Comprehensive Calculus Study Guide: Differentiation Rules, Chain Rule, Implicit Differentiation, and Related Rates

Fundamental Differentiation Rules

  • The Constant Rule

    • Theorem Statement: Let cc be any real constant. Then the derivative of cc with respect to xx is zero:     ddx(c)=0\frac{d}{dx}(c) = 0

    • Geometric Interpretation: The graph of a constant function y=cy = c is a horizontal straight line. Because the slope of any horizontal line is identically 00 everywhere, the instantaneous rate of change (derivative) is always 00.     

      Horizontal line graph showing constant function y = c with slope equal to zero
    • Worked Examples:

    • For f(x)=7f(x) = 7: f′(x)=ddx(7)=0f'(x) = \frac{d}{dx}(7) = 0.

    • For y=πy = \pi: dydx=ddx(π)=0\frac{dy}{dx} = \frac{d}{dx}(\pi) = 0.

    • For g(t)=e2g(t) = e^2: g′(t)=ddt(e2)=0g'(t) = \frac{d}{dt}(e^2) = 0.

    • For v=cos⁡(1)v = \cos(1): dvds=dds(cos⁡(1))=0\frac{dv}{ds} = \frac{d}{ds}(\cos(1)) = 0.

    • For f(x)=sin⁡(π2)f(x) = \sin\left(\frac{\pi}{2}\right): dfdx=ddx(sin⁡(π2))=0\frac{df}{dx} = \frac{d}{dx}\left(\sin\left(\frac{\pi}{2}\right)\right) = 0.

    • For y=eπ−52+2y = e^\pi - 5^2 + 2: Since every term is a constant real number, y′=0y' = 0.

    • For f(x)=cos⁡(3)−2+π2+ln⁡(7)f(x) = \cos(3) - 2 + \pi^2 + \ln(7): All constituent terms are constants, so f′(x)=0−0+0+0=0f'(x) = 0 - 0 + 0 + 0 = 0.

  • The Power Rule

    • Theorem Statement: Let nn be any real number. Then the derivative of the power function xnx^n with respect to xx is given by:     ddx(xn)=nxn−1\frac{d}{dx}(x^n) = n x^{n-1}

    • Worked Examples:

    • Differentiating a radical term ddx(x3)\frac{d}{dx}\left(\sqrt{x^3}\right): Rewrite as a rational exponent x3/2x^{3/2}, yielding ddx(x3/2)=32x(3/2)−1=32x1/2=32x\frac{d}{dx}\left(x^{3/2}\right) = \frac{3}{2} x^{(3/2) - 1} = \frac{3}{2} x^{1/2} = \frac{3}{2}\sqrt{x}.

    • For f(x)=x100f(x) = x^{100}: f′(x)=100x99f'(x) = 100 x^{99}.

    • For y=1x=x−1y = \frac{1}{x} = x^{-1}: dydx=(−1)x−1−1=−x−2=−1x2\frac{dy}{dx} = (-1)x^{-1-1} = -x^{-2} = -\frac{1}{x^2}.

    • For s(t)=1t3=t−3s(t) = \frac{1}{t^3} = t^{-3}: dsdt=−3t−3−1=−3t−4=−3t4\frac{ds}{dt} = -3 t^{-3-1} = -3 t^{-4} = -\frac{3}{t^4}.

    • For g(x)=x503=x50/3g(x) = \sqrt[3]{x^{50}} = x^{50/3}: g′(x)=503x(50/3)−1=503x47/3g'(x) = \frac{50}{3} x^{(50/3) - 1} = \frac{50}{3} x^{47/3}.

    • For y=xπy = x^\pi: dydx=πxπ−1\frac{dy}{dx} = \pi x^{\pi - 1}.

  • The Constant Multiple Rule

    • Theorem Statement: Let cc be a constant and ff be a differentiable function. Then:     ddx(cf(x))=cf′(x)\frac{d}{dx}(c f(x)) = c f'(x)

    • Application:

    • For y=2x4y = 2x^4: dydx=2⋅ddx(x4)=2(4x3)=8x3\frac{dy}{dx} = 2 \cdot \frac{d}{dx}(x^4) = 2(4x^3) = 8x^3.

  • The Sum and Difference Rule

    • Theorem Statement: Let ff and gg be differentiable functions. Then:     ddx(f(x)±g(x))=f′(x)±g′(x)\frac{d}{dx}(f(x) \pm g(x)) = f'(x) \pm g'(x)

    • Worked Examples with Algebraic Manipulation:

    • For s(r)=r5−3r3+r2−7s(r) = r^5 - 3r^3 + r^2 - 7: dsdr=5r4−9r2+2r\frac{ds}{dr} = 5r^4 - 9r^2 + 2r.

    • For y=x2(x−x3)y = x^2(x - x^3): Expand algebraically first to get y=x3−x5y = x^3 - x^5, then differentiate to obtain y′=3x2−5x4y' = 3x^2 - 5x^4.

    • For s(t)=t3/5+t−2/7s(t) = t^{3/5} + t^{-2/7}: dsdt=35t−2/5−27t−9/7\frac{ds}{dt} = \frac{3}{5}t^{-2/5} - \frac{2}{7}t^{-9/7}.

    • For f(y)=y+1y2f(y) = \frac{y + 1}{y^2}: Rewrite by splitting the fraction into y−1+y−2y^{-1} + y^{-2}, yielding f′(y)=−y−2−2y−3f'(y) = -y^{-2} - 2y^{-3}.

    • For f(x)=2x4+x3xf(x) = \frac{2x^4 + \sqrt{x}}{3x}: Split into individual terms and simplify exponents:       f(x)=2x43x+x1/23x=23x3+13x−1/2f(x) = \frac{2x^4}{3x} + \frac{x^{1/2}}{3x} = \frac{2}{3}x^3 + \frac{1}{3}x^{-1/2}       f′(x)=23(3x2)+13(−12)x−3/2=2x2−16x−3/2f'(x) = \frac{2}{3}(3x^2) + \frac{1}{3}\left(-\frac{1}{2}\right)x^{-3/2} = 2x^2 - \frac{1}{6}x^{-3/2}

    • For r(θ)=eθ+θ−2+θ4=eθ+θ−2+θ1/4r(\theta) = e^\theta + \theta^{-2} + \sqrt[4]{\theta} = e^\theta + \theta^{-2} + \theta^{1/4}: r′(θ)=eθ−2θ−3+14θ−3/4r'(\theta) = e^\theta - 2\theta^{-3} + \frac{1}{4}\theta^{-3/4}.

  • Exponential Derivatives

    • Theorem Statement: Let bb be a positive real number (b>0b > 0). Then:     ddx(bx)=bxln⁡(b)\frac{d}{dx}(b^x) = b^x \ln(b)

    • Natural Exponential Base (b=eb = e): Because ln⁡(e)=1\ln(e) = 1, the derivative simplifies to:     ddx(ex)=ex\frac{d}{dx}(e^x) = e^x

    • Worked Examples:

    • For y=2x+3x5=15(2x)+15(3x)y = \frac{2^x + 3^x}{5} = \frac{1}{5}(2^x) + \frac{1}{5}(3^x): dydx=15ln⁡(2)2x+15ln⁡(3)3x\frac{dy}{dx} = \frac{1}{5}\ln(2) 2^x + \frac{1}{5}\ln(3) 3^x.

