Single-Variable-Calculus · Unit 3 · Video 6 · Interactive Practice

Finishing the Geometric Proof: One Rotation, Then the Product and Quotient Rules

IKey Formulas

FormulaNameWhere it comes from
∠QPR=θ+Δθ2≈θ\angle QPR = \theta + \tfrac{\Delta\theta}{2} \approx \thetaThe angle at PPTurn the angle θ\theta at OO through 90°90\degree
Δy≈Δθcos⁡θ  ⟹  lim⁡Δθ→0ΔyΔθ=cos⁡θ\Delta y \approx \Delta\theta\cos\theta \;\Longrightarrow\; \lim\limits_{\Delta\theta \to 0}\dfrac{\Delta y}{\Delta\theta} = \cos\thetaDerivative of sine, geometricallyAdjacent == hypotenuse ×cos⁡\times \cos in △PQR\triangle PQR
(uv)′=u′v+uv′(uv)' = u'v + uv'Product ruleThe two strips of a growing rectangle
(uv)′=u′v−uv′v2,v≠0\left(\dfrac{u}{v}\right)' = \dfrac{u'v - uv'}{v^2}, \quad v \neq 0Quotient ruleThe same two terms, joined by a minus

Key Insight: Both new rules change one function at a time. In the rectangle picture the strips u Δvu\,\Delta v and v Δuv\,\Delta u become the two terms of (uv)′(uv)', while the corner Δu Δv\Delta u\,\Delta v dies faster than Δx\Delta x — which is why the product u′v′u'v' never appears in either rule.

IIVisualization 1 — One Rotation Names the Angle at PP

Turning the angle at OO through a right angle carries it exactly onto the angle at PP.

💡 Small-change triangles like PQRPQR return in multivariable calculus, and cutting a curve into such triangles is how arc length is built.

IIIVisualization 2 — The Difference Quotient Becomes cos⁡θ\cos\theta

Shrinking Δθ\Delta\theta drives the difference quotient of sin⁡θ\sin\theta onto the graph of cos⁡θ\cos\theta.

IVVisualization 3 — Two Strips and a Vanishing Corner

Growing uu and vv one at a time adds two strips; the corner is the piece the product rule discards.

💡 The quotient rule is proved the same way, one function at a time — and it carries the extra condition v≠0v \neq 0, since v2v^2 sits in the denominator.

VQuiz Questions

Problem 1 · Reading the Right Triangle

Given: in △PQR\triangle PQR the right angle is at RR, the hypotenuse PQPQ has length ≈Δθ\approx \Delta\theta, and the angle at PP is ≈θ\approx \theta. The vertical side PRPR, of length Δy\Delta y, is the side next to that angle. Which relation follows?

✅ Correct! Adjacent == hypotenuse ×cos⁡(angle)\times \cos(\text{angle}), and dividing by Δθ\Delta\theta gives Δy/Δθ≈cos⁡θ\Delta y/\Delta\theta \approx \cos\theta.
❌ That is the other leg. sin⁡θ\sin\theta multiplies the hypotenuse to give the side opposite the angle at PP — the horizontal side RQRQ, not PRPR.
❌ The cosine multiplies, it does not divide. cos⁡θ=adjacenthypotenuse=ΔyΔθ\cos\theta = \dfrac{\text{adjacent}}{\text{hypotenuse}} = \dfrac{\Delta y}{\Delta\theta}, so Δy=Δθcos⁡θ\Delta y = \Delta\theta\cos\theta.
❌ The hypotenuse is missing. cos⁡θ\cos\theta alone is a ratio, not a length; it has to be scaled by the hypotenuse Δθ\Delta\theta.
❌ Not quite. Write the definition of cosine in this triangle first: cos⁡(∠QPR)=PR/PQ\cos(\angle QPR) = PR/PQ.
Show solution

In a right triangle the cosine of an angle is the adjacent side over the hypotenuse. At PP:

cos⁡(∠QPR)=PRPQ≈ΔyΔθ\cos(\angle QPR) = \frac{PR}{PQ} \approx \frac{\Delta y}{\Delta\theta}

With ∠QPR≈θ\angle QPR \approx \theta this rearranges to

Δy≈Δθcos⁡θ\Delta y \approx \Delta\theta\cos\theta

Dividing by Δθ\Delta\theta turns the geometry into the difference quotient of the sine, ΔyΔθ≈cos⁡θ\dfrac{\Delta y}{\Delta\theta} \approx \cos\theta, and letting Δθ→0\Delta\theta \to 0 makes both approximations exact:

ddxsin⁡x=cos⁡x\frac{d}{dx}\sin x = \cos x

Problem 2 · Product Rule, First Use

Given: f(x)=x2sin⁡xf(x) = x^2 \sin x — differentiate it.

✅ Correct! Each factor is differentiated once, in its own term, while the other factor is left alone.
❌ That is u′v′u'v'. The derivative of a product is never the product of the derivatives — the vanishing corner Δu Δv\Delta u\,\Delta v is exactly the piece that would have produced such a term.
❌ The minus belongs to the quotient rule. The product rule joins its two terms with a plus: both strips add area to the rectangle.
❌ The derivatives are on the wrong factors. In each term exactly one factor wears the prime: u′vu'v then uv′uv'.
❌ Not quite. Take u=x2u = x^2 and v=sin⁡xv = \sin x, so u′=2xu' = 2x and v′=cos⁡xv' = \cos x, and assemble u′v+uv′u'v + uv'.
Show solution

Set u=x2u = x^2 and v=sin⁡xv = \sin x, so u′=2xu' = 2x and v′=cos⁡xv' = \cos x. The product rule gives

(uv)′=u′v+uv′=(2x)(sin⁡x)+(x2)(cos⁡x)(uv)' = u'v + uv' = (2x)(\sin x) + (x^2)(\cos x) f′(x)=2xsin⁡x+x2cos⁡xf'(x) = 2x\sin x + x^2\cos x

Check the shape of the answer: each term contains one primed factor and one unprimed factor. A term with two primes (2xcos⁡x2x\cos x) or with no prime (x2sin⁡xx^2\sin x) cannot belong to the rule.

