Math 355: Higher Derivatives and Derivatives of Trigonometric Functions

Page 1: Higher-Order Derivatives and Motion

Higher-Order Derivatives: Concept and Notations

When a function f(x)f(x) is differentiated, the resulting function f′(x)f'(x) is called the first derivative. Because f′(x)f'(x) is itself a function of xx, it can be differentiated again with respect to xx. The derivative of the first derivative is called the second derivative, denoted f′′(x)f''(x). Continuing this process yields higher-order derivatives.

Derivative Notations
  • First Derivative:

  f′(x)=dfdx=dydxf'(x) = \frac{df}{dx} = \frac{dy}{dx}

  • Second Derivative:

  f′′(x)=d2fdx2=d2ydx2f''(x) = \frac{d^2f}{dx^2} = \frac{d^2y}{dx^2}

  • Third Derivative:

  f′′′(x)=d3fdx3=d3ydx3f'''(x) = \frac{d^3f}{dx^3} = \frac{d^3y}{dx^3}

  • Fourth Derivative:

  To avoid an unwieldy number of prime tick marks, roman numerals or parenthesized integer exponents are used for derivatives of order four and higher:

  f(4)(x)=d4fdx4=d4ydx4f^{(4)}(x) = \frac{d^4f}{dx^4} = \frac{d^4y}{dx^4}

  • nn-th Derivative:

  For an arbitrary positive integer nn:

  f(n)(x)=dnfdxn=dnydxnf^{(n)}(x) = \frac{d^n f}{dx^n} = \frac{d^n y}{dx^n}


Example: Higher Derivatives of a Power Function

Consider the power function f(x)=xnf(x) = x^n, where nn is a positive integer.

Applying the power rule successively:

  • First derivative:

  f′(x)=nxn−1f'(x) = n x^{n-1}

  • Second derivative:

  f′′(x)=n(n−1)xn−2f''(x) = n(n-1) x^{n-2}

  • Third derivative:

  f′′′(x)=n(n−1)(n−2)xn−3f'''(x) = n(n-1)(n-2) x^{n-3}

  • General kk-th derivative (k≤nk \le n):

  f(k)(x)=n!(n−k)!xn−kf^{(k)}(x) = \frac{n!}{(n-k)!} x^{n-k}

  • nn-th derivative:

  f(n)(x)=n!f^{(n)}(x) = n!

  • (n+1)(n+1)-th derivative and beyond:

  f(n+1)(x)=0f^{(n+1)}(x) = 0


Kinematic Applications: Position, Velocity, and Acceleration

In rectilinear motion along a coordinate axis, higher derivatives provide descriptions of motion:

  • Position Function: s(t)s(t) represents the position of an object along a coordinate line relative to the origin at time tt.

  • Velocity Function: The instantaneous rate of change of position with respect to time represents velocity v(t)v(t), given by the first derivative:

  v(t)=s′(t)=dsdtv(t) = s'(t) = \frac{ds}{dt}

  • Acceleration Function: The instantaneous rate of change of velocity with respect to time represents acceleration a(t)a(t), given by the second derivative of position (or first derivative of velocity):

  a(t)=v′(t)=s′′(t)=d2sdt2a(t) = v'(t) = s''(t) = \frac{d^2s}{dt^2}

Example Problem: Motion of a Particle

Find the velocity and acceleration functions in terms of tt for the position function:

s(t)=t4−2ts(t) = t^4 - 2t

Step 1: Differentiate to find Velocity

v(t)=s′(t)=ddt(t4−2t)v(t) = s'(t) = \frac{d}{dt}(t^4 - 2t)

v(t)=4t3−2v(t) = 4t^3 - 2

Step 2: Differentiate again to find Acceleration

a(t)=v′(t)=s′′(t)=ddt(4t3−2)a(t) = v'(t) = s''(t) = \frac{d}{dt}(4t^3 - 2)

a(t)=12t2a(t) = 12t^2

Page 2: Projectile Motion Applications and Trigonometric Limits

Vertical Projectile Motion

Neglecting air resistance, the height hh (in meters) of an object launched vertically upward from the ground with an initial velocity v0v_0 is modeled by the kinematic formula:

h(t)=v0t−12gt2h(t) = v_0 t - \frac{1}{2} g t^2

Where:

  • g=9.81 m/s2g = 9.81\,m/s^2 is the acceleration due to Earth's gravity.

  • tt is the elapsed time in seconds since release (t≥0t \ge 0).

  • v0v_0 is the initial upward velocity at t=0t = 0.