    • For g(t)=e2t−et3etg(t) = \frac{e^{2t} - e^t}{3e^t}: Simplify using exponent rules:       g(t)=e2t3et−et3et=13e2t−t−13et−t=13et−13g(t) = \frac{e^{2t}}{3e^t} - \frac{e^t}{3e^t} = \frac{1}{3}e^{2t - t} - \frac{1}{3}e^{t - t} = \frac{1}{3}e^t - \frac{1}{3}       g′(t)=13et−0=13etg'(t) = \frac{1}{3}e^t - 0 = \frac{1}{3}e^t

  • Physical Kinematic Application: Position, Velocity, and Acceleration

    • Definitions: Given position s(t)s(t), instantaneous velocity is v(t)=s′(t)=dsdtv(t) = s'(t) = \frac{ds}{dt}, and instantaneous acceleration is a(t)=v′(t)=s′′(t)=dvdta(t) = v'(t) = s''(t) = \frac{dv}{dt}.

    • Full Derivation Example: Let position be s(t)=3t85+5t=3t8/5+5ts(t) = 3\sqrt[5]{t^8} + 5^t = 3t^{8/5} + 5^t.

    • Instantaneous Velocity:       v(t)=s′(t)=3⋅ddt(t8/5)+ddt(5t)v(t) = s'(t) = 3 \cdot \frac{d}{dt}\left(t^{8/5}\right) + \frac{d}{dt}\left(5^t\right)       v(t)=3(85)t3/5+5tln⁡(5)=245t3/5+5tln⁡(5)v(t) = 3\left(\frac{8}{5}\right)t^{3/5} + 5^t \ln(5) = \frac{24}{5}t^{3/5} + 5^t \ln(5)

    • Instantaneous Acceleration:       a(t)=v′(t)=245⋅ddt(t3/5)+ln⁡(5)⋅ddt(5t)a(t) = v'(t) = \frac{24}{5} \cdot \frac{d}{dt}\left(t^{3/5}\right) + \ln(5) \cdot \frac{d}{dt}\left(5^t\right)       a(t)=245(35)t−2/5+ln⁡(5)(5tln⁡(5))=7225t−2/5+5tln⁡2(5)a(t) = \frac{24}{5}\left(\frac{3}{5}\right)t^{-2/5} + \ln(5)\left(5^t \ln(5)\right) = \frac{72}{25}t^{-2/5} + 5^t \ln^2(5)

The Chain Rule

  • Theorem Formulation

    • Lagrange (Prime) Notation: If gg is differentiable at xx and ff is differentiable at g(x)g(x), then the composite function F=f∘gF = f \circ g, defined by F(x)=f(g(x))F(x) = f(g(x)), is differentiable at xx, and its derivative is:     F′(x)=f′(g(x))⋅g′(x)F'(x) = f'(g(x)) \cdot g'(x)

    • Leibniz Notation: If y=f(u)y = f(u) and u=g(x)u = g(x) are both differentiable functions, then:     dydx=dfdu⋅dudx=dydu⋅dudx\frac{dy}{dx} = \frac{df}{du} \cdot \frac{du}{dx} = \frac{dy}{du} \cdot \frac{du}{dx}

    • Intuition via Differentials: Treating Leibniz derivatives as formal ratios reveals the visual cancellation of intermediate differential terms:     dydx=dydu⋅dudx\frac{dy}{dx} = \frac{dy}{du} \cdot \frac{du}{dx}

    • Multi-Layer Chain Rule Extension: When composing three or more functions, such as y=f(g(h(x)))y = f(g(h(x))), or across intermediate variables u,v,wu, v, w:     ddx[f(g(h(x)))]=f′(g(h(x)))⋅g′(h(x))⋅h′(x)\frac{d}{dx}[f(g(h(x)))] = f'(g(h(x))) \cdot g'(h(x)) \cdot h'(x)     dydx=dydu⋅dudv⋅dvdw⋅dwdx\frac{dy}{dx} = \frac{dy}{du} \cdot \frac{du}{dv} \cdot \frac{dv}{dw} \cdot \frac{dw}{dx}

  • Algebraic and Transcendental Worked Examples

    • Polynomial Composite Power: For h(x)=(x2+2x)3h(x) = (x^2 + 2x)^3:

    • Outer function: f(u)=u3f(u) = u^3 with u=g(x)=x2+2xu = g(x) = x^2 + 2x.

    • Outer derivative: f′(u)=3u2=3(x2+2x)2f'(u) = 3u^2 = 3(x^2 + 2x)^2.

    • Inner derivative: g′(x)=2x+2g'(x) = 2x + 2.

    • Final derivative: h′(x)=3(x2+2x)2⋅(2x+2)h'(x) = 3(x^2 + 2x)^2 \cdot (2x + 2).

    • Trigonometric Power: For y=sin⁡2(x)=(sin⁡(x))2y = \sin^2(x) = (\sin(x))^2:

    • Inner function: u=sin⁡(x)u = \sin(x); outer function: y=u2y = u^2.

    • Component derivatives: dydu=2u\frac{dy}{du} = 2u, dudx=cos⁡(x)\frac{du}{dx} = \cos(x).

    • Combined derivative: dydx=2ucos⁡(x)=2sin⁡(x)cos⁡(x)\frac{dy}{dx} = 2u \cos(x) = 2\sin(x)\cos(x).

    • Trigonometric Argument Composite: For f(x)=sin⁡(3x)f(x) = \sin(3x):

    • f′(x)=cos⁡(3x)⋅ddx(3x)=3cos⁡(3x)f'(x) = \cos(3x) \cdot \frac{d}{dx}(3x) = 3\cos(3x).

    • High-Order Polynomial Composite: For g(x)=(x2+1)100g(x) = (x^2 + 1)^{100}:

    • g′(x)=100(x2+1)99⋅ddx(x2+1)=100(x2+1)99(2x)=200x(x2+1)99g'(x) = 100(x^2 + 1)^{99} \cdot \frac{d}{dx}(x^2 + 1) = 100(x^2 + 1)^{99}(2x) = 200x(x^2 + 1)^{99}.

    • Three-Layer Composite with Exponential and Secant: For y=sec⁡(e5x)y = \sec(e^{5x}):

    • Layer 1 (outer): sec⁡(u)\sec(u), derivative is sec⁡(u)tan⁡(u)\sec(u)\tan(u).

    • Layer 2 (middle): u=evu = e^v, derivative is eve^v.

    • Layer 3 (inner): v=5xv = 5x, derivative is 55.

    • Step-by-step differentiation:       dydx=sec⁡(e5x)tan⁡(e5x)⋅ddx(e5x)\frac{dy}{dx} = \sec(e^{5x})\tan(e^{5x}) \cdot \frac{d}{dx}\left(e^{5x}\right)       dydx=sec⁡(e5x)tan⁡(e5x)⋅e5x⋅ddx(5x)=5e5xsec⁡(e5x)tan⁡(e5x)\frac{dy}{dx} = \sec(e^{5x})\tan(e^{5x}) \cdot e^{5x} \cdot \frac{d}{dx}(5x) = 5 e^{5x} \sec(e^{5x})\tan(e^{5x})

    • Nested Radicals with Tangent: For g(u)=u+u+tan⁡(u)=[u+(u+tan⁡(u))1/2]1/2g(u) = \sqrt{u + \sqrt{u + \tan(u)}} = \left[u + (u + \tan(u))^{1/2}\right]^{1/2}.

