Page 1: Higher-Order Derivatives and Motion
Higher-Order Derivatives: Concept and Notations
When a function f(x) is differentiated, the resulting function f′(x) is called the first derivative. Because f′(x) is itself a function of x, it can be differentiated again with respect to x. The derivative of the first derivative is called the second derivative, denoted f′′(x). Continuing this process yields higher-order derivatives.
Derivative Notations
f′(x)=dxdf=dxdy
f′′(x)=dx2d2f=dx2d2y
f′′′(x)=dx3d3f=dx3d3y
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)=dx4d4f=dx4d4y
For an arbitrary positive integer n:
f(n)(x)=dxndnf=dxndny
Example: Higher Derivatives of a Power Function
Consider the power function f(x)=xn, where n is a positive integer.
Applying the power rule successively:
f′(x)=nxn−1
f′′(x)=n(n−1)xn−2
f′′′(x)=n(n−1)(n−2)xn−3
f(k)(x)=(n−k)!n!xn−k
f(n)(x)=n!
f(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) represents the position of an object along a coordinate line relative to the origin at time t.
Velocity Function: The instantaneous rate of change of position with respect to time represents velocity v(t), given by the first derivative:
v(t)=s′(t)=dtds
a(t)=v′(t)=s′′(t)=dt2d2s
Example Problem: Motion of a Particle
Find the velocity and acceleration functions in terms of t for the position function:
s(t)=t4−2t
Step 1: Differentiate to find Velocity
v(t)=s′(t)=dtd(t4−2t)
v(t)=4t3−2
Step 2: Differentiate again to find Acceleration
a(t)=v′(t)=s′′(t)=dtd(4t3−2)
a(t)=12t2
Page 2: Projectile Motion Applications and Trigonometric Limits
Vertical Projectile Motion
Neglecting air resistance, the height h (in meters) of an object launched vertically upward from the ground with an initial velocity v0 is modeled by the kinematic formula:
h(t)=v0t−21gt2
Where:
g=9.81m/s2 is the acceleration due to Earth's gravity.
t is the elapsed time in seconds since release (t≥0).
v0 is the initial upward velocity at t=0.
Substituting g=9.81m/s2 into the position function gives:
h(t)=v0t−21(9.81)t2=v0t−4.905t2
Example Problem: Kinematic Analysis of a Projectile
Part a: Find the Velocity and Acceleration Functions
v(t)=h′(t)=dtd(v0t−21gt2)=v0−gt
Substituting g=9.81m/s2:
v(t)=v0−9.81t
a(t)=v′(t)=h′′(t)=dtd(v0−gt)=−g
a(t)=−9.81m/s2
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)=0
v0−gt=0
gt=v0
t=gv0=9.81v0
Part c: Time Interval When the Object is Traveling Upward
An object moves upward when its velocity is strictly positive (v(t)>0):
v0−gt>0
t<gv0
Since the release occurs at t=0, the time interval during which the object travels upward is:
[0,gv0)=[0,9.81v0)
Part d: Time Interval When the Object is Falling Downward
An object falls downward when its velocity is negative (v(t)<0), continuing until it impacts the ground (h(t)=0).
