋅(x)′′=0⋅0=0(x)'' \cdot (x)'' = 0 \cdot 0 = 0, so it fails. Products need the product rule at every round.

First round:

f′(x)=2x,ex+x2ex=(x2+2x)exf'(x) = 2x,e^x + x^2 e^x = \left(x^2 + 2x\right)e^x

Second round, applying the product rule to (x2+2x)ex\left(x^2 + 2x\right)e^x:

f′′(x)=(2x+2)ex+(x2+2x)exf''(x) = (2x + 2)e^x + \left(x^2 + 2x\right)e^x

f′′(x)=(x2+4x+2)exf''(x) = \left(x^2 + 4x + 2\right)e^x

At x=1x = 1 the correct value is 7e≈19.037e \approx 19.03, while the shortcut gives 2e≈5.442e \approx 5.44.

Final answer: f′′(x)=(x2+4x+2)exf''(x) = \left(x^2 + 4x + 2\right)e^x.

Example 4

Find a formula for the nth derivative of f(x)=1xf(x) = \frac{1}{x}, then evaluate f(5)(1)f^{(5)}(1).

Write f(x)=x−1f(x) = x^{-1} and differentiate four times:

f′(x)=−x−2f'(x) = -x^{-2}

f′′(x)=2x−3f''(x) = 2x^{-3}

f′′′(x)=−6x−4f'''(x) = -6x^{-4}

f(4)(x)=24x−5f^{(4)}(x) = 24x^{-5}

The signs alternate, the power of xx is −(n+1)-(n + 1), and the coefficients 1,2,6,241, 2, 6, 24 are 11, 1⋅21\cdot 2, 1⋅2⋅31\cdot 2\cdot 3, 1⋅2⋅3⋅41\cdot 2\cdot 3\cdot 4. So

f(n)(x)=(−1)n,1⋅2⋅3⋯nxn+1f^{(n)}(x) = (-1)^n,\frac{1\cdot 2\cdot 3\cdots n}{x^{n+1}}

f(5)(1)=(−1)5⋅120=−120f^{(5)}(1) = (-1)^5 \cdot 120 = -120

The common first instinct is to stop at f′′f'' and guess; writing out four rounds before naming the pattern is what keeps the sign and the power from drifting.

Final answer: f(n)(x)=(−1)n,1⋅2⋯nxn+1f^{(n)}(x) = (-1)^n,\frac{1\cdot 2\cdots n}{x^{n+1}}, and f(5)(1)=−120f^{(5)}(1) = -120.

Example 5

A particle moves along a line with position s(t)=t3−6t2+9ts(t) = t^3 - 6t^2 + 9t metres at time tt seconds. Find its velocity, acceleration and jerk. When is it at rest, and when is its acceleration zero?

v(t)=s′(t)=3t2−12t+9v(t) = s'(t) = 3t^2 - 12t + 9

a(t)=s′′(t)=6t−12a(t) = s''(t) = 6t - 12

j(t)=s′′′(t)=6j(t) = s'''(t) = 6

At rest means v(t)=0v(t) = 0:

3(t2−4t+3)=3(t−1)(t−3)=03\left(t^2 - 4t + 3\right) = 3(t - 1)(t - 3) = 0

So t=1t = 1 and t=3t = 3. Acceleration is zero when 6t−12=06t - 12 = 0, at t=2t = 2.

Final answer: v=3t2−12t+9,m/sv = 3t^2 - 12t + 9,\text{m/s}, a=6t−12,m/s2a = 6t - 12,\text{m/s}^2, jerk =6,m/s3= 6,\text{m/s}^3 (constant). The particle is at rest at t=1t = 1 and t=3t = 3 seconds, and its acceleration is zero at t=2t = 2 seconds.

Example 6

For the circle x2+y2=25x^2 + y^2 = 25, find y′′y'' in terms of yy and evaluate it at (3,4)(3, 4).

Differentiate implicitly:

2x+2y,y′=02x + 2y,y' = 0

y′=−xyy' = -\frac{x}{y}

Differentiate y′y' with the quotient rule, keeping in mind that yy depends on xx:

y′′=−y−x,y′y2y'' = -\frac{y - x,y'}{y^2}

Substitute y′=−xyy' = -\frac{x}{y}:

y′′=−y+x2yy2=−x2+y2y3y'' = -\frac{y + \frac{x^2}{y}}{y^2} = -\frac{x^2 + y^2}{y^3}

y′′=−25y3y'' = -\frac{25}{y^3}

At (3,4)(3, 4):

y′′=−2564y'' = -\frac{25}{64}

Final answer: y′′=−25y3y'' = -\frac{25}{y^3}, which is −2564-\frac{25}{64} at (3,4)(3, 4). The negative value fits the picture: the upper half of the circle bends downward.

