Mathematics Advanced • Year 11 • Module 3 • Lesson 7

The Second Derivative

Build procedural fluency in computing f″(x), interpreting concavity, and finding points of inflection.

Build · Skill Drill

1. Quick recall

Answer each in the space provided. 1 mark each

Q1.1 Complete each statement using >, <, or =.

A curve is concave up when f″(x) ______ 0.

A curve is concave down when f″(x) ______ 0.

A point of inflection requires f″(x) ______ 0 and a sign change.

Q1.2 Match each notation with what it means:

f′(x)    ↔   ____________________________

f″(x)    ↔   ____________________________

d²y/dx²   ↔   ____________________________

Q1.3 In kinematics: if s(t) is position, then s′(t) represents ____________ and s″(t) represents ____________.

Stuck? Revisit lesson § Key Terms and § Concept.

2. Worked example — f(x) = 3x⁴ − 2x³ + x

Differentiate twice, then factorise to find candidates for inflection points.

Problem. Find f″(x) for f(x) = 3x⁴ − 2x³ + x.

Step 1 — Differentiate term by term to get f′(x).

f′(x) = 12x³ − 6x² + 1

Reason: power rule on each term; the constant term in f drops to 0 (no contribution).

Step 2 — Differentiate f′(x) to get f″(x).

f″(x) = 36x² − 12x

Reason: differentiate the first derivative; the +1 drops out.

Step 3 — Factorise to find where f″(x) = 0.

f″(x) = 12x(3x − 1) = 0   ⇒   x = 0 or x = 1/3

Reason: factoring exposes the two candidate inflection points (sign change still needs to be checked).

Conclusion. f″(x) = 12x(3x − 1); candidates for inflection are x = 0 and x = 1/3.

3. Faded example — fill in the missing steps

Show that y = x³ − 6x² + 9x has a point of inflection and find its coordinates. Fill in each blank. 4 marks

Step 1 — First derivative:

dy/dx = ______________________

Step 2 — Second derivative:

d²y/dx² = ______________________

Step 3 — Set d²y/dx² = 0 and solve:

______________________ = 0   ⇒   x = ______________

Step 4 — Check sign change of d²y/dx² across x = ______:

For x just below: d²y/dx² is ______; for x just above: d²y/dx² is ______. Sign change confirmed.

Step 5 — y-coordinate: at x = ______, y = ______________________.

Conclusion. Point of inflection at ( ______ , ______ ).

Stuck? Revisit lesson § Worked Example 2.

4. Graduated practice — second derivative work

For each function, compute the requested derivative and answer concisely.

Foundation — pure derivative computation (4 questions)

QFunction f(x)f′(x)f″(x)
4.1 1f(x) = x⁵ − 4x³ + 2x
4.2 1f(x) = sin x
4.3 1f(x) = cos x
4.4 1f(x) = ex

Standard — concavity and inflection (6 questions)

4.5 Find d²y/dx² for y = sin x, then state where d²y/dx² < 0 in the interval 0 ≤ x ≤ 2π.    2 marks

4.6 Determine the concavity of y = x⁴ − 2x² at x = 1.    2 marks

4.7 Find the point of inflection of y = x³ − 3x².    2 marks

4.8 For f(x) = 2x³ − 9x² + 12x, find f″(x) and find the x-values where the curve is concave up.    2 marks

4.9 If s(t) = 2t³ − t² metres, find the acceleration at t = 1 s.    2 marks

4.10 Show that y = x⁴ has f″(0) = 0 but x = 0 is not a point of inflection.    2 marks

Extension — combine ideas (2 questions)

4.11 Show that y = x⁴ − 4x³ has two points of inflection, finding both x-values and the corresponding y-coordinates.    3 marks

4.12 A particle's position is s(t) = t³ − 6t² + 9t metres for t ≥ 0. Find the time at which the acceleration is zero, and the velocity at that instant.    3 marks

Stuck on 4.10? f″(0) = 0 is necessary but not sufficient; you must check sign change in f″.

5. Self-check the easy 3

Tick the first three once you have checked your work.