To find the impact time, solve for h(t)=0:
v0t−21gt2=0
t(v0−21gt)=0
Therefore, the object is falling downward during the time interval:
(gv0,g2v0]=(9.81v0,9.812v0]
Introduction to Derivatives of Trigonometric Functions
The fundamental rates of change for primary trigonometric functions are:
dxd(sin(x))=cos(x)
dxd(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:
limx→0xsin(x)=1
limx→0x1−cos(x)=0
cos(x+h)=cos(x)cos(h)−sin(x)sin(h)
sin(x+h)=sin(x)cos(h)+cos(x)sin(h)
Limit-Definition Proof of dxdsin(x)
Using the definition of the derivative:
dxdsin(x)=limh→0hsin(x+h)−sin(x)
dxdsin(x)=limh→0hsin(x)cos(h)+cos(x)sin(h)−sin(x)
dxdsin(x)=limh→0[sin(x)(hcos(h)−1)+cos(x)(hsin(h))]
dxdsin(x)=sin(x)(−limh→0h1−cos(h))+cos(x)(limh→0hsin(h))
dxdsin(x)=sin(x)(0)+cos(x)(1)=cos(x)
Page 3: Graphical Relationships and Sine/Cosine Derivatives
Graphical Relationship Between Functions and Their Derivatives

Successive Cyclic Differentiation
Differentiating sine and cosine repeatedly demonstrates a 4-step cyclic pattern:
y=sin(x)
y′=cos(x)
y′′=−sin(x)
y′′′=−cos(x)
y(4)=sin(x)
Geometric Interpretation of the Graphs
Worked Examples
Example 1: Differentiating Linear Combinations with Constants
Find the derivative of:
f(x)=−4cos(x)+sin(4π)
Solution:
dxd[−4cos(x)]=−4(−sin(x))=4sin(x)
dxd[sin(4π)]=0
f′(x)=4sin(x)+0=4sin(x)
Example 2: Sine with a Polynomial Argument (Chain Rule)
Find the derivative of:
y=sin(x2)
Solution:
Applying the Chain Rule, dxd[f(g(x))]=f′(g(x))⋅g′(x), where the outer function is f(u)=sin(u) and inner function is u=g(x)=x2:
dxdu=2x
dxdy=cos(x2)⋅dxd(x2)
dxdy=2xcos(x2)
Example 3: Power of a Sine Function (Chain Rule)
Find the derivative of:
y=sin2(x)=(sin(x))2
Solution:
Applying the General Power Rule / Chain Rule, dxd[un]=nun−1⋅dxdu, where u=sin(x) and n=2:
dxdy=2(sin(x))2−1⋅dxd(sin(x))
dxdy=2sin(x)cos(x)
Using the double-angle identity sin(2x)=2sin(x)cos(x), this can also be expressed as:
dxdy=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)
Solution:
Separate the expression into two distinct parts: y=u(x)−v(x), where u(x)=x2sin(3x) and v(x)=cos(5x).
dxd[x2sin(3x)]=dxd[x2]⋅sin(3x)+x2⋅dxd[sin(3x)]
By the Chain Rule, dxd[sin(3x)]=cos(3x)⋅3=3cos(3x).
dxd[u(x)]=2xsin(3x)+3x2cos(3x)
dxd[cos(5x)]=−sin(5x)⋅5=−5sin(5x)
dxdy=(2xsin(3x)+3x2cos(3x))−(−5sin(5x))
dxdy=2xsin(3x)+3x2cos(3x)+5sin(5x)
Example 5: Derivation of the Derivative of tan(x)
Find the derivative of y=tan(x).
Solution:
Rewrite tan(x) using the quotient definition tan(x)=cos(x)sin(x) and apply the Quotient Rule:
dxd(vu)=v2u′v−uv′
dxdtan(x)=cos2(x)dxd[sin(x)]⋅cos(x)−sin(x)⋅dxd[cos(x)]
dxdtan(x)=cos2(x)cos(x)cos(x)−sin(x)(−sin(x))
dxdtan(x)=cos2(x)cos2(x)+sin2(x)
Applying the Pythagorean identity cos2(x)+sin2(x)=1:
dxdtan(x)=cos2(x)1=(cos(x)1)2=sec2(x)
Example 6: Derivation of the Derivative of sec(x)
Find the derivative of y=sec(x).
Solution:
Rewrite sec(x) as the reciprocal of cosine: sec(x)=(cos(x))−1.
Apply the Chain Rule:
dxdsec(x)=−1(cos(x))−2⋅dxd[cos(x)]
dxdsec(x)=−cos2(x)1⋅(−sin(x))
dxdsec(x)=cos2(x)sin(x)
Factor the denominator to express using basic reciprocal functions:
dxdsec(x)=cos(x)1⋅cos(x)sin(x)=sec(x)tan(x)
Summary of Basic Trigonometric Derivatives

Complete List of Derivatives
dxdsin(x)=cos(x)
dxdcos(x)=−sin(x)
dxdtan(x)=sec2(x)
dxdcot(x)=−csc2(x)
dxdsec(x)=sec(x)⋅tan(x)
dxdcsc(x)=−csc(x)⋅cot(x)
Structural Patterns to Note