Applications of Derivatives

A structured guide to using derivatives for related rates, approximation, motion, extrema, the Mean Value Theorem, optimization, and tests for local behavior.

The Role of Derivatives

A derivative measures instantaneous change. Applications begin by translating a situation into a function or equation, differentiating carefully, and interpreting the result in context. The same core idea supports rate calculations, approximations, motion analysis, extreme-value problems, and .

A useful first question is: what quantity is changing, what variable measures the change, and what relationship connects the quantities? Units and signs are part of the mathematical answer, not merely final annotations.

Takeaway: Derivatives connect a changing model to a meaningful rate, estimate, direction, or extremum.

Related Rates

A involves quantities that change with respect to a common variable, usually time. If a variable depends on time, write it as a function such as r(t)r(t), and represent its rate by drdt\frac{dr}{dt}.

A reliable procedure

  1. Define every changing variable and assign units.

  2. Write the given rates and the unknown rate, preserving positive and negative signs.

  3. Find an equation relating the variables.

  4. Differentiate the equation with respect to time, applying the chain rule to every changing quantity.

  5. Substitute numerical values only after differentiating.

  6. Solve and state whether the result represents an increase or decrease.

For a circular ripple with area A=πr2A=\pi r^2, differentiation gives

dAdt=2πrdrdt.\frac{dA}{dt}=2\pi r\frac{dr}{dt}.

If r=5r=5 centimeters and drdt=2\frac{dr}{dt}=2 centimeters per second, then

dAdt=2π(5)(2)=20π cm2/s.\frac{dA}{dt}=2\pi(5)(2)=20\pi\text{ cm}^2/\text{s}.

The area is therefore increasing at 20π cm2/s20\pi\text{ cm}^2/\text{s}. If a radius decreases at 33 centimeters per second, use drdt=−3 cm/s\frac{dr}{dt}=-3\text{ cm}/\text{s}; the negative sign must remain in the calculation and interpretation.

Common relationships include

A=πr2,V=43πr3,V=πr2h,A=\pi r^2,\qquad V=\frac{4}{3}\pi r^3,\qquad V=\pi r^2h,

and

A=12bh,x2+y2=z2.A=\frac{1}{2}bh,\qquad x^2+y^2=z^2.

For example, differentiating V=43πr3V=\frac{4}{3}\pi r^3 gives dVdt=4πr2drdt\frac{dV}{dt}=4\pi r^2\frac{dr}{dt}, not merely 4πr24\pi r^2. The factor drdt\frac{dr}{dt} appears because rr changes with time.

Takeaway: Establish the relationship first, differentiate before substituting, and interpret the signed result with units.

Approximation and Differentials

uses the tangent line at a convenient point to approximate a function nearby. At x=ax=a, the approximation is

L(x)=f(a)+f′(a)(x−a),L(x)=f(a)+f'(a)(x-a),

so that f(x)≈L(x)f(x)\approx L(x) when xx is close to aa.

To estimate 4.1\sqrt{4.1}, choose f(x)=xf(x)=\sqrt{x} and a=4a=4. Then

f(4)=2,f′(x)=12x,f′(4)=14.f(4)=2,\qquad f'(x)=\frac{1}{2\sqrt{x}},\qquad f'(4)=\frac{1}{4}.

Thus,

L(x)=2+14(x−4),L(x)=2+\frac{1}{4}(x-4),

and

4.1≈L(4.1)=2+14(0.1)=2.025.\sqrt{4.1}\approx L(4.1)=2+\frac{1}{4}(0.1)=2.025.

The actual error is f(x)−L(x)f(x)-L(x). Accuracy generally improves when xx is close to aa, the function is differentiable nearby, and the graph has little curvature. For f(x)=xf(x)=\sqrt{x}, the graph is concave down, so the tangent-line approximation lies above the graph locally.

A expresses the same approximation in change notation. If y=f(x)y=f(x), then

dy=f′(x) dx.dy=f'(x)\,dx.

The actual change is Δy=f(x+Δx)−f(x)\Delta y=f(x+\Delta x)-f(x), and for a small change, Δy≈dy\Delta y\approx dy. Consequently,

f(a+dx)≈f(a)+f′(a) dx.f(a+dx)\approx f(a)+f'(a)\,dx.

For a sphere with V=43πr3V=\frac{4}{3}\pi r^3,

dV=4πr2 dr.dV=4\pi r^2\,dr.

At r=10r=10 centimeters and dr=0.02dr=0.02 centimeters,

dV=4π(10)2(0.02)=8π cm3.dV=4\pi(10)^2(0.02)=8\pi\text{ cm}^3.

The relative-error relationship is

dVV≈3drr,\frac{dV}{V}\approx 3\frac{dr}{r},

so a relative radius error of approximately 0.2%0.2\% produces a relative volume error of approximately 0.6%0.6\%.

Takeaway: approximates function values, while differentials approximate small changes and propagated measurement errors.

Motion Along a Line

For motion along a line, let s(t)s(t) denote position at time tt. The related quantities are

v(t)=s′(t),a(t)=v′(t)=s′′(t),speed=∣v(t)∣.v(t)=s'(t),\qquad a(t)=v'(t)=s''(t),\qquad \text{speed}=|v(t)|.

has a sign: v(t)>0v(t)>0 means motion in the positive direction, v(t)<0v(t)<0 means motion in the negative direction, and v(t)=0v(t)=0 means the object is instantaneously at rest. A change of direction requires a sign change in at a time when is zero or undefined.

