The product rule is a general rule for differentiation problems where one function is multiplied by another function. The derivative of the product of two differentiable functions is equal to the sum of the first function multiplied by the derivative of the second, and the second function multiplied by the derivative of the first function. The functions may be exponential, logarithmic, or of other types.
Let \( F(x) = f(x) \cdot g(x) \). If \( f'(x) \) and \( g'(x) \) exist, then
\[ F'(x) = f(x) \cdot g'(x) + g(x) \cdot f'(x) \]
For example, consider \( F(x) = (x^2 + 3x)(4x + 5) \). Then \( F \) is the product of two functions \( f \) and \( g \), where \( f(x) = x^2 + 3x \) and \( g(x) = 4x + 5 \). The product rule gives:
\[ F'(x) = f(x) \cdot g'(x) + g(x) \cdot f'(x) \]
\[ = (x^2 + 3x) \cdot 4 + (4x + 5) \cdot (2x + 3) \]
\[ = 4x^2 + 12x + 8x^2 + 22x + 15 \]
\[ = 12x^2 + 34x + 15 \]
This could also have been found by multiplying \( x^2 + 3x \) by \( 4x + 5 \) and then differentiating.
Let \( F(x) = f(x) \cdot g(x) \). If \( f'(x) \) and \( g'(x) \) exist, then
\[ F'(x) = f(x) \cdot g'(x) + g(x) \cdot f'(x) \]
By the definition of the derivative of \( F \), we have
\[ F'(x) = \lim_{h \to 0} \frac{F(x + h) - F(x)}{h} = \lim_{h \to 0} \frac{f(x + h) g(x + h) - f(x) g(x)}{h} \]
Adding and subtracting \( f(x + h) g(x) \):
\[ F'(x) = \lim_{h \to 0} \frac{f(x + h) g(x + h) - f(x) g(x) + f(x + h) g(x) - f(x + h) g(x)}{h} \]
\[ = \lim_{h \to 0} \left[ f(x + h) \cdot \frac{g(x + h) - g(x)}{h} + g(x) \cdot \frac{f(x + h) - f(x)}{h} \right] \]
Since \( f \) and \( g \) are differentiable, we obtain
\[ F'(x) = f(x) \cdot g'(x) + g(x) \cdot f'(x) \]
We can state the product rule in Leibniz notation and give a geometric interpretation.
If \( y = uv \), where \( u \) and \( v \) are functions of \( x \), then
\[ \frac{dy}{dx} = u \frac{dv}{dx} + v \frac{du}{dx} \]
In the following figure, the white region represents \( y = uv \) and the shaded region \( \delta y \), as explained below.
\(\delta v\) \(u \delta v\) \( \delta u \delta v\)
\(v\) \(uv\) \(v \delta u\)
\(u\) \(\delta u\)
\(\delta y = (u + \delta u)(v + \delta v) - uv\)
\(= uv + v \delta u + u \delta v + \delta u \delta v - uv\)
\(= v \delta u + u \delta v + \delta u \delta v\)
\(\therefore \frac{\delta y}{\delta x} = v \frac{\delta u}{\delta x} + u \frac{\delta v}{\delta x} + \frac{\delta u}{\delta x} \frac{\delta v}{\delta x} \delta x\)
In the limit, as \(\delta x \to 0\), we have
\(\frac{\delta u}{\delta x} = \frac{du}{dx}, \quad \frac{\delta v}{\delta x} = \frac{dv}{dx}, \quad \text{and} \quad \frac{\delta y}{\delta x} = \frac{dy}{dx}\)
Therefore
\(\frac{dy}{dx} = v \frac{du}{dx} + u \frac{dv}{dx}\)