Substituting g=9.81 m/s2g = 9.81\,m/s^2 into the position function gives:

h(t)=v0t−12(9.81)t2=v0t−4.905t2h(t) = v_0 t - \frac{1}{2}(9.81) t^2 = v_0 t - 4.905 t^2


Example Problem: Kinematic Analysis of a Projectile

Part a: Find the Velocity and Acceleration Functions
  • Velocity Function:

  v(t)=h′(t)=ddt(v0t−12gt2)=v0−gtv(t) = h'(t) = \frac{d}{dt}\left(v_0 t - \frac{1}{2} g t^2\right) = v_0 - g t

  Substituting g=9.81 m/s2g = 9.81\,m/s^2:

  v(t)=v0−9.81tv(t) = v_0 - 9.81 t

  • Acceleration Function:

  a(t)=v′(t)=h′′(t)=ddt(v0−gt)=−ga(t) = v'(t) = h''(t) = \frac{d}{dt}(v_0 - g t) = -g

  a(t)=−9.81 m/s2a(t) = -9.81\,m/s^2

  The acceleration is constant and directed downward toward the Earth.

Part b: Find the Time When the Velocity is Equal to 0

The velocity reaches zero at the peak of the trajectory (maximum height):

v(t)=0v(t) = 0

v0−gt=0v_0 - g t = 0

gt=v0g t = v_0

t=v0g=v09.81t = \frac{v_0}{g} = \frac{v_0}{9.81}

Part c: Time Interval When the Object is Traveling Upward

An object moves upward when its velocity is strictly positive (v(t)>0v(t) > 0):

v0−gt>0v_0 - g t > 0

t<v0gt < \frac{v_0}{g}

Since the release occurs at t=0t = 0, the time interval during which the object travels upward is:

[0,v0g)=[0,v09.81)\left[0, \frac{v_0}{g}\right) = \left[0, \frac{v_0}{9.81}\right)

Part d: Time Interval When the Object is Falling Downward

An object falls downward when its velocity is negative (v(t)<0v(t) < 0), continuing until it impacts the ground (h(t)=0h(t) = 0).

To find the impact time, solve for h(t)=0h(t) = 0:

v0t−12gt2=0v_0 t - \frac{1}{2} g t^2 = 0

t(v0−12gt)=0t\left(v_0 - \frac{1}{2} g t\right) = 0

  • t=0t = 0 (time of launch)

  • t=2v0gt = \frac{2v_0}{g} (time of landing)

Therefore, the object is falling downward during the time interval:

(v0g,2v0g]=(v09.81,2v09.81]\left(\frac{v_0}{g}, \frac{2v_0}{g}\right] = \left(\frac{v_0}{9.81}, \frac{2v_0}{9.81}\right]


Introduction to Derivatives of Trigonometric Functions

The fundamental rates of change for primary trigonometric functions are:

ddx(sin⁡(x))=cos⁡(x)\frac{d}{dx}(\sin(x)) = \cos(x)

ddx(cos⁡(x))=−sin⁡(x)\frac{d}{dx}(\cos(x)) = -\sin(x)

Essential Limits and Identities for Derivations

The formal proofs of these derivative formulas rely on two fundamental limits and angle addition identities:

  • Fundamental Trigonometric Limits:

  lim⁡x→0sin⁡(x)x=1\lim_{x \to 0} \frac{\sin(x)}{x} = 1

  lim⁡x→01−cos⁡(x)x=0\lim_{x \to 0} \frac{1 - \cos(x)}{x} = 0

  • Trigonometric Angle Sum Formulas:

  cos⁡(x+h)=cos⁡(x)cos⁡(h)−sin⁡(x)sin⁡(h)\cos(x + h) = \cos(x)\cos(h) - \sin(x)\sin(h)

  sin⁡(x+h)=sin⁡(x)cos⁡(h)+cos⁡(x)sin⁡(h)\sin(x + h) = \sin(x)\cos(h) + \cos(x)\sin(h)

Limit-Definition Proof of ddxsin⁡(x)\frac{d}{dx}\sin(x)

