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7.4 Area Under Curves & First-Order Differential Equations

Key Takeaways

  • The definite integral evaluates signed net area; computing the physical geometric area bounded by y=f(x)y = f(x) and the xx-axis requires partitioning at roots to integrate absolute magnitudes: A=∫ab∣f(x)∣dxA = \int_a^b |f(x)| dx.

  • The area bounded between two continuous curves y=f(x)y = f(x) and y=g(x)y = g(x) from x=ax = a to x=bx = b is given by A=∫ab[yupper−ylower]dxA = \int_a^b [y_{\text{upper}} - y_{\text{lower}}] dx, independent of whether the curves lie above or below the xx-axis.

  • Archimedes' parabolic shortcut establishes that the area bounded by a standard parabola and a chord perpendicular to its axis of symmetry is precisely two-thirds of the circumscribed rectangle: A=23×base×heightA = \frac{2}{3} \times \text{base} \times \text{height}, solving standard ECAT area questions in under 20 seconds.

  • First-order differential equations are classified by order (the highest derivative present, which equals 1) and degree (the algebraic power of that highest derivative after eliminating all fractional powers and radical expressions).

  • Linear first-order differential equations in standard Leibniz form dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x) are solved using the integrating factor I(x)=e∫P(x)dxI(x) = e^{\int P(x) dx}, yielding the closed-form general solution y⋅I(x)=∫Q(x)I(x)dx+cy \cdot I(x) = \int Q(x) I(x) dx + c.

Last updated: October 2026

Area Under Curves & First-Order Differential Equations

The practical power of integral calculus is demonstrated across two vital engineering domains: determining planar areas bounded by geometric curves and solving differential equations that govern dynamic physical systems. Both topics constitute core components of intermediate mathematics (FSc Part II) and feature prominently on the UET ECAT. Engineering entrance questions test not only your ability to perform rigorous integration, but also your proficiency with geometric shortcuts (such as Archimedes' parabolic area formula) and rapid differential equation classification. This section explores geometric area calculations, establishes rigorous sign-management principles, defines differential order and degree, and provides systematic solution blueprints for first-order ordinary differential equations.


1. Geometric Interpretation of Definite Integrals & Planar Area

Net Signed Area vs. Geometric Physical Area

When a curve y=f(x)y = f(x) lies entirely above the xx-axis on [a,b][a, b], the definite integral ∫abf(x)dx\int_a^b f(x) dx evaluates the exact geometric area enclosed between the curve, the xx-axis, and the vertical lines x=ax = a and x=bx = b. However, if f(x)f(x) drops below the xx-axis, the function values are negative, and the Riemann sum evaluates these regions with a negative algebraic sign. The definite integral calculates the net signed area:

Net Signed Area=∫abf(x)dx=Aabove−Abelow\text{Net Signed Area} = \int_a^b f(x) dx = A_{\text{above}} - A_{\text{below}}

To compute the true total geometric area AA, one must integrate the absolute value of the function:

A=∫ab∣f(x)∣dxA = \int_a^b |f(x)| dx

Systematic Three-Step Procedure for Single-Curve Area

  1. Find Real Roots: Solve f(x)=0f(x) = 0 on the interval [a,b][a, b] to identify all xx-intercepts where the curve crosses the axis.
  2. Partition Interval: Subdivide [a,b][a, b] at each root into subintervals where f(x)f(x) maintains a constant sign.
  3. Sum Absolute Magnitudes: Integrate f(x)f(x) over each subinterval, taking the absolute value of each resulting quantity: A=∣∫ac1f(x)dx∣+∣∫c1c2f(x)dx∣+⋯+∣∫ckbf(x)dx∣A = \left| \int_a^{c_1} f(x) dx \right| + \left| \int_{c_1}^{c_2} f(x) dx \right| + \dots + \left| \int_{c_k}^b f(x) dx \right|

ECAT Walkthrough Example: Find the total area bounded by y=sin⁡xy = \sin x and the xx-axis from x=0x = 0 to x=2πx = 2\pi.

  • If you blindly integrate without splitting: ∫02πsin⁡xdx=[−cos⁡x]02π=−1−(−1)=0\int_0^{2\pi} \sin x dx = [-\cos x]_0^{2\pi} = -1 - (-1) = 0, which is geometrically absurd!
  • The root on (0,2π)(0, 2\pi) is x=πx = \pi.
  • Partition at π\pi: A1=∫0πsin⁡xdx=[−cos⁡x]0π=−(−1)−(−1)=2A_1 = \int_0^\pi \sin x dx = [-\cos x]_0^\pi = -(-1) - (-1) = 2 A2=∫π2πsin⁡xdx=[−cos⁡x]π2π=−1−(−(−1))=−2  ⟹  ∣A2∣=2A_2 = \int_\pi^{2\pi} \sin x dx = [-\cos x]_\pi^{2\pi} = -1 - (-(-1)) = -2 \implies |A_2| = 2
  • Total geometric area: A=2+2=4A = 2 + 2 = 4 square units.

