MATH U101 · Multivariable Calculus · Module 2

Limits, Continuity & Vector-Valued Functions

Two halves: the self-study revision block §2.3–2.6 (limits & continuity of single-variable functions), then the new material — vector functions, motion, arc length and curvature §13.1–13.4.

How to read this module strategically

The handout marks §2.3–2.6 as "self-study — revision of 12th class topics." This is the one block where BITSAT students genuinely have a head start, and the one block the lecturer will not teach — so this is exactly where your extra weekly hours should go, and go first. Part A below is a complete map of it. Part B (vector functions) is new to everyone and builds directly on Part A: a vector function is just three ordinary functions in a trench coat.

Part A · Limits and continuity, the complete refresher

Thomas §2.3–2.6 — self-study block. Budget: the biggest single slice of catch-up time.

A1 · What a limit is

limxa f(x) = L says: as x gets close to a — from either side, without ever equalling a — the values f(x) get and stay close to L.

The crucial subtlety: the limit is about the journey, not the destination. f(a) may be undefined, or defined with a different value — the limit doesn't care. That's why (x2−9)/(x−3) has a perfectly good limit at x = 3 even though the function is undefined there.

The 0/0 toolbox — 90% of limit problems

If plugging in gives a number, that's the answer (for the nice functions in this course). If it gives 0/0, the form is hiding a common factor. Three tools, in order of frequency:

ToolUse whenOne-line example
Factor & cancelPolynomialslimx→3 x2−9x−3 = limx→3 (x+3) = 6
RationaliseSquare rootslimx→0 √(x+1) − 1x = limx→0 1√(x+1) + 1 = ½
Known special limitTrig over xlimθ→0 sin θθ = 1 (θ in radians — memorise)

A fourth tool worth knowing by name: the Sandwich (Squeeze) Theorem — if gfh near a and g and h share the limit L, then fL too. Its signature use: limx→0 x2 sin(1/x) = 0, squeezed between x2 and x2.

A2 · The precise (ε–δ) definition §2.3

This is the part that is genuinely new even to BITSAT students — 12th boards state limits informally; Thomas §2.3 makes it rigorous. Think of it as a challenge game between a skeptic and you:

The game

Skeptic: "I bet f(x) doesn't really stay within ε = 0.01 of L."
You: "It does — keep x within δ = 0.003 of a and you'll see."
The limit exists if you can win for every ε the skeptic picks, by producing a suitable δ. Formally: for every ε > 0 there is a δ > 0 such that 0 < |xa| < δ|f(x) − L| < ε.

Worked example 1Prove limx→2 (3x − 1) = 5 with ε–δ

  1. Start from what must be small: |f(x) − 5| = |3x − 6| = 3|x − 2|.
  2. We need 3|x − 2| < ε, i.e. |x − 2| < ε/3.
  3. So choose δ = ε/3. Then 0 < |x−2| < δ forces |f(x)−5| < ε. Done.

Every linear ε–δ proof is this same two-line algebra: express |f(x) − L| as (constant)·|xa|, then divide ε by the constant. Master the linear case cold; anything harder is rarely examined at this level.

A3 · One-sided limits §2.4

xa approaches from the left, xa+ from the right. The two-sided limit exists iff both one-sided limits exist and agree. The canonical counterexample: f(x) = |x|/x, which is −1 for negative x and +1 for positive x — the one-sided limits at 0 are −1 and 1, so limx→0 does not exist.

One-sided limits are the working tool for every piecewise function — and piecewise functions are the exam's favourite way to test this whole block.

A4 · Continuity §2.5

f is continuous at a when three things hold — and exam answers are expected to check all three:

  1. f(a) exists (the point is on the graph),
  2. limxa f(x) exists (both sides agree),
  3. the two are equal.

Polynomials, sin, cos, exponentials are continuous everywhere; rational functions everywhere their denominator isn't zero; sums, products, quotients (nonzero denominator) and compositions of continuous functions are continuous. In practice: to evaluate a limit of a continuous function, just substitute.

Worked example 2Find c so that f is continuous everywhere

f(x) = x2 for x < 1, and f(x) = 2xc for x ≥ 1.

  1. Each piece is a polynomial — continuous on its own territory. The only risk is the seam at x = 1.
  2. Left limit: x2 → 1. Right limit (and value): 2(1) − c = 2 − c.
  3. Match them: 2 − c = 1c = 1.

This "match at the seam" pattern is the single most common exam question from §2.5.

One theorem to know by name: the Intermediate Value Theorem — a function continuous on [a, b] takes every value between f(a) and f(b). Standard use: "show x3x − 1 = 0 has a root in [1, 2]" — evaluate at both ends (−1 and 5), note the sign change, cite IVT.

A5 · Limits at infinity & asymptotes §2.6

For x → ±∞ in a ratio, divide top and bottom by the highest power of x in the denominator. The shortcut you'll use forever, for rational functions:

Classic traps in Part A

1) Writing lim = f(a) by reflex when the function is piecewise or has a hole — check the seam. 2) Using sin x/x → 1 in degrees mode — it's a radians fact. 3) "Denominator is 0, so vertical asymptote" — not if the numerator is 0 too (factor first!). 4) Saying a limit "= ∞" and calling it "exists" — ∞ is a description of behaviour, not a number; the limit does not exist.

Part B · Vector-valued functions and motion in space

Thomas §13.1–13.4 — new to everyone. Prereqs: Part A, vectors, differentiation rules.