    • First outer differentiation:       g′(u)=12[u+u+tan⁡(u)]−1/2⋅ddu(u+[u+tan⁡(u)]1/2)g'(u) = \frac{1}{2}\left[u + \sqrt{u + \tan(u)}\right]^{-1/2} \cdot \frac{d}{du}\left(u + [u + \tan(u)]^{1/2}\right)

    • Inner expression differentiation:       ddu(u+[u+tan⁡(u)]1/2)=1+12[u+tan⁡(u)]−1/2⋅ddu(u+tan⁡(u))\frac{d}{du}\left(u + [u + \tan(u)]^{1/2}\right) = 1 + \frac{1}{2}[u + \tan(u)]^{-1/2} \cdot \frac{d}{du}(u + \tan(u))

    • Innermost differentiation: ddu(u+tan⁡(u))=1+sec⁡2(u)\frac{d}{du}(u + \tan(u)) = 1 + \sec^2(u).

    • Fully assembled derivative:       g′(u)=12[u+u+tan⁡(u)]−1/2⋅[1+12[u+tan⁡(u)]−1/2(1+sec⁡2(u))]g'(u) = \frac{1}{2}\left[u + \sqrt{u + \tan(u)}\right]^{-1/2} \cdot \left[1 + \frac{1}{2}[u + \tan(u)]^{-1/2}\left(1 + \sec^2(u)\right)\right]

    • Power of Tangent with Rational Exponential Argument: For s(t)=tan⁡2(2t+1t)s(t) = \tan^2\left(\frac{2^t + 1}{t}\right).

    • Outer derivative: 2tan⁡(2t+1t)2\tan\left(\frac{2^t + 1}{t}\right).

    • Middle derivative: sec⁡2(2t+1t)\sec^2\left(\frac{2^t + 1}{t}\right).

    • Inner derivative via Quotient Rule on 2t+1t\frac{2^t + 1}{t}:       ddt(2t+1t)=t⋅ddt(2t+1)−(2t+1)⋅ddt(t)t2=t(2tln⁡(2))−(2t+1)(1)t2\frac{d}{dt}\left(\frac{2^t + 1}{t}\right) = \frac{t \cdot \frac{d}{dt}(2^t + 1) - (2^t + 1) \cdot \frac{d}{dt}(t)}{t^2} = \frac{t(2^t \ln(2)) - (2^t + 1)(1)}{t^2}

    • Combined derivative:       s′(t)=2tan⁡(2t+1t)sec⁡2(2t+1t)[t2tln⁡(2)−2t−1t2]s'(t) = 2\tan\left(\frac{2^t + 1}{t}\right) \sec^2\left(\frac{2^t + 1}{t}\right) \left[\frac{t 2^t \ln(2) - 2^t - 1}{t^2}\right]

  • Graphical and Tabular Evaluation of Composite Derivatives

    • Piecewise Linear Graphical Example: Let h(x)=f(x3−1)h(x) = f(x^3 - 1), where ff is defined by the following graph:     

      Piecewise linear graph of y = f(x) with linear segments passing through (0,0), reaching a vertex at (2,1), and descending through (3,-1)
    • Differentiating h(x)h(x) using the Chain Rule:       h′(x)=f′(x3−1)⋅ddx(x3−1)=f′(x3−1)⋅3x2h'(x) = f'(x^3 - 1) \cdot \frac{d}{dx}(x^3 - 1) = f'(x^3 - 1) \cdot 3x^2

    • Evaluating at x=1x = 1:       h′(1)=f′(13−1)⋅3(1)2=f′(0)⋅3h'(1) = f'(1^3 - 1) \cdot 3(1)^2 = f'(0) \cdot 3

    • Determining f′(0)f'(0): The value f′(0)f'(0) represents the slope of the tangent line to f(x)f(x) at x=0x = 0. From the graph, f(x)f(x) is a straight line segment on the interval [−2,2][-2, 2] connecting (−2,−1)(-2, -1), (0,0)(0, 0), and (2,1)(2, 1). The slope is:       m=1−02−0=12m = \frac{1 - 0}{2 - 0} = \frac{1}{2}

    • Final calculation:       h′(1)=12⋅3=32h'(1) = \frac{1}{2} \cdot 3 = \frac{3}{2}

    • Tabular Values Example: Let ff and gg be differentiable functions with values provided in the reference table:     

      Table containing values for x, f(x), f'(x), g(x), g'(x), and g''(x) at x = 0, 1, 2
    • Values from the table:

      • At x=0x = 0: f(0)=1f(0) = 1, f′(0)=−4f'(0) = -4, g(0)=2g(0) = 2, g′(0)=−6g'(0) = -6, g′′(0)=0g''(0) = 0.

      • At x=1x = 1: f(1)=1f(1) = 1, f′(1)=4f'(1) = 4, g(1)=−3g(1) = -3, g′(1)=−3g'(1) = -3, g′′(1)=6g''(1) = 6.

      • At x=2x = 2: f(2)=9f(2) = 9, f′(2)=12f'(2) = 12, g(2)=−2g(2) = -2, g′(2)=6g'(2) = 6, g′′(2)=12g''(2) = 12.

    • Problem: Let K(x)=g(f(x)+ex−1)K(x) = g(f(x) + e^{x-1}). Find K′(1)K'(1).

    • Differentiating K(x)K(x) via Chain Rule:       K′(x)=g′(f(x)+ex−1)⋅ddx(f(x)+ex−1)=g′(f(x)+ex−1)⋅[f′(x)+ex−1]K'(x) = g'(f(x) + e^{x-1}) \cdot \frac{d}{dx}\left(f(x) + e^{x-1}\right) = g'(f(x) + e^{x-1}) \cdot \left[f'(x) + e^{x-1}\right]

    • Evaluating at x=1x = 1:       K′(1)=g′(f(1)+e1−1)⋅[f′(1)+e1−1]=g′(f(1)+e0)⋅[f′(1)+e0]K'(1) = g'(f(1) + e^{1-1}) \cdot \left[f'(1) + e^{1-1}\right] = g'(f(1) + e^0) \cdot \left[f'(1) + e^0\right]       K′(1)=g′(1+1)⋅[4+1]=g′(2)⋅5=6⋅5=30K'(1) = g'(1 + 1) \cdot [4 + 1] = g'(2) \cdot 5 = 6 \cdot 5 = 30

    • Multi-Function Graphical Analysis:     

      Graph displaying curves f and g with discontinuities and piecewise linear segments
    • Evaluating derivatives at x=1x = 1:

      • For ddx[x+g(x)f(2x+1)]\frac{d}{dx}\left[\frac{x + g(x)}{f(2x + 1)}\right]: Apply the Quotient Rule in conjunction with the Chain Rule on the denominator:         [1+g′(x)]f(2x+1)−[x+g(x)]⋅f′(2x+1)⋅2[f(2x+1)]2\frac{[1 + g'(x)] f(2x + 1) - [x + g(x)] \cdot f'(2x + 1) \cdot 2}{[f(2x + 1)]^2}         Evaluate at x=1x = 1 using function values and slopes from the graph at x=1x = 1 and 2x+1=32x+1 = 3.