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What I'll revisit before next class:

Answers — Do not peek before attempting

Q1.1 — Concavity conditions

Concave up: f″(x) > 0.   Concave down: f″(x) < 0.   Inflection: f″(x) = 0 (and sign change).

Q1.2 — Notation

f′(x): first derivative (rate of change / gradient).   f″(x): second derivative (rate of change of the gradient / concavity / acceleration).   d²y/dx²: Leibniz notation for the second derivative (single symbol, not a fraction to cancel).

Q1.3 — Kinematics

s′(t) = velocity.   s″(t) = acceleration.

Q3 — Faded example y = x³ − 6x² + 9x

Step 1: dy/dx = 3x² − 12x + 9.   Step 2: d²y/dx² = 6x − 12.   Step 3: 6x − 12 = 0 ⇒ x = 2.   Step 4: at x = 1, d²y/dx² = −6 (negative); at x = 3, d²y/dx² = 6 (positive); sign change confirmed.   Step 5: y(2) = 8 − 24 + 18 = 2.   Conclusion: point of inflection at (2, 2).

Q4.1 — f(x) = x⁵ − 4x³ + 2x

f′(x) = 5x⁴ − 12x² + 2.   f″(x) = 20x³ − 24x.

Q4.2 — f(x) = sin x

f′(x) = cos x.   f″(x) = −sin x.

Q4.3 — f(x) = cos x

f′(x) = −sin x.   f″(x) = −cos x.

Q4.4 — f(x) = ex

f′(x) = ex.   f″(x) = ex. The exponential function is its own derivative at every order.

Q4.5 — d²y/dx² for y = sin x; concavity on [0, 2π]

d²y/dx² = −sin x. We need −sin x < 0, i.e. sin x > 0. On [0, 2π] this happens for 0 < x < π.

Q4.6 — concavity of y = x⁴ − 2x² at x = 1

dy/dx = 4x³ − 4x; d²y/dx² = 12x² − 4. At x = 1: d²y/dx² = 12 − 4 = 8 > 0, so the curve is concave up at x = 1.

Q4.7 — point of inflection of y = x³ − 3x²

dy/dx = 3x² − 6x; d²y/dx² = 6x − 6 = 0 ⇒ x = 1. Sign change: at x = 0, d²y/dx² = −6 (−); at x = 2, d²y/dx² = 6 (+). ✓ y(1) = 1 − 3 = −2. Point of inflection at (1, −2).

Q4.8 — f(x) = 2x³ − 9x² + 12x

f′(x) = 6x² − 18x + 12; f″(x) = 12x − 18. Concave up when f″(x) > 0: 12x − 18 > 0 ⇒ x > 3/2.

Q4.9 — acceleration for s(t) = 2t³ − t² at t = 1

v(t) = 6t² − 2t; a(t) = 12t − 2. a(1) = 12 − 2 = 10 m/s².

Q4.10 — y = x⁴ at x = 0

y′ = 4x³; y″ = 12x². At x = 0, y″(0) = 0. But for x < 0, y″ = 12x² > 0, and for x > 0, y″ = 12x² > 0 also. There is no sign change, so x = 0 is not a point of inflection (the curve is concave up on both sides — it's actually a minimum).

Q4.11 — inflection points of y = x⁴ − 4x³

y′ = 4x³ − 12x²; y″ = 12x² − 24x = 12x(x − 2) = 0 ⇒ x = 0 or x = 2.
At x = 0: for x = −1, y″ = 36 (+); for x = 1, y″ = −12 (−). Sign change ✓   y(0) = 0.
At x = 2: for x = 1, y″ = −12 (−); for x = 3, y″ = 36 (+). Sign change ✓   y(2) = 16 − 32 = −16.
Inflection points at (0, 0) and (2, −16).

Q4.12 — s(t) = t³ − 6t² + 9t: when a = 0

v(t) = 3t² − 12t + 9; a(t) = 6t − 12 = 0 ⇒ t = 2 s.   v(2) = 12 − 24 + 9 = −3 m/s (particle moving in the negative direction at the instant acceleration vanishes).