Problem 3 · Both Rules at a Single Point

Given: u(2)=3u(2) = 3, u′(2)=−1u'(2) = -1, v(2)=4v(2) = 4, v′(2)=5v'(2) = 5 — evaluate both rules at x=2x = 2.

What is (uv)′(2)(uv)'(2)?

What is (uv)′(2)\left(\dfrac{u}{v}\right)'(2)?

✅ Correct! The same two products, u′v=−4u'v = -4 and uv′=15uv' = 15, are added for the product rule and subtracted (then divided by v2=16v^2 = 16) for the quotient rule.
❌ That is u′(2) v′(2)u'(2)\,v'(2). The product of the derivatives is never a term of either rule.
❌ A sign was dropped. u′(2)=−1u'(2) = -1, so u′v=(−1)(4)=−4u'v = (-1)(4) = -4, not +4+4.
❌ The numerator is the wrong way round. The derivative of the top function comes first: u′v−uv′u'v - uv', not uv′−u′vuv' - u'v.
❌ That is the product rule's numerator. The quotient rule joins the same two terms with a minus sign.
❌ Check the denominator. It is v2=42=16v^2 = 4^2 = 16, not v=4v = 4.
❌ Check the product rule. (uv)′=u′v+uv′(uv)' = u'v + uv', so evaluate (−1)(4)+(3)(5)(-1)(4) + (3)(5).
❌ Check the quotient rule. (uv)′=u′v−uv′v2\left(\frac{u}{v}\right)' = \frac{u'v - uv'}{v^2}, so evaluate (−1)(4)−(3)(5)42\frac{(-1)(4) - (3)(5)}{4^2}.
Show solution

Both rules are built from the same two products:

u′(2) v(2)=(−1)(4)=−4,u(2) v′(2)=(3)(5)=15u'(2)\,v(2) = (-1)(4) = -4, \qquad u(2)\,v'(2) = (3)(5) = 15

Product rule:

(uv)′(2)=u′v+uv′=−4+15=11(uv)'(2) = u'v + uv' = -4 + 15 = 11

Quotient rule (the top function is differentiated first, and the denominator is squared):

(uv)′(2)=u′v−uv′v2=−4−1542=−1916\left(\frac{u}{v}\right)'(2) = \frac{u'v - uv'}{v^2} = \frac{-4 - 15}{4^2} = \frac{-19}{16}

Since v(2)=4≠0v(2) = 4 \neq 0, the quotient rule applies at this point.

Problem 4 · The Same Triangle Gives the Derivative of Cosine

Given: the same triangle, now read horizontally. The side RQRQ is opposite the angle θ\theta at PP, and in the first quadrant QQ lies to the left of PP, so Δx=cos⁡(θ+Δθ)−cos⁡θ\Delta x = \cos(\theta + \Delta\theta) - \cos\theta is negative. Find the derivative of cosine.

How long is the horizontal side RQRQ?

So what is lim⁡Δθ→0ΔxΔθ\lim\limits_{\Delta\theta \to 0} \dfrac{\Delta x}{\Delta\theta}?

✅ Correct! One triangle yields both trigonometric derivatives: its vertical leg gives cos⁡x\cos x, its horizontal leg gives −sin⁡x-\sin x.
❌ That is the vertical leg. cos⁡θ\cos\theta scales the side adjacent to the angle at PP, which is PR=ΔyPR = \Delta y. The opposite side takes sin⁡θ\sin\theta.
❌ The length is right, the sign is not. RQRQ is a length, but Δx\Delta x is a displacement to the left, so Δx=−Δθsin⁡θ\Delta x = -\Delta\theta\sin\theta.
❌ Check which leg you are measuring. Opposite == hypotenuse ×sin⁡(angle)\times \sin(\text{angle}), with hypotenuse ≈Δθ\approx \Delta\theta and angle ≈θ\approx \theta.
❌ Check the sign. Moving counterclockwise in the first quadrant pushes QQ to the left of PP, so Δx<0\Delta x < 0 while Δθ>0\Delta\theta > 0.
Show solution

In △PQR\triangle PQR the angle at PP is ≈θ\approx \theta and the hypotenuse PQPQ is ≈Δθ\approx \Delta\theta. The horizontal side RQRQ is opposite that angle, so

RQ≈Δθsin⁡θRQ \approx \Delta\theta \sin\theta

QQ sits to the left of PP, so the signed horizontal change is Δx≈−Δθsin⁡θ\Delta x \approx -\Delta\theta\sin\theta. Dividing by Δθ\Delta\theta and letting Δθ→0\Delta\theta \to 0:

lim⁡Δθ→0ΔxΔθ=−sin⁡θ⟹ddxcos⁡x=−sin⁡x\lim_{\Delta\theta \to 0}\frac{\Delta x}{\Delta\theta} = -\sin\theta \qquad\Longrightarrow\qquad \frac{d}{dx}\cos x = -\sin x

This matches the formula proved earlier from the two limits at zero, so the geometric picture reproduces both trigonometric derivatives at a general angle.

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