      • For ddx[g(f(3x+1))+4x−g2(x)]\frac{d}{dx}\left[g(f(3x + 1)) + 4^x - g^2(x)\right]: Apply the Chain Rule across all terms:         g′(f(3x+1))⋅f′(3x+1)⋅3+4xln⁡(4)−2g(x)g′(x)g'(f(3x + 1)) \cdot f'(3x + 1) \cdot 3 + 4^x \ln(4) - 2g(x)g'(x)         Evaluate at x=1x = 1 using coordinates and tangent slopes from the graph.

  • Recognizing Derivative Limits via the Chain Rule

    • Problem: Evaluate the limit:     lim⁡x→0sin⁡((3+x)2)−sin⁡(9)x\lim_{x \to 0} \frac{\sin((3 + x)^2) - \sin(9)}{x}

    • Limit Definition Formulation: Recall the limit definition of the derivative at a point aa:     f′(a)=lim⁡h→0f(a+h)−f(a)hf'(a) = \lim_{h \to 0} \frac{f(a + h) - f(a)}{h}

    • Structural Identification: Replacing the variable name xx with hh:     lim⁡h→0sin⁡((3+h)2)−sin⁡(32)h\lim_{h \to 0} \frac{\sin((3 + h)^2) - \sin(3^2)}{h}     This matches the definition of f′(a)f'(a) with function f(t)=sin⁡(t2)f(t) = \sin(t^2) evaluated at a=3a = 3.

    • Evaluation via Differentiation: Differentiating f(t)=sin⁡(t2)f(t) = \sin(t^2) using the Chain Rule:     f′(t)=cos⁡(t2)⋅ddt(t2)=2tcos⁡(t2)f'(t) = \cos(t^2) \cdot \frac{d}{dt}(t^2) = 2t \cos(t^2)

    • Final Value:     f′(3)=2(3)cos⁡(32)=6cos⁡(9)f'(3) = 2(3) \cos(3^2) = 6\cos(9)     Therefore, lim⁡x→0sin⁡((3+x)2)−sin⁡(9)x=6cos⁡(9)\lim_{x \to 0} \frac{\sin((3 + x)^2) - \sin(9)}{x} = 6\cos(9).

Implicit Differentiation

  • Implicit vs. Explicit Functions

    • Explicit Functions: A function is explicit when the dependent variable yy is isolated directly on one side in terms of the independent variable xx:     y=f(x)y = f(x)

    • Examples: y=x3+1y = \sqrt{x^3 + 1} and y=xsin⁡(x)y = x\sin(x).

    • Implicit Functions: An equation defines a function implicitly when the relationship between xx and yy is expressed as a combined relation where yy is not explicitly solved:

    • Examples: x2+y2=25x^2 + y^2 = 25 and x3+y3=6xyx^3 + y^3 = 6xy.

    • Multi-Branch Explicit Representation: Solving an implicit equation explicitly may require multiple equations to satisfy the vertical line test.

    • Consider the unit circle x2+y2=1x^2 + y^2 = 1:       y2=1−x2  ⟹  y=±1−x2y^2 = 1 - x^2 \implies y = \pm\sqrt{1 - x^2}

    • The complete relation is not a single function because it fails the vertical line test:       

      Complete circle x^2 + y^2 = 1 failing vertical line test
    • It must be decomposed into two distinct explicit functions:       {+1−x2when y≥0−1−x2when y<0\begin{cases} +\sqrt{1 - x^2} & \text{when } y \ge 0 \\ -\sqrt{1 - x^2} & \text{when } y < 0 \end{cases}       

      Upper semicircle y = +sqrt(1 - x^2)

            

      Lower semicircle y = -sqrt(1 - x^2)
    • Drawback of Explicit Conversion: Solving for yy explicitly often produces cumbersome square roots requiring separate differentiations, which becomes intractable or impossible for higher-degree polynomials (such as x3+y3=6xyx^3 + y^3 = 6xy).

  • The Implicit Differential Operator Technique

    • Expanding the Differential Operator: The differential operator ddx\frac{d}{dx} can be viewed as multiplying by one via the chain rule differential ratio:     ddx≈ddy⋅dydx\frac{d}{dx} \approx \frac{d}{dy} \cdot \frac{dy}{dx}

    • Fundamental Rule for Differentiating Expressions Containing yy: When differentiating an expression involving yy with respect to xx, differentiate with respect to yy first, then multiply by dydx\frac{dy}{dx} (or y′y'):     ddx[g(y)]=ddy[g(y)]⋅dydx=g′(y)y′\frac{d}{dx}[g(y)] = \frac{d}{dy}[g(y)] \cdot \frac{dy}{dx} = g'(y) y'

    • Basic Derivative Demonstrations:

    • ddx(y2)=ddy(y2)dydx=2ydydx=2yy′\frac{d}{dx}(y^2) = \frac{d}{dy}(y^2) \frac{dy}{dx} = 2y \frac{dy}{dx} = 2y y'

    • ddx(y3)=ddy(y3)dydx=3y2dydx=3y2y′\frac{d}{dx}(y^3) = \frac{d}{dy}(y^3) \frac{dy}{dx} = 3y^2 \frac{dy}{dx} = 3y^2 y'

    • ddx(cos⁡(y))=ddy(cos⁡(y))dydx=−sin⁡(y)dydx=−sin⁡(y)y′\frac{d}{dx}(\cos(y)) = \frac{d}{dy}(\cos(y)) \frac{dy}{dx} = -\sin(y) \frac{dy}{dx} = -\sin(y) y'

    • ddx(y2/3)=ddy(y2/3)dydx=23y−1/3dydx=23y−1/3y′\frac{d}{dx}(y^{2/3}) = \frac{d}{dy}(y^{2/3}) \frac{dy}{dx} = \frac{2}{3}y^{-1/3} \frac{dy}{dx} = \frac{2}{3}y^{-1/3} y'

  • Algorithmic Step-by-Step Procedure

    • Step 1: Apply the differentiation operator ddx\frac{d}{dx} to both sides of the equation.

    • Step 2: Differentiate each term, applying the Product, Quotient, and Chain Rules as necessary, appending y′y' whenever differentiating a term involving yy.

    • Step 3: Collect all terms containing y′y' on one side of the equation and move all terms without y′y' to the opposite side.

    • Step 4: Factor out y′y' as a common factor.

    • Step 5: Divide by the remaining coefficient factor to solve explicitly for y′y'.

  • Comprehensive Implicit Differentiation Examples

    • Example 1: The Circle x2+y2=25x^2 + y^2 = 25     ddx(x2+y2)=ddx(25)\frac{d}{dx}(x^2 + y^2) = \frac{d}{dx}(25)     ddx(x2)+ddx(y2)=0\frac{d}{dx}(x^2) + \frac{d}{dx}(y^2) = 0     2x+2yy′=02x + 2y y' = 0     2yy′=−2x2y y' = -2x     y′=−2x2y=−xyy' = -\frac{2x}{2y} = -\frac{x}{y}

    • Example 2: Folium of Descartes x3+y3=6xyx^3 + y^3 = 6xy     ddx(x3+y3)=ddx(6xy)\frac{d}{dx}(x^3 + y^3) = \frac{d}{dx}(6xy)     3x2+3y2y′=6(ddx(x)⋅y+x⋅ddx(y))3x^2 + 3y^2 y' = 6\left(\frac{d}{dx}(x) \cdot y + x \cdot \frac{d}{dx}(y)\right)     3x2+3y2y′=6(1⋅y+xy′)=6y+6xy′3x^2 + 3y^2 y' = 6(1 \cdot y + x y') = 6y + 6x y'     3y2y′−6xy′=6y−3x23y^2 y' - 6x y' = 6y - 3x^2     y′(3y2−6x)=6y−3x2y'(3y^2 - 6x) = 6y - 3x^2     y′=6y−3x23y2−6x=3(2y−x2)3(y2−2x)=2y−x2y2−2xy' = \frac{6y - 3x^2}{3y^2 - 6x} = \frac{3(2y - x^2)}{3(y^2 - 2x)} = \frac{2y - x^2}{y^2 - 2x}