Why Do We Need A Derivative Of A Derivative?

Higher-order derivatives exist because "force changes velocity, and velocity changes position", so the laws of motion are written one derivative deeper than speed. Newton's Principia of 1687 tied force to change in motion, and in modern form that is force equals mass times acceleration, a second derivative of position. Once one law of nature needed a second derivative, the whole ladder followed:

  • Motion. Isaac Newton built his method of fluxions in 1665 to 1667, and his laws of motion use the rate of change of a rate of change. Every differential equation in mechanics carries a second derivative for this reason.

  • Shape. Curve sketching needs to know not only whether a graph rises but whether it bends up or down, and where that bending changes.

  • Approximation. Polynomials built from the higher-order derivatives at a single point can approximate sin⁡x\sin x and exe^x to any accuracy you need near that point, and each extra derivative buys more accuracy.

Higher derivatives are not a new idea stacked on calculus. They are the first derivative used again, with each round answering a sharper question.

The Mathematicians Behind Higher-Order Derivatives

Isaac Newton (1643 to 1727, England) developed his method of fluxions during 1665 to 1667, while his university was closed by the plague. His dot notation for rates of change, with one dot per order, is still how physicists write time derivatives such as s¨\ddot{s} for acceleration.

Gottfried Wilhelm Leibniz (1646 to 1716, Germany) published his dd notation for differentials in Acta Eruditorum in 1684. That notation extends naturally to d2ydx2\frac{d^2y}{dx^2} and dnydxn\frac{d^ny}{dx^n}, which is why it dominates in physics and differential equations.

When Do Higher-Order Derivatives Matter In Real Life?

A Quora thread asks when higher-order derivatives actually matter in physics; the honest answer is "whenever smoothness or accuracy matters", which is more often than textbooks suggest:

  • Rides and lifts. Designers limit jerk, the third derivative of position, so that lifts start and stop gently and roller-coaster tracks ease into loops.

  • Economics. The second derivative of cost shows whether marginal cost and marginal revenue are rising or falling, which tells a firm whether producing one more unit is getting cheaper or dearer.

  • Engineering. The Euler-Bernoulli beam equation, EI,d4wdx4=q(x)EI,\frac{d^4w}{dx^4} = q(x), links the load on a beam to the fourth derivative of its deflection ww.

  • Machines and robots. Motion planners keep jerk and snap small so that arms and camera rigs move without vibration.

  • Numerical methods. Error bounds for approximations are written in terms of a higher derivative, so knowing f(n)f^{(n)} tells you how far an estimate can be trusted.

The Easy-To-Make Errors (And How To Catch Them)

Higher-order work fails in a small number of ways, and almost all of them come from one round being done carelessly.

Mistake 1: Confusing A Fourth Power With A Fourth Derivative

Where it slips in:

Notation questions and any problem that writes f(4)f^{(4)}.

Don't do this:

Treating f4(x)f^{4}(x) and f(4)(x)f^{(4)}(x) as the same thing.

The correct way:

Brackets mean order of differentiation; no brackets usually means a power. sin⁡2x\sin^2 x is (sin⁡x)2(\sin x)^2, while the second derivative of sin⁡x\sin x is −sin⁡x-\sin x.

Mistake 2: Dividing Second Derivatives In Parametric Form

Where it slips in:

Second derivatives of curves given by x(t)x(t) and y(t)y(t).

Don't do this:

Writing d2ydx2=d2y/dt2d2x/dt2\frac{d^2y}{dx^2} = \frac{d^2y/dt^2}{d^2x/dt^2}. For x=t2x = t^2, y=t3y = t^3 this gives 6t2=3t\frac{6t}{2} = 3t.

The correct way:

Differentiate dydx\frac{dy}{dx} with respect to tt, then divide by dxdt\frac{dx}{dt}, which gives 34t\frac{3}{4t}. The memorizer who learned "divide the derivatives" for the first derivative applies the same move one level up, where it no longer holds.

Mistake 3: Losing The Chain-Rule Factor At Each Round

Where it slips in:

nth derivatives of eaxe^{ax}, sin⁡(ax)\sin(ax) and 1ax+b\frac{1}{ax + b}.

Don't do this:

Writing the tenth derivative of e−2xe^{-2x} as e−2xe^{-2x} or −2e−2x-2e^{-2x}.

The correct way:

Each round contributes a factor of −2-2, so ten rounds give (−2)10=1024(-2)^{10} = 1024, and the answer is 1024,e−2x1024,e^{-2x}. The rusher who writes only the final round misses factors exactly like this; counting the factors round by round fixes it. Students who first write (−2)n(-2)^n in the general formula and only then substitute n=10n = 10 rarely lose the sign.