B1 · A curve as a moving point §13.1

A vector-valued function feeds in a time t and returns a position vector:

r(t) = f(t) i + g(t) j + h(t) k = ⟨f(t), g(t), h(t)⟩

As t runs, the tip of r(t) traces a curve in space. The mental model for the whole chapter: a fly buzzing along a path. The path is geometry; the fly's speed along it is dynamics — this chapter connects the two (exactly the "relation between dynamics and geometry of motion" your learning outcome promises).

The headline example, used in every section: the helix r(t) = ⟨cos t, sin t, t — a point circling the z-axis while rising at a steady rate, like a spiral staircase.

The one idea that makes this chapter easy

Everything happens componentwise. Limits, continuity, derivatives, integrals of r(t) are all computed by doing ordinary single-variable calculus to f, g, h separately. A vector function is three scalar functions in a trench coat. If you can differentiate cos t, you can differentiate a helix. Continuity of r at a = continuity of all three components at a — which is why Part A had to come first.

B2 · Velocity, speed, acceleration

Differentiate componentwise; the results have physical names:

ObjectDefinitionTypeMeaning
Velocityv(t) = r′(t)vectortangent to the path, points where you're heading
Speed|v(t)|scalarhow fast, ignoring direction
Accelerationa(t) = v′(t)vectorhow velocity changes (turning counts, even at constant speed)
Unit tangentT = v/|v|unit vectorpure direction of travel

The differentiation rules all survive, including two product rules — note the cross-product rule preserves order, because u × vv × u:

(u · v)′ = u′ · v + u · v′  (u × v)′ = u′ × v + u × v

A beautiful consequence worth quoting in exams: if |r(t)| is constant (motion on a sphere or circle), then differentiating r · r = const gives r · r′ = 0position and velocity are perpendicular. That's why the moon's velocity is always at right angles to its position vector.

B3 · Arc length §13.3

Why this matters

Distance travelled = speed × time, integrated: over a tiny dt the fly covers |v| dt. Sum the pieces:

L = ∫ab |v(t)| dt = ∫ab √(f′(t)2 + g′(t)2 + h′(t)2) dt

The arc-length parameter s(t) is distance travelled since a start time; its key property is ds/dt = |v| ("rate of covering distance = speed"). It exists so curvature (next) can be defined in terms of the road, not the driver.

B4 · Curvature and the normal vector §13.4

Curvature κ measures how sharply the road bends, per metre of road. Sharp hairpin = large κ; motorway = small κ; straight line = 0. Definition: how fast the direction T turns per unit of distance (not time — bending is a property of the road, not of how fast you drive it):

κ = |dT/ds| = |dT/dt||v|   N = dT/dt|dT/dt|

The principal unit normal N points the way the curve is turning — always perpendicular to T (because T has constant length 1, the perpendicularity fact from B2 applies). Anchor facts to sanity-check every answer: a straight line has κ = 0; a circle of radius a has κ = 1/a — the bigger the circle, the gentler the bend.

Worked example 3Full workout on the helix r(t) = ⟨cos t, sin t, t

This one example exercises every formula in Part B — it is the exam rehearsal.

  1. Velocity: differentiate componentwise: v = ⟨−sin t, cos t, 1⟩.
  2. Speed: |v| = √(sin2t + cos2t + 1) = √2 — constant. (The identity sin2+cos2 = 1 saves the day, as it will constantly.)
  3. Arc length over one full turn 0 ≤ t ≤ 2π: L = ∫0 √2 dt = 2π√2.
  4. Unit tangent: T = v/√2 = ⟨−sin t, cos t, 1⟩/√2.
  5. Turn rate: dT/dt = ⟨−cos t, −sin t, 0⟩/√2, so |dT/dt| = 1/√2.
  6. Curvature: κ = (1/√2)/√2 = 1/2 — constant, and sensibly less than the κ = 1 of the unit circle it shadows: stretching a circle upward into a helix straightens it slightly.
  7. Normal: N = ⟨−cos t, −sin t, 0⟩ — horizontal, pointing straight at the z-axis. The helix is forever "turning toward" its own axis. Check: T · N = 0 ✓.
Classic traps in Part B

1) Speed is not velocity — one is a scalar, one a vector; exam questions dock marks for answering with the wrong type. 2) |r′(t)| ≠ (|r(t)|)′ — the magnitude of the derivative is not the derivative of the magnitude. Compute r first, then take the magnitude. 3) Zero acceleration is not implied by constant speed — the helix has constant speed √2 yet nonzero acceleration, because direction changes. 4) Forgetting to normalise: T and N must have length 1 — always divide by the magnitude and verify.

Your minimal prerequisite kit for this module

What to practise in Thomas

SkillWhereHow many
0/0 limits (factor, rationalise, sin θ/θ), one-sided limits§2.4 exercises10–12
ε–δ for linear functions§2.3 exercises3–4
Continuity of piecewise functions, find-the-constant, IVT§2.5 exercises6–8
Limits at ∞, all asymptote types§2.6 exercises6–8
r(t): sketch, v, a, speed§13.1 exercises6–8
Arc length; T§13.3 exercises4–6
Curvature, N (circles, helices, plane curves)§13.4 exercises4–6

(§13.2 — integrals of vector functions and projectile motion — is starred on the handout; skim the integral definition, and ask the instructor whether projectile motion is examinable before investing time there.)