Using the definition of the derivative:

ddxsin⁡(x)=lim⁡h→0sin⁡(x+h)−sin⁡(x)h\frac{d}{dx}\sin(x) = \lim_{h \to 0} \frac{\sin(x + h) - \sin(x)}{h}

ddxsin⁡(x)=lim⁡h→0sin⁡(x)cos⁡(h)+cos⁡(x)sin⁡(h)−sin⁡(x)h\frac{d}{dx}\sin(x) = \lim_{h \to 0} \frac{\sin(x)\cos(h) + \cos(x)\sin(h) - \sin(x)}{h}

ddxsin⁡(x)=lim⁡h→0[sin⁡(x)(cos⁡(h)−1h)+cos⁡(x)(sin⁡(h)h)]\frac{d}{dx}\sin(x) = \lim_{h \to 0} \left[ \sin(x) \left(\frac{\cos(h) - 1}{h}\right) + \cos(x) \left(\frac{\sin(h)}{h}\right) \right]

ddxsin⁡(x)=sin⁡(x)(−lim⁡h→01−cos⁡(h)h)+cos⁡(x)(lim⁡h→0sin⁡(h)h)\frac{d}{dx}\sin(x) = \sin(x) \left( -\lim_{h \to 0} \frac{1 - \cos(h)}{h} \right) + \cos(x) \left(\lim_{h \to 0} \frac{\sin(h)}{h}\right)

ddxsin⁡(x)=sin⁡(x)(0)+cos⁡(x)(1)=cos⁡(x)\frac{d}{dx}\sin(x) = \sin(x)(0) + \cos(x)(1) = \cos(x)

Page 3: Graphical Relationships and Sine/Cosine Derivatives

Graphical Relationship Between Functions and Their Derivatives

Four-panel comparison of trigonometric functions and their successive derivatives
Successive Cyclic Differentiation

Differentiating sine and cosine repeatedly demonstrates a 4-step cyclic pattern:

  1. y=sin⁡(x)y = \sin(x)

  2. y′=cos⁡(x)y' = \cos(x)

  3. y′′=−sin⁡(x)y'' = -\sin(x)

  4. y′′′=−cos⁡(x)y''' = -\cos(x)

  5. y(4)=sin⁡(x)y^{(4)} = \sin(x)

Geometric Interpretation of the Graphs
  • Derivative of y=sin⁡(x)y = \sin(x) is y=cos⁡(x)y = \cos(x):

    • At x=0x = 0, the graph of sin⁡(x)\sin(x) passes through the origin with a slope of 11, corresponding to cos⁡(0)=1\cos(0) = 1.

    • At x=π2x = \frac{\pi}{2}, sin⁡(x)\sin(x) reaches a crest (horizontal tangent line with slope 00), corresponding to cos⁡(π2)=0\cos\left(\frac{\pi}{2}\right) = 0.

    • At x=πx = \pi, sin⁡(x)\sin(x) decreases with a slope of −1-1, corresponding to cos⁡(π)=−1\cos(\pi) = -1.

    • At x=3π2x = \frac{3\pi}{2}, sin⁡(x)\sin(x) reaches a trough (horizontal tangent line with slope 00), corresponding to cos⁡(3π2)=0\cos\left(\frac{3\pi}{2}\right) = 0.

  • Derivative of y=cos⁡(x)y = \cos(x) is y=−sin⁡(x)y = -\sin(x):

    • At x=0x = 0, cos⁡(x)\cos(x) has a horizontal tangent line with slope 00, matching −sin⁡(0)=0-\sin(0) = 0.

    • At x=π2x = \frac{\pi}{2}, cos⁡(x)\cos(x) crosses the horizontal axis with a downward slope of −1-1, matching −sin⁡(π2)=−1-\sin\left(\frac{\pi}{2}\right) = -1.

    • At x=πx = \pi, cos⁡(x)\cos(x) reaches its minimum with a slope of 00, matching −sin⁡(π)=0-\sin(\pi) = 0.

    • At x=3π2x = \frac{3\pi}{2}, cos⁡(x)\cos(x) crosses the horizontal axis with an upward slope of 11, matching −sin⁡(3π2)=−(−1)=1-\sin\left(\frac{3\pi}{2}\right) = -(-1) = 1.


Worked Examples

Example 1: Differentiating Linear Combinations with Constants

Find the derivative of:

f(x)=−4cos⁡(x)+sin⁡(π4)f(x) = -4\cos(x) + \sin\left(\frac{\pi}{4}\right)

Solution:
  • Differentiate −4cos⁡(x)-4\cos(x) with respect to xx:

  ddx[−4cos⁡(x)]=−4(−sin⁡(x))=4sin⁡(x)\frac{d}{dx}[-4\cos(x)] = -4(-\sin(x)) = 4\sin(x)

  • Notice that sin⁡(π4)=22\sin\left(\frac{\pi}{4}\right) = \frac{\sqrt{2}}{2} is a constant containing no variable xx. The derivative of any constant is 00:

  ddx[sin⁡(π4)]=0\frac{d}{dx}\left[\sin\left(\frac{\pi}{4}\right)\right] = 0

  • Combining the terms yields:

  f′(x)=4sin⁡(x)+0=4sin⁡(x)f'(x) = 4\sin(x) + 0 = 4\sin(x)

