IB Maths AA HL Topic 5 — Calculus Paper 1 & 2 ~7 min read

Concavity & Points of Inflection

The sign of f″(x) determines whether the curve “smiles” or “frowns”. f″(x) > 0 means concave up (smile shape); f″(x) < 0 means concave down (frown shape). A point of inflection is where the concavity changes — both f″ = 0 AND a sign change of f″ are needed. Crucially, points of inflection don’t need to be stationary points.

📘 What you need to know

What concavity looks like

Concave up vs concave down — see where the tangents lie CONCAVE UP f″(x) > 0 • smiling ☺ • tangents below curve CONCAVE DOWN f″(x) < 0 • frowning ☹ • tangents above curve
The tangent lines sit on the inside of the bend. If they lie below the curve → concave up. If they lie above → concave down.
Memory trick: concave UP looks like a cUp ☕ (or a smile); concave Down looks like a froWN. The second derivative sign matches: positive = up, negative = down.

Points of inflection

Point of inflection — concavity flips through this point point of inflection f″ = 0 AND sign changes concave down (f″ < 0) concave up (f″ > 0)
At a point of inflection the curve transitions from one concavity to the other. The tangent crosses through the curve at this point.
Conditions for a point of inflection at x = a f″(a) = 0    AND    f″ changes sign through x = a
Both conditions matter: if f″(a) = 0 but f″ has the same sign on both sides (e.g. f″(x) = x² touches zero at 0 but is non-negative everywhere), then x = a is NOT a point of inflection — concavity didn’t change.

Stationary vs non-stationary inflection

Stationary (horizontal) POI
f′(a) = 0 & f″(a) = 0
tangent is horizontal at the POI
example: y = x³ at x = 0
Non-stationary POI
f′(a) ≠ 0 & f″(a) = 0
tangent is sloped at the POI
example: y = x³ + x at x = 0

🧭 Recipe — find & justify points of inflection

  1. Differentiate twice to get f″(x); solve f″(x) = 0 for the candidate x-values.
  2. Test concavity on each side of each candidate by evaluating f″ slightly left and slightly right.
  3. Confirm sign change: if concavity flips through x = a, then x = a is a point of inflection.
  4. Find the y-coordinate by substituting into the original f(x).
  5. State the answer fully: “(a, f(a)) is a POI because f″(a) = 0 AND concavity changes from … to …”.

Worked examples

WE 1

Concavity at specific points

The function f(x) = 2x³ − x² + 5. Determine whether the curve is concave up or concave down at: (a) x = 1; (b) x = −1.

Find f″(x) f′(x) = 6x² − 2x f″(x) = 12x − 2 (a) Evaluate at x = 1 f″(1) = 12 − 2 = 10 > 0 → concave up (b) Evaluate at x = −1 f″(−1) = −12 − 2 = −14 < 0 → concave down (a) concave up at x = 1; (b) concave down at x = −1 at a single point, just check the SIGN of f″ — magnitude doesn’t matter
WE 2

Find intervals of concavity

For f(x) = x³ + 2x² − 7, find the values of x for which the graph is (a) concave up; (b) concave down.

Find f″(x) f′(x) = 3x² + 4x f″(x) = 6x + 4 (a) Concave up: solve f″(x) > 0 6x + 4 > 0 → 6x > −4 → x > −2/3 (b) Concave down: solve f″(x) < 0 6x + 4 < 0 → x < −2/3 (a) concave up for x > −2/3; (b) concave down for x < −2/3 at x = −2/3 the concavity changes — this is the POI of any cubic with positive leading coeff
WE 3

Find the POI of a cubic — fully justified

Find the coordinates of the point of inflection on the graph of y = x³ − 6x² + 9x + 2. Fully justify your answer.

Differentiate twice y′ = 3x² − 12x + 9 y″ = 6x − 12 Solve y″(x) = 0 6x − 12 = 0 → x = 2 Test concavity each side of x = 2 y″(1.9) = 11.4 − 12 = −0.6 < 0 (concave down) y″(2.1) = 12.6 − 12 = 0.6 > 0 (concave up) → concavity changes through x = 2 ✓ y-coordinate y(2) = 8 − 24 + 18 + 2 = 4 (2, 4) is a point of inflection (since y″(2) = 0 AND concavity changes) a cubic with non-zero leading coefficient ALWAYS has exactly one POI
WE 4

Non-stationary POI — POI ≠ stationary point

For f(x) = x³ + x: (a) Show that (0, 0) is a point of inflection. (b) Show that (0, 0) is NOT a stationary point.

Compute f′ and f″ f′(x) = 3x² + 1 f″(x) = 6x (a) f″(0) = 0; check concavity changes f″(−1) = −6 < 0 (concave down) f″(1) = 6 > 0 (concave up) → concavity changes through x = 0; f(0) = 0 → (0, 0) is a POI ✓ (b) Test if it’s a stationary point f′(0) = 3·0 + 1 = 1 ≠ 0 → tangent has slope 1 at (0, 0), NOT horizontal (a) (0, 0) is a POI; (b) NOT a stationary point — slope is 1, tangent is y = x key takeaway: POI is about CONCAVITY change, NOT about gradient being zero
WE 5

Quartic — multiple points of inflection

Find all points of inflection on the graph of f(x) = x⁴ − 6x².

Compute f″(x) f′(x) = 4x³ − 12x f″(x) = 12x² − 12 = 12(x² − 1) = 12(x − 1)(x + 1) Solve f″(x) = 0 → x = −1 or x = 1 Test concavity in each region x < −1: f″(−2) = 36 > 0 (concave up) −1 < x < 1: f″(0) = −12 < 0 (concave down) x > 1: f″(2) = 36 > 0 (concave up) → concavity changes at BOTH x = −1 and x = 1 y-coordinates f(−1) = 1 − 6 = −5 f(1) = 1 − 6 = −5 Points of inflection: (−1, −5) and (1, −5) a quartic can have up to 2 POIs (since f″ is quadratic, with up to 2 roots)
WE 6

Application — kinematics: when does the acceleration change sign?

A car’s displacement (in metres) from a starting point at time t seconds is given by s(t) = −t³ + 6t² + 2t, for 0 ≤ t ≤ 5.

(a) Find the velocity v(t) and acceleration a(t). (b) Find the time at which the acceleration is zero, and the displacement at that time. (c) Interpret what happens physically at this moment.

(a) Differentiate v(t) = s′(t) = −3t² + 12t + 2 a(t) = s″(t) = −6t + 12 (b) Solve a(t) = 0 −6t + 12 = 0 → t = 2 seconds s(2) = −8 + 24 + 4 = 20 metres Check concavity change a(1) = 6 > 0 (s concave up; car speeding up) a(3) = −6 < 0 (s concave down; car slowing down) → POI on s(t) at t = 2 (c) v(2) = −12 + 24 + 2 = 14 m/s — maximum velocity (a) v(t) = −3t² + 12t + 2, a(t) = −6t + 12; (b) t = 2 s, s = 20 m; (c) the car reaches its maximum speed (14 m/s) and then starts decelerating in kinematics: s″(t) is acceleration. POI on s ↔ acceleration crosses zero ↔ maximum velocity

💡 Top tips

⚠ Common mistakes

Up next: Derivatives & Graphs. Putting it all together — given the graph of f, sketch the graphs of f′ and f″, and vice versa. Roots of f′ correspond to stationary points of f; roots of f″ correspond to points of inflection of f. The interplay between f, f′, and f″ in a single problem is a Paper 1 favourite.

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