Area Bounded with Respect to the yy-Axis

When a curve is given by x=g(y)x = g(y), bounded by the yy-axis and horizontal lines y=cy = c and y=dy = d:

A=∫cd∣g(y)∣dyA = \int_c^d |g(y)| dy


2. Area Bounded Between Two Curves

General Formulation

If f(x)f(x) and g(x)g(x) are continuous functions such that f(x)≥g(x)f(x) \ge g(x) for all x∈[a,b]x \in [a, b], the area bounded between the two curves from x=ax = a to x=bx = b is the integral of the vertical difference:

A=∫ab[yupper−ylower]dx=∫ab[f(x)−g(x)]dxA = \int_a^b [y_{\text{upper}} - y_{\text{lower}}] dx = \int_a^b [f(x) - g(x)] dx

Critical Insight: This formula holds strictly true regardless of whether both curves lie above the xx-axis, both lie below the xx-axis, or one lies above and one below. The vertical height of a representative strip is always yupper−ylowery_{\text{upper}} - y_{\text{lower}}.

Integration Along the yy-Axis

When curves are expressed more simply as functions of yy, such as horizontal parabolas x=f(y)x = f(y), vertical strips are replaced with horizontal strips of width dydy and length xright−xleftx_{\text{right}} - x_{\text{left}}:

A=∫cd[xright−xleft]dyA = \int_c^d [x_{\text{right}} - x_{\text{left}}] dy


3. High-Speed ECAT Area Shortcuts (Archimedes' Theorems)

Manually solving for intersection limits and integrating quadratic polynomials consumes 2 to 3 minutes. The following closed-form geometric shortcuts allow candidates to solve standard ECAT parabola area questions in under 15 seconds.

1. Parabola Bounded by a Chord Perpendicular to its Axis (Archimedes' Formula)

The area of a parabolic segment bounded by the parabola and a chord perpendicular to its axis of symmetry equals two-thirds of the area of the circumscribed bounding rectangle:

A=23×base×heightA = \frac{2}{3} \times \text{base} \times \text{height}

Application: Area bounded by y2=4axy^2 = 4ax and its Latus Rectum (x=ax = a):

  • Base (length of latus rectum) =4a= 4a.
  • Height (distance from vertex (0,0)(0,0) to chord x=ax = a) =a= a.
  • Area A=23(4a)(a)=83a2A = \frac{2}{3}(4a)(a) = \frac{8}{3}a^2.

2. Area Bounded by Parabola y2=4axy^2 = 4ax and Line y=mxy = mx

A=8a23m3A = \frac{8 a^2}{3 m^3}

Example: Find the area bounded by y2=8xy^2 = 8x and y=2xy = 2x.

  • Here 4a=8  ⟹  a=24a = 8 \implies a = 2, and m=2m = 2.
  • A=8(22)3(23)=8(4)3(8)=43A = \frac{8(2^2)}{3(2^3)} = \frac{8(4)}{3(8)} = \frac{4}{3} square units. Solved in 5 seconds!

3. Area Bounded by Two Orthogonal Parabolas y2=4axy^2 = 4ax and x2=4byx^2 = 4by

A=16ab3A = \frac{16 a b}{3}

Example: Find the area enclosed between y2=4xy^2 = 4x and x2=4yx^2 = 4y.

  • Here 4a=4  ⟹  a=14a = 4 \implies a = 1 and 4b=4  ⟹  b=14b = 4 \implies b = 1.
  • A=16(1)(1)3=163A = \frac{16(1)(1)}{3} = \frac{16}{3} square units.

4. Area Bounded by Parabola y=ax2y = ax^2 and Line y=cy = c

A=43ccaA = \frac{4}{3} c \sqrt{\frac{c}{a}}


4. Introduction to Differential Equations: Order & Degree

A differential equation (DE) is an algebraic equation that establishes a relationship between an independent variable xx, a dependent variable yy, and one or more derivatives of yy with respect to xx:

F(x,y,dydx,d2ydx2,…,dnydxn)=0F\left(x, y, \frac{dy}{dx}, \frac{d^2y}{dx^2}, \dots, \frac{d^n y}{dx^n}\right) = 0

Definitions of Order and Degree

  1. Order: The order of a differential equation is the order of the highest derivative appearing anywhere in the equation.
  2. Degree: The degree of a differential equation is the power (positive integer exponent) of the highest-order derivative, after the differential equation has been converted into a rational integral form (meaning all fractional powers and radical signs on derivatives have been cleared).