    • Example 3: Mixed Trigonometric and Product Relation sin⁡(x+y)=y2cos⁡(x)\sin(x + y) = y^2 \cos(x)     ddx[sin⁡(x+y)]=ddx[y2cos⁡(x)]\frac{d}{dx}[\sin(x + y)] = \frac{d}{dx}[y^2 \cos(x)]     cos⁡(x+y)⋅(1+y′)=(ddx(y2))cos⁡(x)+y2(ddx(cos⁡(x)))\cos(x + y) \cdot (1 + y') = \left(\frac{d}{dx}(y^2)\right)\cos(x) + y^2\left(\frac{d}{dx}(\cos(x))\right)     cos⁡(x+y)+y′cos⁡(x+y)=2yy′cos⁡(x)−y2sin⁡(x)\cos(x + y) + y' \cos(x + y) = 2y y' \cos(x) - y^2 \sin(x)     cos⁡(x+y)+y2sin⁡(x)=2yy′cos⁡(x)−y′cos⁡(x+y)\cos(x + y) + y^2 \sin(x) = 2y y' \cos(x) - y' \cos(x + y)     cos⁡(x+y)+y2sin⁡(x)=y′[2ycos⁡(x)−cos⁡(x+y)]\cos(x + y) + y^2 \sin(x) = y'[2y \cos(x) - \cos(x + y)]     y′=cos⁡(x+y)+y2sin⁡(x)2ycos⁡(x)−cos⁡(x+y)y' = \frac{\cos(x + y) + y^2 \sin(x)}{2y \cos(x) - \cos(x + y)}

    • Example 4: Second Derivative of x4+y4=16x^4 + y^4 = 16

    • Find y′y' first:       ddx(x4+y4)=ddx(16)\frac{d}{dx}(x^4 + y^4) = \frac{d}{dx}(16)       4x3+4y3y′=0  ⟹  4y3y′=−4x3  ⟹  y′=−x3y34x^3 + 4y^3 y' = 0 \implies 4y^3 y' = -4x^3 \implies y' = -\frac{x^3}{y^3}

    • Differentiate y′y' with respect to xx using the Quotient Rule:       y′′=ddx(−x3y3)=−(ddx(x3))y3−x3(ddx(y3))(y3)2y'' = \frac{d}{dx}\left(-\frac{x^3}{y^3}\right) = -\frac{\left(\frac{d}{dx}(x^3)\right)y^3 - x^3\left(\frac{d}{dx}(y^3)\right)}{(y^3)^2}       y′′=−3x2y3−x3(3y2y′)y6=−3x2y3−3x3y2y′y6y'' = -\frac{3x^2 y^3 - x^3 (3y^2 y')}{y^6} = -\frac{3x^2 y^3 - 3x^3 y^2 y'}{y^6}

    • Substitute y′=−x3y3y' = -\frac{x^3}{y^3} into the second derivative expression:       y′′=−3x2y3−3x3y2(−x3y3)y6=−3x2y3+3x6y2y3y6=−3x2y3+3x6yy6y'' = -\frac{3x^2 y^3 - 3x^3 y^2 \left(-\frac{x^3}{y^3}\right)}{y^6} = -\frac{3x^2 y^3 + \frac{3x^6 y^2}{y^3}}{y^6} = -\frac{3x^2 y^3 + \frac{3x^6}{y}}{y^6}       y′′=−3x2y4+3x6y7=−3x2(y4+x4)y7y'' = -\frac{3x^2 y^4 + 3x^6}{y^7} = -\frac{3x^2(y^4 + x^4)}{y^7}

    • Simplify using the original constraint x4+y4=16x^4 + y^4 = 16:       y′′=−3x2(16)y7=−48x2y7y'' = -\frac{3x^2(16)}{y^7} = -\frac{48x^2}{y^7}

    • Example 5: Second-Degree Polynomial Curve x2−4xy+y2=4x^2 - 4xy + y^2 = 4     ddx(x2−4xy+y2)=ddx(4)\frac{d}{dx}(x^2 - 4xy + y^2) = \frac{d}{dx}(4)     2x−4(1⋅y+xy′)+2yy′=02x - 4(1 \cdot y + x y') + 2y y' = 0     2x−4y−4xy′+2yy′=02x - 4y - 4x y' + 2y y' = 0     −4xy′+2yy′=4y−2x-4x y' + 2y y' = 4y - 2x     y′(−4x+2y)=4y−2xy'(-4x + 2y) = 4y - 2x     y′=4y−2x−4x+2y=2(2y−x)2(−2x+y)=2y−xy−2xy' = \frac{4y - 2x}{-4x + 2y} = \frac{2(2y - x)}{2(-2x + y)} = \frac{2y - x}{y - 2x}

    • Example 6: Quartic Implicit Curve x4+x2y2+y3=5x^4 + x^2 y^2 + y^3 = 5     ddx(x4+x2y2+y3)=ddx(5)\frac{d}{dx}(x^4 + x^2 y^2 + y^3) = \frac{d}{dx}(5)     4x3+(2xy2+x2(2yy′))+3y2y′=04x^3 + \left(2x y^2 + x^2 (2y y')\right) + 3y^2 y' = 0     4x3+2xy2+2x2yy′+3y2y′=04x^3 + 2x y^2 + 2x^2 y y' + 3y^2 y' = 0     y′(2x2y+3y2)=−4x3−2xy2y'(2x^2 y + 3y^2) = -4x^3 - 2x y^2     y′=−4x3−2xy22x2y+3y2y' = \frac{-4x^3 - 2x y^2}{2x^2 y + 3y^2}

    • Example 7: Linear and Trigonometric Mix sin⁡(x)+cos⁡(y)=2x−3y\sin(x) + \cos(y) = 2x - 3y     ddx(sin⁡(x)+cos⁡(y))=ddx(2x−3y)\frac{d}{dx}(\sin(x) + \cos(y)) = \frac{d}{dx}(2x - 3y)     cos⁡(x)−sin⁡(y)y′=2−3y′\cos(x) - \sin(y)y' = 2 - 3y'     3y′−sin⁡(y)y′=2−cos⁡(x)3y' - \sin(y)y' = 2 - \cos(x)     y′(3−sin⁡(y))=2−cos⁡(x)y'(3 - \sin(y)) = 2 - \cos(x)     y′=2−cos⁡(x)3−sin⁡(y)=cos⁡(x)−2sin⁡(y)−3y' = \frac{2 - \cos(x)}{3 - \sin(y)} = \frac{\cos(x) - 2}{\sin(y) - 3}

    • Example 8: Coupled Exponential Terms 2xey+yex=32x e^y + y e^x = 3     ddx(2xey+yex)=ddx(3)\frac{d}{dx}(2x e^y + y e^x) = \frac{d}{dx}(3)     (2ey+2xeyy′)+(y′ex+yex)=0\left(2 e^y + 2x e^y y'\right) + \left(y' e^x + y e^x\right) = 0     2xeyy′+y′ex=−2ey−yex2x e^y y' + y' e^x = -2e^y - y e^x     y′(2xey+ex)=−(2ey+yex)y'(2x e^y + e^x) = -(2e^y + y e^x)     y′=−(2ey+yex)2xey+ex=−2ey+yex2xey+exy' = \frac{-(2e^y + y e^x)}{2x e^y + e^x} = -\frac{2e^y + y e^x}{2x e^y + e^x}

Introduction to Related Rates and Problem-Solving Strategy

  • Core Conceptual Foundation

    • Definition: In a related rates problem, physical or geometric quantities that change over time tt are connected through an governing equation. The instantaneous rate of change of one or more quantities is provided, and the objective is to determine the unknown instantaneous rate of change of another quantity at a specific instant.

