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Digital Garden | OER Curriculum
Core Definition

If functions u(x)u(x) and v(x)v(x) are both differentiable at xx, then their product f(x)=u(x)β‹…v(x)f(x) = u(x) \cdot v(x) is also differentiable, and its derivative is given by:

ddx[u(x)β‹…v(x)]=uβ€²(x)v(x)+u(x)vβ€²(x)\frac{d}{dx}[u(x) \cdot v(x)] = u'(x)v(x) + u(x)v'(x)
In words: "The derivative of the first times the second, plus the first times the derivative of the second."

Concept Explanation

1. Geometric Intuition (The Expanding Rectangle)

Consider a rectangle whose area is A(x)=u(x)β‹…v(x)A(x) = u(x) \cdot v(x), where both side lengths u(x)u(x) and v(x)v(x) change as xx varies. When xx increases by a small increment Ξ”x\Delta x, the side lengths increase by Ξ”u\Delta u and Ξ”v\Delta v. The total change in area is:

Ξ”A=(u+Ξ”u)(v+Ξ”v)βˆ’uv=uΞ”v+vΞ”u+Ξ”uΞ”v\Delta A = (u + \Delta u)(v + \Delta v) - uv = u \Delta v + v \Delta u + \Delta u \Delta v
Dividing by Δx\Delta x and taking the limit as Δx→0\Delta x \to 0:
dAdx=udvdx+vdudx+lim⁑Δxβ†’0(Ξ”uΞ”xβ‹…Ξ”v)=uvβ€²+vuβ€²+(uβ€²β‹…0)=uβ€²v+uvβ€²\frac{dA}{dx} = u \frac{dv}{dx} + v \frac{du}{dx} + \lim_{\Delta x \to 0}\left(\frac{\Delta u}{\Delta x} \cdot \Delta v\right) = u v' + v u' + (u' \cdot 0) = u'v + uv'
The corner sliver Ξ”uΞ”v\Delta u \Delta v shrinks to zero faster than the two rectangular strips uΞ”vu \Delta v and vΞ”uv \Delta u.

2. Common Pitfall: The False Product Rule

A frequent mistake is assuming ddx[uv]=uβ€²β‹…vβ€²\frac{d}{dx}[uv] = u' \cdot v'. For instance, if f(x)=xβ‹…x=x2f(x) = x \cdot x = x^2, the correct derivative is 2x2x. But uβ€²β‹…vβ€²=1β‹…1=1β‰ 2xu' \cdot v' = 1 \cdot 1 = 1 \neq 2x. Always use the sum of two cross-terms!

3. The Component Dictionary Strategy

To avoid misplacing terms or algebraic sign errors in multi-step problems, build a 4-part component dictionary before assembling the derivative:

u=FirstΒ functionβ€…β€ŠβŸΉβ€…β€Šuβ€²=dudxv=SecondΒ functionβ€…β€ŠβŸΉβ€…β€Švβ€²=dvdx\begin{aligned} u &= \text{First function} &\implies u' &= \frac{du}{dx} \\ v &= \text{Second function} &\implies v' &= \frac{dv}{dx} \end{aligned}
Then assemble: fβ€²(x)=uβ€²v+uvβ€²f'(x) = u'v + uv'.

4. Extended Product Rule for Three or More Factors

For three differentiable functions f(x)=u(x)β‹…v(x)β‹…w(x)f(x) = u(x) \cdot v(x) \cdot w(x):

ddx[uvw]=uβ€²vw+uvβ€²w+uvwβ€²\frac{d}{dx}[u v w] = u' v w + u v' w + u v w'


Engineering Applications

  • Mechanical Engineering (Dynamic Power Transmission): Mechanical power is the product of torque and angular velocity: P(t)=Ο„(t)β‹…Ο‰(t)P(t) = \tau(t) \cdot \omega(t). The time rate of change of power is dPdt=Ο„β€²(t)Ο‰(t)+Ο„(t)Ο‰β€²(t)\frac{dP}{dt} = \tau'(t)\omega(t) + \tau(t)\omega'(t).
  • Electrical Engineering (Instantaneous Power): Electrical power delivered to an AC load is p(t)=v(t)β‹…i(t)p(t) = v(t) \cdot i(t). The derivative dpdt=vβ€²(t)i(t)+v(t)iβ€²(t)\frac{dp}{dt} = v'(t)i(t) + v(t)i'(t) measures transient power spikes.
  • Entertainment Engineering (Vibrational Rigs): The displacement profile of a damped show platform y(t)=(at+b)sin⁑(Ο‰t)y(t) = (at + b)\sin(\omega t) combines polynomial motion with harmonic oscillations, requiring the product rule to determine velocity.

Example Problems

Example 1: Algebraic and Trigonometric Product

Find the derivative of f(x)=x3sin⁑(x)f(x) = x^3 \sin(x).

Solution
  1. Build the Component Dictionary:
    • u=x3β€…β€ŠβŸΉβ€…β€Šuβ€²=3x2u = x^3 \implies u' = 3x^2
    • v=sin⁑(x)β€…β€ŠβŸΉβ€…β€Švβ€²=cos⁑(x)v = \sin(x) \implies v' = \cos(x)
  2. Apply the Product Rule (uβ€²v+uvβ€²u'v + uv'):
    fβ€²(x)=(3x2)(sin⁑x)+(x3)(cos⁑x)f'(x) = (3x^2)(\sin x) + (x^3)(\cos x)
  3. Factor out common factors:
    fβ€²(x)=x2(3sin⁑x+xcos⁑x)f'(x) = x^2 (3\sin x + x\cos x)

Example 2: Product of Linear and Radical Terms

Find the derivative of g(t)=(2tβˆ’5)t2+1g(t) = (2t - 5)\sqrt{t^2 + 1} or g(t)=(2tβˆ’5)tg(t) = (2t - 5)\sqrt{t}.

Solution

For g(t)=(2tβˆ’5)t12g(t) = (2t - 5)t^{\frac{1}{2}}:

  1. Method 1: Product Rule:
    • u=2tβˆ’5β€…β€ŠβŸΉβ€…β€Šuβ€²=2u = 2t - 5 \implies u' = 2
    • v=t12β€…β€ŠβŸΉβ€…β€Švβ€²=12tβˆ’12v = t^{\frac{1}{2}} \implies v' = \frac{1}{2}t^{-\frac{1}{2}}
      gβ€²(t)=2(t12)+(2tβˆ’5)(12tβˆ’12)=2t+tβˆ’52t=3tβˆ’52tg'(t) = 2(t^{\frac{1}{2}}) + (2t - 5)\left(\frac{1}{2}t^{-\frac{1}{2}}\right) = 2\sqrt{t} + \sqrt{t} - \frac{5}{2\sqrt{t}} = 3\sqrt{t} - \frac{5}{2\sqrt{t}}
  2. Method 2: Pre-Processing (Distributing first):
    g(t)=2t32βˆ’5t12β€…β€ŠβŸΉβ€…β€Šgβ€²(t)=2(32t12)βˆ’5(12tβˆ’12)=3tβˆ’52tg(t) = 2t^{\frac{3}{2}} - 5t^{\frac{1}{2}} \implies g'(t) = 2\left(\frac{3}{2}t^{\frac{1}{2}}\right) - 5\left(\frac{1}{2}t^{-\frac{1}{2}}\right) = 3\sqrt{t} - \frac{5}{2\sqrt{t}}
    Both methods yield the identical result.

Connections & References