Example 2: Sine with a Polynomial Argument (Chain Rule)

Find the derivative of:

y=sin⁡(x2)y = \sin(x^2)

Solution:

Applying the Chain Rule, ddx[f(g(x))]=f′(g(x))⋅g′(x)\frac{d}{dx}[f(g(x))] = f'(g(x)) \cdot g'(x), where the outer function is f(u)=sin⁡(u)f(u) = \sin(u) and inner function is u=g(x)=x2u = g(x) = x^2:

dudx=2x\frac{du}{dx} = 2x

dydx=cos⁡(x2)⋅ddx(x2)\frac{dy}{dx} = \cos(x^2) \cdot \frac{d}{dx}(x^2)

dydx=2xcos⁡(x2)\frac{dy}{dx} = 2x\cos(x^2)

Example 3: Power of a Sine Function (Chain Rule)

Find the derivative of:

y=sin⁡2(x)=(sin⁡(x))2y = \sin^2(x) = (\sin(x))^2

Solution:

Applying the General Power Rule / Chain Rule, ddx[un]=nun−1⋅dudx\frac{d}{dx}[u^n] = n u^{n-1} \cdot \frac{du}{dx}, where u=sin⁡(x)u = \sin(x) and n=2n = 2:

dydx=2(sin⁡(x))2−1⋅ddx(sin⁡(x))\frac{dy}{dx} = 2(\sin(x))^{2-1} \cdot \frac{d}{dx}(\sin(x))

dydx=2sin⁡(x)cos⁡(x)\frac{dy}{dx} = 2\sin(x)\cos(x)

Using the double-angle identity sin⁡(2x)=2sin⁡(x)cos⁡(x)\sin(2x) = 2\sin(x)\cos(x), this can also be expressed as:

dydx=sin⁡(2x)\frac{dy}{dx} = \sin(2x)

Page 4: Derivatives of Other Trigonometric Functions and Complete Summary

Advanced Derivative Calculations

Example 4: Mixed Product and Chain Rule Expression

Find the derivative of:

y=x2sin⁡(3x)−cos⁡(5x)y = x^2 \sin(3x) - \cos(5x)

Solution:

Separate the expression into two distinct parts: y=u(x)−v(x)y = u(x) - v(x), where u(x)=x2sin⁡(3x)u(x) = x^2 \sin(3x) and v(x)=cos⁡(5x)v(x) = \cos(5x).

  • Differentiating u(x)=x2sin⁡(3x)u(x) = x^2 \sin(3x) via the Product Rule:

  ddx[x2sin⁡(3x)]=ddx[x2]⋅sin⁡(3x)+x2⋅ddx[sin⁡(3x)]\frac{d}{dx}[x^2 \sin(3x)] = \frac{d}{dx}[x^2] \cdot \sin(3x) + x^2 \cdot \frac{d}{dx}[\sin(3x)]

  By the Chain Rule, ddx[sin⁡(3x)]=cos⁡(3x)⋅3=3cos⁡(3x)\frac{d}{dx}[\sin(3x)] = \cos(3x) \cdot 3 = 3\cos(3x).

  ddx[u(x)]=2xsin⁡(3x)+3x2cos⁡(3x)\frac{d}{dx}[u(x)] = 2x\sin(3x) + 3x^2\cos(3x)

  • Differentiating v(x)=cos⁡(5x)v(x) = \cos(5x) via the Chain Rule:

  ddx[cos⁡(5x)]=−sin⁡(5x)⋅5=−5sin⁡(5x)\frac{d}{dx}[\cos(5x)] = -\sin(5x) \cdot 5 = -5\sin(5x)

  • Combining all components:

  dydx=(2xsin⁡(3x)+3x2cos⁡(3x))−(−5sin⁡(5x))\frac{dy}{dx} = \left(2x\sin(3x) + 3x^2\cos(3x)\right) - (-5\sin(5x))

  dydx=2xsin⁡(3x)+3x2cos⁡(3x)+5sin⁡(5x)\frac{dy}{dx} = 2x\sin(3x) + 3x^2\cos(3x) + 5\sin(5x)

Example 5: Derivation of the Derivative of tan⁡(x)\tan(x)

Find the derivative of y=tan⁡(x)y = \tan(x).