    • Mathematical Representation: All rates of change are modeled as derivatives with respect to time tt (ddt\frac{d}{dt}), treating every time-dependent variable as an implicit function of time: x=x(t)x = x(t), y=y(t)y = y(t), r=r(t)r = r(t), V=V(t)V = V(t), A=A(t)A = A(t).

  • The Systematic 7-Step Strategy

    • Step 1: Draw and label a diagram. Identify the geometric setup, assign variables to all dynamic quantities that vary with time, and assign constants to dimensions that remain strictly fixed.

    • Step 2: Identify known rates and known values. Express all given quantitative information as numerical values or time derivatives (e.g., dxdt=500 mph\frac{dx}{dt} = 500\,\text{mph}).

    • Step 3: Identify the unknown rate. Explicitly state the derivative sought (e.g., dzdt=?\frac{dz}{dt} = ?) and specify the precise instant of evaluation (e.g., when z=2 milesz = 2\,\text{miles}).

    • Step 4: Write an equation relating the variables. Connect the parameters using geometric, trigonometric, or physical formulas (e.g., Pythagorean theorem, volume, area, similar triangles). Ensure the relation contains only relevant variables.

    • Step 5: Differentiate implicitly with respect to tt. Apply ddt\frac{d}{dt} across the equation, using the Chain Rule to attach time derivative factors (such as dxdt\frac{dx}{dt}, dydt\frac{dy}{dt}) to each variable.

    • Step 6: Substitute known values. Substitute the instantaneous measurements and rates into the differentiated equation. Critical rule: Never substitute instantaneous values prior to differentiating, as doing so erroneously treats dynamic variables as constants.

    • Step 7: Solve and include units. Algebraically isolate the desired derivative rate and append proper dimensional units (e.g., cm2/s\text{cm}^2/\text{s}, ft/s\text{ft/s}, cm/min\text{cm/min}).

  • Fundamental Geometric Rate Applications

    • Expanding Square Problem:

    • Geometry: Area of a square of side length ss is A=s2A = s^2.

    • Given: Side length expands at dsdt=6 cm/s\frac{ds}{dt} = 6\,\text{cm/s}.

    • Instant: Find dAdt\frac{dA}{dt} when area A=16 cm2A = 16\,\text{cm}^2.

    • Intermediate Value: s=16=4 cms = \sqrt{16} = 4\,\text{cm}.

    • Implicit Differentiation with respect to tt:       dAdt=2sdsdt\frac{dA}{dt} = 2s \frac{ds}{dt}

    • Substitution and Solution:       dAdt=2(4 cm)(6 cm/s)=48 cm2/s\frac{dA}{dt} = 2(4\,\text{cm})(6\,\text{cm/s}) = 48\,\text{cm}^2/\text{s}

    • Inflating Spherical Balloon Problem:

    • Geometry: Volume of a sphere of radius rr is V=43πr3V = \frac{4}{3}\pi r^3.

    • Given: Air is pumped into the balloon at a constant rate of dVdt=100 cm3/min\frac{dV}{dt} = 100\,\text{cm}^3/\text{min}.

    • Instant: Find the rate of increase of the radius, drdt\frac{dr}{dt}, when radius r=5 cmr = 5\,\text{cm}.

    • Implicit Differentiation with respect to tt:       dVdt=43π(3r2drdt)=4πr2drdt\frac{dV}{dt} = \frac{4}{3}\pi\left(3r^2 \frac{dr}{dt}\right) = 4\pi r^2 \frac{dr}{dt}

    • Substitution and Solution:       100=4π(5)2drdt=100πdrdt100 = 4\pi (5)^2 \frac{dr}{dt} = 100\pi \frac{dr}{dt}       drdt=100100π=1π cm/min\frac{dr}{dt} = \frac{100}{100\pi} = \frac{1}{\pi}\,\text{cm/min}

    • Deflating Spherical Balloon Problem:

    • Geometry: Surface area of a sphere is A=4πr2A = 4\pi r^2; diameter is D=2rD = 2r.

    • Given: Surface area decreases at a rate of dAdt=−1 cm2/min\frac{dA}{dt} = -1\,\text{cm}^2/\text{min}.

    • Instant: Find the rate of decrease of the diameter, dDdt\frac{dD}{dt}, when diameter D=10 cmD = 10\,\text{cm} (r=5 cmr = 5\,\text{cm}).

    • Differentiating Surface Area with respect to tt:       dAdt=8πrdrdt\frac{dA}{dt} = 8\pi r \frac{dr}{dt}

    • Solving for drdt\frac{dr}{dt}:       −1=8π(5)drdt=40πdrdt  ⟹  drdt=−140π cm/min-1 = 8\pi(5) \frac{dr}{dt} = 40\pi \frac{dr}{dt} \implies \frac{dr}{dt} = -\frac{1}{40\pi}\,\text{cm/min}

    • Differentiating Diameter relation D=2rD = 2r:       dDdt=2drdt=2(−140π)=−120π cm/min\frac{dD}{dt} = 2 \frac{dr}{dt} = 2\left(-\frac{1}{40\pi}\right) = -\frac{1}{20\pi}\,\text{cm/min}

    • Conclusion: The diameter decreases at a rate of 120π cm/min\frac{1}{20\pi}\,\text{cm/min}.

    • Expanding Cube Problem:

    • Geometry: Volume of a cube of edge length xx is V=x3V = x^3.

    • Given: Edge length expands at dxdt=4 cm/s\frac{dx}{dt} = 4\,\text{cm/s}.

    • Instant: Find dVdt\frac{dV}{dt} when x=15 cmx = 15\,\text{cm}.

    • Implicit Differentiation with respect to tt:       dVdt=3x2dxdt\frac{dV}{dt} = 3x^2 \frac{dx}{dt}

    • Substitution and Solution:       dVdt=3(15)2(4)=3(225)(4)=2700 cm3/s\frac{dV}{dt} = 3(15)^2(4) = 3(225)(4) = 2700\,\text{cm}^3/\text{s}

    • Abstract Multi-Variable Function Rate Problem:

    • Given Equation: y=3x4+6xy = 3x^4 + 6x.

    • Rates and State: x=1x = 1, dxdt=−3\frac{dx}{dt} = -3. Find dydt\frac{dy}{dt}.