Consider

s(t)=t3−6t2+9t,0≤t≤4.s(t)=t^3-6t^2+9t, \qquad 0\leq t\leq 4.

Its is

v(t)=3t2−12t+9=3(t−1)(t−3).v(t)=3t^2-12t+9=3(t-1)(t-3).

The critical times are t=1t=1 and t=3t=3. The sign of is positive on (0,1)(0,1), negative on (1,3)(1,3), and positive on (3,4)(3,4). Thus, the object changes direction at both t=1t=1 and t=3t=3.

Displacement is the net change in position,

s(4)−s(0),s(4)-s(0),

whereas total distance must account for reversals:

∣s(1)−s(0)∣+∣s(3)−s(1)∣+∣s(4)−s(3)∣.|s(1)-s(0)|+|s(3)-s(1)|+|s(4)-s(3)|.

Takeaway: Differentiate position to obtain , use signs to determine direction, and split distance calculations at direction changes.

Extreme Values and Derivative Tests

An absolute maximum is the greatest value on the entire domain, while an absolute minimum is the least value. A local maximum or minimum compares the function only with nearby values.

The Extreme Value Theorem guarantees both an absolute maximum and an absolute minimum when a function is continuous on a closed, bounded interval [a,b][a,b]. To find absolute extrema on such an interval:

  1. Find all critical numbers in (a,b)(a,b), where f′(x)=0f'(x)=0 or f′(x)f'(x) does not exist.

  2. Evaluate the function at every interior critical number.

  3. Evaluate the function at both endpoints.

  4. Compare all resulting values.

For

f(x)=x3−3x2+1f(x)=x^3-3x^2+1

on [0,3][0,3],

f′(x)=3x2−6x=3x(x−2).f'(x)=3x^2-6x=3x(x-2).

The interior critical number is x=2x=2. The relevant values are

f(0)=1,f(2)=−3,f(3)=1.f(0)=1,\qquad f(2)=-3,\qquad f(3)=1.

Therefore, the absolute minimum is −3-3 at x=2x=2, and the absolute maximum is 11 at both x=0x=0 and x=3x=3.

The uses the sign of f′f' around a critical number. A change from positive to negative gives a local maximum; a change from negative to positive gives a local minimum. The provides a shortcut when f′(c)=0f'(c)=0: f′′(c)>0f''(c)>0 indicates a local minimum, f′′(c)<0f''(c)<0 indicates a local maximum, and f′′(c)=0f''(c)=0 is inconclusive.

Takeaway: Critical numbers are candidates, not automatic extrema; absolute-extrema problems on closed intervals require endpoint comparisons.

The

The connects average and instantaneous rates. If ff is continuous on [a,b][a,b] and differentiable on (a,b)(a,b), then at least one number c∈(a,b)c\in(a,b) satisfies

f′(c)=f(b)−f(a)b−a.f'(c)=\frac{f(b)-f(a)}{b-a}.

The right side is the secant slope, or average rate of change, and f′(c)f'(c) is the tangent slope at an interior point.

For f(x)=x2f(x)=x^2 on [1,3][1,3], the average rate is

f(3)−f(1)3−1=9−12=4.\frac{f(3)-f(1)}{3-1}=\frac{9-1}{2}=4.

Since f′(x)=2xf'(x)=2x, the required point satisfies 2c=42c=4, so c=2c=2.

Rolle's Theorem is the special case in which f(a)=f(b)f(a)=f(b). Under the same continuity and differentiability conditions, there is a point c∈(a,b)c\in(a,b) where f′(c)=0f'(c)=0.

Important consequences include:

  • If f′(x)>0f'(x)>0 throughout an interval, then ff is increasing there.

  • If f′(x)<0f'(x)<0 throughout an interval, then ff is decreasing there.

  • If f′(x)=0f'(x)=0 throughout an interval, then ff is constant there.

  • If two functions have the same derivative on an interval, they differ by a constant on that interval.

Takeaway: The theorem turns derivative information into conclusions about average rates, monotonicity, and constancy, provided its hypotheses hold.

Problems

seeks the largest or smallest possible value of a quantity such as area, volume, cost, distance, time, or profit. A sound solution connects the real situation to a one-variable objective function.

General method

  1. Identify the quantity to maximize or minimize.

  2. Define variables and make a diagram when useful.

  3. Write the constraint equation.

  4. Use the constraint to express the objective in one variable.

  5. Determine the feasible domain from the physical restrictions.

  6. Find critical numbers by solving f′(x)=0f'(x)=0 and including points where f′f' is undefined.

  7. Check critical numbers and endpoints.

  8. State the result with units and in the original context.

For a rectangular garden with perimeter 4040 meters, let the dimensions be xx and yy. The constraint is

2x+2y=40,2x+2y=40,

so y=20−xy=20-x. The area becomes the one-variable objective

A(x)=x(20−x)=20x−x2,0≤x≤20.A(x)=x(20-x)=20x-x^2, \qquad 0\leq x\leq 20.

Differentiate and solve:

A′(x)=20−2x=0⟹x=10.A'(x)=20-2x=0 \quad\Longrightarrow\quad x=10.

Then y=20−10=10y=20-10=10. Since the objective is a downward-opening parabola, the maximum occurs for a 10 m×10 m10\text{ m}\times 10\text{ m} square, with area

A(10)=100 m2.A(10)=100\text{ m}^2.

A critical point is not automatically a maximum or minimum. Use a derivative sign chart, a derivative test, endpoint comparison, or direct comparison of objective values.

Takeaway: Translate the constraint into a feasible one-variable objective, then test every relevant candidate and interpret the result.