Solution:

Rewrite tan⁡(x)\tan(x) using the quotient definition tan⁡(x)=sin⁡(x)cos⁡(x)\tan(x) = \frac{\sin(x)}{\cos(x)} and apply the Quotient Rule:

ddx(uv)=u′v−uv′v2\frac{d}{dx}\left(\frac{u}{v}\right) = \frac{u'v - uv'}{v^2}

ddxtan⁡(x)=ddx[sin⁡(x)]⋅cos⁡(x)−sin⁡(x)⋅ddx[cos⁡(x)]cos⁡2(x)\frac{d}{dx}\tan(x) = \frac{\frac{d}{dx}[\sin(x)] \cdot \cos(x) - \sin(x) \cdot \frac{d}{dx}[\cos(x)]}{\cos^2(x)}

ddxtan⁡(x)=cos⁡(x)cos⁡(x)−sin⁡(x)(−sin⁡(x))cos⁡2(x)\frac{d}{dx}\tan(x) = \frac{\cos(x)\cos(x) - \sin(x)(-\sin(x))}{\cos^2(x)}

ddxtan⁡(x)=cos⁡2(x)+sin⁡2(x)cos⁡2(x)\frac{d}{dx}\tan(x) = \frac{\cos^2(x) + \sin^2(x)}{\cos^2(x)}

Applying the Pythagorean identity cos⁡2(x)+sin⁡2(x)=1\cos^2(x) + \sin^2(x) = 1:

ddxtan⁡(x)=1cos⁡2(x)=(1cos⁡(x))2=sec⁡2(x)\frac{d}{dx}\tan(x) = \frac{1}{\cos^2(x)} = \left(\frac{1}{\cos(x)}\right)^2 = \sec^2(x)

Example 6: Derivation of the Derivative of sec⁡(x)\sec(x)

Find the derivative of y=sec⁡(x)y = \sec(x).

Solution:

Rewrite sec⁡(x)\sec(x) as the reciprocal of cosine: sec⁡(x)=(cos⁡(x))−1\sec(x) = (\cos(x))^{-1}.

Apply the Chain Rule:

ddxsec⁡(x)=−1(cos⁡(x))−2⋅ddx[cos⁡(x)]\frac{d}{dx}\sec(x) = -1(\cos(x))^{-2} \cdot \frac{d}{dx}[\cos(x)]

ddxsec⁡(x)=−1cos⁡2(x)⋅(−sin⁡(x))\frac{d}{dx}\sec(x) = -\frac{1}{\cos^2(x)} \cdot (-\sin(x))

ddxsec⁡(x)=sin⁡(x)cos⁡2(x)\frac{d}{dx}\sec(x) = \frac{\sin(x)}{\cos^2(x)}

Factor the denominator to express using basic reciprocal functions:

ddxsec⁡(x)=1cos⁡(x)⋅sin⁡(x)cos⁡(x)=sec⁡(x)tan⁡(x)\frac{d}{dx}\sec(x) = \frac{1}{\cos(x)} \cdot \frac{\sin(x)}{\cos(x)} = \sec(x)\tan(x)


Summary of Basic Trigonometric Derivatives

Summary of derivatives of all six basic trigonometric functions
Complete List of Derivatives

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

ddxcos⁡(x)=−sin⁡(x)\frac{d}{dx}\cos(x) = -\sin(x)

ddxtan⁡(x)=sec⁡2(x)\frac{d}{dx}\tan(x) = \sec^2(x)

ddxcot⁡(x)=−csc⁡2(x)\frac{d}{dx}\cot(x) = -\csc^2(x)

ddxsec⁡(x)=sec⁡(x)⋅tan⁡(x)\frac{d}{dx}\sec(x) = \sec(x) \cdot \tan(x)

ddxcsc⁡(x)=−csc⁡(x)⋅cot⁡(x)\frac{d}{dx}\csc(x) = -\csc(x) \cdot \cot(x)

Structural Patterns to Note
  • Negative Signs on "Co-" Functions: The derivatives of all three co-functions (cos⁡(x)\cos(x), cot⁡(x)\cot(x), and csc⁡(x)\csc(x)) contain a negative sign.

  • Pairs of Functions:

    • Tangent maps to secant squared (sec⁡2(x)\sec^2(x)), whereas cotangent maps to negative cosecant squared (−csc⁡2(x)-\csc^2(x)).

    • Secant differentiates into the product of itself and tangent (sec⁡(x)tan⁡(x)\sec(x)\tan(x)), whereas cosecant differentiates into the negative product of itself and cotangent (−csc⁡(x)cot⁡(x)-\csc(x)\cot(x)).