Mistake 4: Assuming Derivatives Past The Second Carry No Information

Where it slips in:

Motion and design questions that mention comfort, smoothness or vibration.

Don't do this:

Stopping at acceleration because "the third derivative never matters".

The correct way:

Check whether the question is about how acceleration changes; if it is, the third derivative is the quantity being asked for. The silent understander who can compute s′′′s''' but has never been asked what it means usually stumbles here.

Mistake 4 has a real engineering version. A track that joined a straight run directly onto a circular loop would make the rider's sideways acceleration jump the instant the loop began, which is a jerk spike. Roller-coaster and railway designers use transition curves to limit jerk; the Euler spiral is the standard example, raising the curvature steadily so that the acceleration builds at a constant rate and the jerk stays constant.

Practice Problems On Higher-Order Derivatives

Work each problem, then compare with the answers below. Every answer has been recomputed.

  1. Find f′′′(x)f'''(x) for f(x)=x5−4x3f(x) = x^5 - 4x^3.

  2. Find f′′(x)f''(x) for f(x)=xln⁡xf(x) = x\ln x, with x>0x > 0.

  3. Find the third derivative of f(x)=xf(x) = \sqrt{x}.

  4. Find the tenth derivative of e−2xe^{-2x}.

  5. Find the 25th derivative of cos⁡x\cos x.

  6. Find f′′′(x)f'''(x) for f(x)=12x+1f(x) = \frac{1}{2x + 1}.

Answer to Question 1: f′′′(x)=60x2−24f'''(x) = 60x^2 - 24.

Answer to Question 2: f′′(x)=1xf''(x) = \frac{1}{x}.

Answer to Question 3: f′′′(x)=38x5/2f'''(x) = \frac{3}{8x^{5/2}}.

Answer to Question 4: 1024,e−2x1024,e^{-2x}.

Answer to Question 5: −sin⁡x-\sin x (25 leaves remainder 1 on division by 4, and the cycle for cosine starts −sin⁡x-\sin x).

Answer to Question 6: f′′′(x)=−48(2x+1)4f'''(x) = -\frac{48}{(2x + 1)^4}.

Key Takeaways

  • Higher-order derivatives come from differentiating repeatedly, with f(n)f^{(n)} defined as the derivative of f(n−1)f^{(n-1)}.

  • Brackets matter: f(4)f^{(4)} is a fourth derivative, while f4f^4 is a fourth power.

  • Exponentials scale, sines cycle every four steps, 1x\frac{1}{x} alternates in sign, and polynomials reach zero.

  • In motion, the ladder runs position, velocity, acceleration, jerk and snap.

  • Products need the product rule at every round, never a product of second derivatives.

Where To Go From Here

Work through Practice Problems 1 to 6; if Problem 4 or 5 trips you up, return to the table of nth-derivative patterns, and if Problem 6 does, reread Mistake 3 on chain-rule factors.

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Frequently Asked Questions

When do college math courses start talking about higher-order derivatives, such as third order and higher?
Usually in the first calculus course, right after the basic differentiation rules, where the second and third derivatives appear in motion and curve-sketching problems. Derivatives of every order return later with Taylor series and with differential equations.
What is meant by "terms of higher order" when calculating derivatives in motion?
It means terms with a higher power of a small quantity, such as (Δt)2(\Delta t)^2 or (Δt)3(\Delta t)^3. When Δt\Delta t is tiny, those terms shrink much faster than the first-order term, so they drop out in the limit that defines the derivative.
What is an example of higher-order derivatives, and how does an integral undo one?
Take f(x)=x3f(x) = x^3: f′(x)=3x2f'(x) = 3x^2, f′′(x)=6xf''(x) = 6x, f′′′(x)=6f'''(x) = 6. Integrating f′′(x)=6xf''(x) = 6x once gives 3x2+C3x^2 + C, which recovers f′f' up to a constant.
In optimization, why is the first derivative used more than the second or higher-order derivatives?
The first derivative finds the candidates, because a smooth function has zero slope at an interior maximum or minimum. The second derivative then classifies them. Higher orders are needed only when f′′f'' is also zero at the candidate, which is uncommon in textbook problems.
Do higher-order derivatives give options traders more insight than delta, gamma and vega?
Yes, a little. Gamma is already a second derivative of an option's price with respect to the underlying price, and third-order sensitivities exist with names of their own. They describe how quickly the familiar measures themselves change.
What does the third derivative tell you about a graph?
It tells you how fast the concavity is changing, as covered in the section on derivatives above order two.
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