    • Differentiating with respect to tt:       dydt=12x3dxdt+6dxdt\frac{dy}{dt} = 12x^3 \frac{dx}{dt} + 6 \frac{dx}{dt}

    • Substitution:       dydt=12(1)3(−3)+6(−3)=−36−18=−54\frac{dy}{dt} = 12(1)^3(-3) + 6(-3) = -36 - 18 = -54

Advanced Related Rates Applications

  • Pythagorean Models: Radar Tracking of an Aircraft

    • Physical Setup: An airplane flies horizontally at a constant altitude of 1 mile1\,\text{mile} at a constant ground speed of 500 mph500\,\text{mph}. The plane passes directly over a ground radar tracking station.     

      Right triangle diagram for radar tracking of an airplane at altitude 1 mile with direct distance z and horizontal distance x
    • Identification of Parameters:

    • Altitude: y=1 miley = 1\,\text{mile} (constant, so dydt=0\frac{dy}{dt} = 0\,mph).

    • Horizontal distance: xx, with horizontal velocity dxdt=500 mph\frac{dx}{dt} = 500\,\text{mph}.

    • Direct distance to station: zz.

    • Instant: z=2 milesz = 2\,\text{miles}.

    • Geometric Evaluation of xx:     x2+y2=z2  ⟹  x2+12=22  ⟹  x2=3  ⟹  x=3 milesx^2 + y^2 = z^2 \implies x^2 + 1^2 = 2^2 \implies x^2 = 3 \implies x = \sqrt{3}\,\text{miles}

    • Implicit Differentiation with respect to tt:     ddt(x2+y2)=ddt(z2)\frac{d}{dt}(x^2 + y^2) = \frac{d}{dt}(z^2)     2xdxdt+2ydydt=2zdzdt  ⟹  xdxdt+ydydt=zdzdt2x \frac{dx}{dt} + 2y \frac{dy}{dt} = 2z \frac{dz}{dt} \implies x \frac{dx}{dt} + y \frac{dy}{dt} = z \frac{dz}{dt}

    • Substitution and Solution:     3(500)+1(0)=2dzdt\sqrt{3}(500) + 1(0) = 2 \frac{dz}{dt}     5003=2dzdt  ⟹  dzdt=2503 mph500\sqrt{3} = 2 \frac{dz}{dt} \implies \frac{dz}{dt} = 250\sqrt{3}\,\text{mph}

    • Conclusion: The direct line-of-sight distance between the aircraft and the radar station is increasing at an instantaneous rate of 2503 mph250\sqrt{3}\,\text{mph}.

  • Pythagorean Models: Sliding Ladder

    • Physical Setup: A ladder of fixed length 10 ft10\,\text{ft} leans against a vertical wall. The base of the ladder slides outward along the horizontal floor at a rate of dxdt=2 ft/s\frac{dx}{dt} = 2\,\text{ft/s}.     

      Diagram of a 10 ft ladder leaning against a wall, forming a right triangle with base x and height y
    • Part 1: Downward Velocity of the Ladder Top

    • Identification of Parameters: Ladder length z=10 ftz = 10\,\text{ft} (constant, so dzdt=0 ft/s\frac{dz}{dt} = 0\,\text{ft/s}), horizontal distance x=6 ftx = 6\,\text{ft}, dxdt=2 ft/s\frac{dx}{dt} = 2\,\text{ft/s}.

    • Evaluation of Vertical Height yy:       x2+y2=z2  ⟹  62+y2=102  ⟹  36+y2=100  ⟹  y=8 ftx^2 + y^2 = z^2 \implies 6^2 + y^2 = 10^2 \implies 36 + y^2 = 100 \implies y = 8\,\text{ft}

    • Implicit Differentiation with respect to tt:       2xdxdt+2ydydt=2zdzdt  ⟹  xdxdt+ydydt=02x \frac{dx}{dt} + 2y \frac{dy}{dt} = 2z \frac{dz}{dt} \implies x \frac{dx}{dt} + y \frac{dy}{dt} = 0

    • Solving for dydt\frac{dy}{dt}:       (6)(2)+8dydt=0  ⟹  12+8dydt=0(6)(2) + 8 \frac{dy}{dt} = 0 \implies 12 + 8 \frac{dy}{dt} = 0       dydt=−128=−32 ft/s\frac{dy}{dt} = -\frac{12}{8} = -\frac{3}{2}\,\text{ft/s}

    • Conclusion: The top of the ladder is sliding down the wall at a speed of 32 ft/s\frac{3}{2}\,\text{ft/s} (rate of change is −32 ft/s-\frac{3}{2}\,\text{ft/s}).

    • Part 2: Rate of Angular Change with Respect to the Floor

    • Identification of Parameters: Let θ\theta be the interior angle formed between the ladder and the horizontal ground.       

      Diagram of the ladder with angle theta between ladder and ground
    • Trigonometric Relationship: cos⁡(θ)=xz\cos(\theta) = \frac{x}{z}.

    • Differentiating implicitly with respect to tt via the Quotient Rule:       −sin⁡(θ)dθdt=zdxdt−xdzdtz2-\sin(\theta) \frac{d\theta}{dt} = \frac{z \frac{dx}{dt} - x \frac{dz}{dt}}{z^2}

    • Solving for dθdt\frac{d\theta}{dt} using 1sin⁡(θ)=zy\frac{1}{\sin(\theta)} = \frac{z}{y}:       dθdt=−zdxdt−xdzdtz2⋅zy=−zdxdt−xdzdtzy\frac{d\theta}{dt} = -\frac{z \frac{dx}{dt} - x \frac{dz}{dt}}{z^2} \cdot \frac{z}{y} = -\frac{z \frac{dx}{dt} - x \frac{dz}{dt}}{z y}

    • Using fixed ladder length z=10z = 10, dzdt=0\frac{dz}{dt} = 0, y=8y = 8, and given values:       dθdt=−(10)(2)−0(10)(8)=−2080=−14 rad/s\frac{d\theta}{dt} = -\frac{(10)(2) - 0}{(10)(8)} = -\frac{20}{80} = -\frac{1}{4}\,\text{rad/s}

    • Verification with alternate recorded numerator substitution −(4)(2)−(10)(0)/[(10)(8)]-(4)(2) - (10)(0) / [(10)(8)]: Yields −880=−25 rad/s-\frac{8}{80} = -\frac{2}{5}\,\text{rad/s}.

  • Pythagorean Models: Vehicles Departing an Intersection

    • Physical Setup: Two vehicles diverge from an intersection simultaneously. Car A travels East at 30 mph30\,\text{mph}, and Car B travels North at 40 mph40\,\text{mph}.     

      Right triangle formed by Car A traveling East along the x-axis and Car B traveling North along the y-axis
    • Identification of Parameters:

    • Position East: x=3 milesx = 3\,\text{miles}, with rate dxdt=30 mph\frac{dx}{dt} = 30\,\text{mph}.

    • Position North: y=4 milesy = 4\,\text{miles}, with rate dydt=40 mph\frac{dy}{dt} = 40\,\text{mph}.

    • Separation distance: zz.

    • Evaluation of Separation Distance zz:     z=x2+y2=32+42=9+16=5 milesz = \sqrt{x^2 + y^2} = \sqrt{3^2 + 4^2} = \sqrt{9 + 16} = 5\,\text{miles}

    • Implicit Differentiation and Solution:     z2=x2+y2  ⟹  2zdzdt=2xdxdt+2ydydtz^2 = x^2 + y^2 \implies 2z \frac{dz}{dt} = 2x \frac{dx}{dt} + 2y \frac{dy}{dt}     dzdt=xdxdt+ydydtz\frac{dz}{dt} = \frac{x \frac{dx}{dt} + y \frac{dy}{dt}}{z}     dzdt=(3)(30)+(4)(40)5=90+1605=2505=50 mph\frac{dz}{dt} = \frac{(3)(30) + (4)(40)}{5} = \frac{90 + 160}{5} = \frac{250}{5} = 50\,\text{mph}

    • Conclusion: The distance between the two vehicles is increasing at a rate of 50 mph50\,\text{mph}.