ECAT Trap Alert: Degree is defined only when the equation can be written as a polynomial in its derivatives. If derivatives appear inside transcendental functions (e.g., sin⁡(dydx)+y=0\sin\left(\frac{dy}{dx}\right) + y = 0 or ey′=xe^{y'} = x), the degree is undefined, though the order remains well-defined!

Walkthrough: Determining Order and Degree

Determine the order and degree of: [1+(dydx)2]3/2=5d2ydx2\left[ 1 + \left(\frac{dy}{dx}\right)^2 \right]^{3/2} = 5 \frac{d^2y}{dx^2}

  1. Identify the highest derivative: d2ydx2\frac{d^2y}{dx^2}, which has order 22.
  2. Clear the fractional exponent 32\frac{3}{2} by squaring both sides: [1+(dydx)2]3=25(d2ydx2)2\left[ 1 + \left(\frac{dy}{dx}\right)^2 \right]^3 = 25 \left(\frac{d^2y}{dx^2}\right)^2
  3. The highest-order derivative d2ydx2\frac{d^2y}{dx^2} now carries power 22.
  4. Order = 2, Degree = 2.

General Solution vs. Particular Solution

  • General Solution: A solution containing nn independent arbitrary constants, where nn is equal to the order of the differential equation. A first-order DE contains exactly 11 arbitrary constant cc.
  • Particular Solution: A solution obtained from the general solution by assigning specific numerical values to the arbitrary constants using given initial or boundary conditions (e.g., y(0)=1y(0) = 1).

5. First-Order Differential Equations: Three Primary Forms

Most first-order differential equations in the Intermediate syllabus fall into one of three standard categories:

Category 1: Variable Separable Differential Equations

An equation is variable separable if it can be algebraically factored such that all terms involving yy multiply dydy on one side, and all terms involving xx multiply dxdx on the opposite side:

dydx=g(x)h(y)  ⟹  1h(y)dy=g(x)dx\frac{dy}{dx} = g(x) h(y) \implies \frac{1}{h(y)} dy = g(x) dx

Integrate both sides directly: ∫1h(y)dy=∫g(x)dx+c\int \frac{1}{h(y)} dy = \int g(x) dx + c

Example: Solve dydx=1+y21+x2\frac{dy}{dx} = \frac{1 + y^2}{1 + x^2}.

  • Separate: dy1+y2=dx1+x2\frac{dy}{1 + y^2} = \frac{dx}{1 + x^2}.
  • Integrate: arctan⁡y=arctan⁡x+c\arctan y = \arctan x + c.
  • Using the tangent addition formula, this simplifies to y=x+C1−Cxy = \frac{x + C}{1 - Cx}.

Category 2: Homogeneous First-Order Differential Equations

A first-order equation dydx=f(x,y)g(x,y)\frac{dy}{dx} = \frac{f(x, y)}{g(x, y)} is homogeneous if both f(x,y)f(x, y) and g(x,y)g(x, y) are homogeneous polynomials of the same degree nn, meaning f(λx,λy)=λnf(x,y)f(\lambda x, \lambda y) = \lambda^n f(x, y). Alternatively, dydx=F(yx)\frac{dy}{dx} = F\left(\frac{y}{x}\right).

Standard Substitution: Let y=vxy = vx. Differentiating with respect to xx via the product rule: dydx=v+xdvdx\frac{dy}{dx} = v + x \frac{dv}{dx}

Substitute into the differential equation: v+xdvdx=F(v)  ⟹  xdvdx=F(v)−vv + x \frac{dv}{dx} = F(v) \implies x \frac{dv}{dx} = F(v) - v

This transforms the homogeneous equation into a variable-separable equation in vv and xx: dvF(v)−v=dxx\frac{dv}{F(v) - v} = \frac{dx}{x} After integrating, replace vv with yx\frac{y}{x} to express the solution in terms of the original variables.

Category 3: Linear First-Order Differential Equations (Leibniz Form)

A differential equation is linear of first order if it can be written in the canonical form:

dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x) y = Q(x)

where P(x)P(x) and Q(x)Q(x) are continuous functions of xx alone (or constants), and yy appears strictly to the first power with no products involving yy and dydx\frac{dy}{dx}.