  • Similar Triangle Models: Streetlight and Shadow

    • Physical Setup: A streetlamp is mounted atop a 15 ft15\,\text{ft} pole. A man of height 6 ft6\,\text{ft} walks directly away from the pole along a level path at a speed of 5 ft/s5\,\text{ft/s}.     

      Similar triangles diagram showing 15 ft pole, 6 ft man, distance x from pole, and shadow length y
    • Identification of Parameters:

    • Distance from pole to man: xx, with dxdt=5 ft/s\frac{dx}{dt} = 5\,\text{ft/s}.

    • Length of the man's shadow: yy.

    • Total distance from pole to tip of shadow: x+yx + y.

    • Geometric Equation via Similar Triangles:     6y=15x+y\frac{6}{y} = \frac{15}{x + y}     15y=6(x+y)=6x+6y15y = 6(x + y) = 6x + 6y     9y=6x  ⟹  y=23x9y = 6x \implies y = \frac{2}{3}x

    • Rate of Change of Shadow Length (dydt\frac{dy}{dt}):     dydt=23dxdt=23(5)=103 ft/s\frac{dy}{dt} = \frac{2}{3} \frac{dx}{dt} = \frac{2}{3}(5) = \frac{10}{3}\,\text{ft/s}

    • Rate of Motion of the Tip of the Shadow: The location of the shadow tip relative to the base of the lamppost is x+yx + y. Its rate of motion is given by:     ddt(x+y)=dxdt+dydt=5+103=153+103=253 ft/s\frac{d}{dt}(x + y) = \frac{dx}{dt} + \frac{dy}{dt} = 5 + \frac{10}{3} = \frac{15}{3} + \frac{10}{3} = \frac{25}{3}\,\text{ft/s}

    • Conclusion: The tip of the shadow is moving along the ground at an instantaneous rate of 253 ft/s\frac{25}{3}\,\text{ft/s}, independent of the man's distance from the pole.

  • Similar Triangle Models: Ground Spotlight and Wall Shadow

    • Physical Setup: A ground-level spotlight shines toward a vertical building wall located 12 m12\,\text{m} away. A man of height 2 m2\,\text{m} walks from the light directly toward the building at a speed of 1.6 m/s1.6\,\text{m/s}.     

      Similar triangle diagram of a person of height 2 m walking toward a wall 12 m away from a spotlight
    • Identification of Parameters:

    • Distance from spotlight to man: xx, with dxdt=1.6 m/s=85 m/s\frac{dx}{dt} = 1.6\,\text{m/s} = \frac{8}{5}\,\text{m/s}.

    • Distance between spotlight and wall: Fixed at 12 m12\,\text{m}.

    • Height of shadow cast on the building: yy.

    • Instant: When the man is 4 m4\,\text{m} from the building, his distance from the spotlight is x=12−4=8 mx = 12 - 4 = 8\,\text{m}.

    • Geometric Relationship via Similar Triangles:     2x=y12  ⟹  y=24x=24x−1\frac{2}{x} = \frac{y}{12} \implies y = \frac{24}{x} = 24 x^{-1}

    • Implicit Differentiation with respect to tt:     dydt=−24x2dxdt\frac{dy}{dt} = -\frac{24}{x^2} \frac{dx}{dt}

    • Substitution and Solution at x=8 mx = 8\,\text{m}:     dydt=−2482(1.6)=−2464(85)=−38(85)=−35 m/s=−0.6 m/s\frac{dy}{dt} = -\frac{24}{8^2}(1.6) = -\frac{24}{64}\left(\frac{8}{5}\right) = -\frac{3}{8}\left(\frac{8}{5}\right) = -\frac{3}{5}\,\text{m/s} = -0.6\,\text{m/s}

    • Conclusion: The height of the man's shadow on the wall is decreasing at an instantaneous rate of 35 m/s\frac{3}{5}\,\text{m/s} (or −0.6 m/s-0.6\,\text{m/s}).

  • Volume and Similar Triangle Models: Inverted Conical Reservoir

    • Physical Setup: An inverted circular conical water tank has a total height of H=6 m=600 cmH = 6\,\text{m} = 600\,\text{cm} and a top radius of R=2 m=200 cmR = 2\,\text{m} = 200\,\text{cm}. Water leaks out from the bottom apex at a constant rate of Rateout=10,000 cm3/min\text{Rate}_{\text{out}} = 10{,}000\,\text{cm}^3/\text{min} while water is simultaneously pumped in at an unknown constant rate Ratein\text{Rate}_{\text{in}}.     

      Inverted cone showing water height h, water radius r, and leaking volumetric outflow
    • Identification of Parameters:

    • Water level height: h=2 m=200 cmh = 2\,\text{m} = 200\,\text{cm}.

    • Rate of water level rise: dhdt=20 cm/min\frac{dh}{dt} = 20\,\text{cm/min}.

    • Volume of a circular cone: V=13πr2hV = \frac{1}{3}\pi r^2 h.

    • Eliminating Radius rr via Similar Triangles:     rh=RH=200600=13  ⟹  r=h3\frac{r}{h} = \frac{R}{H} = \frac{200}{600} = \frac{1}{3} \implies r = \frac{h}{3}

    • Expressing Volume Solely as a Function of hh:     V=13π(h3)2h=13π(h29)h=π27h3V = \frac{1}{3}\pi \left(\frac{h}{3}\right)^2 h = \frac{1}{3}\pi \left(\frac{h^2}{9}\right) h = \frac{\pi}{27} h^3

    • Implicit Differentiation with respect to tt:     dVdt=π27(3h2dhdt)=π9h2dhdt\frac{dV}{dt} = \frac{\pi}{27}\left(3h^2 \frac{dh}{dt}\right) = \frac{\pi}{9} h^2 \frac{dh}{dt}

    • Evaluating Net Rate of Volume Change at h=200 cmh = 200\,\text{cm}:     dVdt=π9(200)2(20)=π9(40,000)(20)=800,000π9 cm3/min\frac{dV}{dt} = \frac{\pi}{9} (200)^2 (20) = \frac{\pi}{9} (40{,}000)(20) = \frac{800{,}000\pi}{9}\,\text{cm}^3/\text{min}

    • Relating Net Volume Change to Inflow and Outflow:     dVdt=Ratein−Rateout\frac{dV}{dt} = \text{Rate}_{\text{in}} - \text{Rate}_{\text{out}}     Ratein=dVdt+Rateout\text{Rate}_{\text{in}} = \frac{dV}{dt} + \text{Rate}_{\text{out}}     Ratein=800,000π9+10,000 cm3/min\text{Rate}_{\text{in}} = \frac{800{,}000\pi}{9} + 10{,}000\,\text{cm}^3/\text{min}

    • Conclusion: Water is being pumped into the inverted conical reservoir at an exact rate of (800,000π9+10,000) cm3/min\left(\frac{800{,}000\pi}{9} + 10{,}000\right)\,\text{cm}^3/\text{min}.