The Integrating Factor (I.F.) Method

  1. Identify P(x)P(x) and Q(x)Q(x) from standard form.
  2. Compute the Integrating Factor I(x)I(x): I(x)=e∫P(x)dxI(x) = e^{\int P(x) dx}
  3. Write the General Solution: y⋅I(x)=∫Q(x)I(x)dx+cy \cdot I(x) = \int Q(x) I(x) dx + c

Proof: Multiply the canonical equation by I(x)=e∫P(x)dxI(x) = e^{\int P(x) dx}: e∫P(x)dxdydx+P(x)e∫P(x)dxy=Q(x)e∫P(x)dxe^{\int P(x) dx} \frac{dy}{dx} + P(x) e^{\int P(x) dx} y = Q(x) e^{\int P(x) dx} By the product rule, the left-hand side is the exact derivative ddx[ye∫P(x)dx]\frac{d}{dx}\left[ y e^{\int P(x) dx} \right]. Integrating both sides with respect to xx yields y⋅I(x)=∫Q(x)I(x)dx+cy \cdot I(x) = \int Q(x) I(x) dx + c.

Linear Form with Dependent Variable xx

If dydx\frac{dy}{dx} is non-linear in yy but linear in xx, invert to find dxdy\frac{dx}{dy}: dxdy+P(y)x=Q(y)  ⟹  I(y)=e∫P(y)dy,x⋅I(y)=∫Q(y)I(y)dy+c\frac{dx}{dy} + P(y) x = Q(y) \implies I(y) = e^{\int P(y) dy}, \quad x \cdot I(y) = \int Q(y) I(y) dy + c


6. Differential Equation Diagnostic & Classification Table

Differential Equation FormIdentification CriterionSolution ProcedureKey Formula / Substitution
Variable Separabledydx=f(x)g(y)\frac{dy}{dx} = f(x)g(y)Separate variables and integrate∫dyg(y)=∫f(x)dx+c\int \frac{dy}{g(y)} = \int f(x) dx + c
Reducible to Separabledydx=f(ax+by+c)\frac{dy}{dx} = f(ax + by + c)Substitute linear argumentLet u=ax+by+c  ⟹  dudx=a+bdydxu = ax + by + c \implies \frac{du}{dx} = a + b\frac{dy}{dx}
Homogeneousdydx=F(yx)\frac{dy}{dx} = F\left(\frac{y}{x}\right)Degree of numerator == degree of denominatorLet y=vx  ⟹  dydx=v+xdvdxy = vx \implies \frac{dy}{dx} = v + x\frac{dv}{dx}
Linear in yydydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x)yy and dydx\frac{dy}{dx} appear to 1st power onlyI=e∫Pdx,y⋅I=∫Q⋅Idx+cI = e^{\int P dx}, \quad y \cdot I = \int Q \cdot I dx + c
Linear in xxdxdy+P(y)x=Q(y)\frac{dx}{dy} + P(y)x = Q(y)xx and dxdy\frac{dx}{dy} appear to 1st power onlyI=e∫Pdy,x⋅I=∫Q⋅Idy+cI = e^{\int P dy}, \quad x \cdot I = \int Q \cdot I dy + c
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Decision Flowchart for Solving First-Order Ordinary Differential Equations
Test Your Knowledge

What is the area of the region enclosed between the parabola y2=8xy^2 = 8x and the line y=2xy = 2x?

A

83\frac{8}{3}

B

163\frac{16}{3}

C

43\frac{4}{3}

D

22

Test Your Knowledge

What are the order and degree of the differential equation [1+(dydx)2]3/2=5d2ydx2\left[ 1 + \left(\frac{dy}{dx}\right)^2 \right]^{3/2} = 5 \frac{d^2y}{dx^2}?

A

Order 2, Degree 2

B

Order 2, Degree 3

C

Order 1, Degree 3

D

Order 2, Degree 1

Test Your Knowledge

What is the general solution of the linear first-order differential equation dydx+2xy=3x\frac{dy}{dx} + \frac{2}{x}y = 3x for x>0x > 0?

A

y=32x2+cy = \frac{3}{2}x^2 + c

B

y=x3+cxy = x^3 + \frac{c}{x}

C

y=3x2+cx2y = 3x^2 + \frac{c}{x^2}

D

y=34x2+cx2y = \frac{3}{4}x^2 + \frac{c}{x^2}

Sections you finish are checked off in the contents.