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GATE Mathematics 100 practice problems


GATE Problem Bank - Ordinary Differential Equations (ODE)

Problem 1: First Order Linear ODE

Question:

\[ \frac{dy}{dx}+2y=e^{-x} \]

Step 1: Compare with standard form

\[ \frac{dy}{dx}+P(x)y=Q(x) \] Here, \[ P(x)=2 \] Integrating factor: \[ IF=e^{\int2dx}=e^{2x} \]

Step 2: Multiply by IF

\[ e^{2x}\frac{dy}{dx}+2e^{2x}y=e^x \] Left side: \[ \frac{d}{dx}(ye^{2x})=e^x \]

Step 3: Integrate

\[ ye^{2x}=e^x+C \] Therefore:
\[ \boxed{ y=e^{-x}+Ce^{-2x} } \]

Problem 2: Separable Differential Equation

Question:

\[ \frac{dy}{dx}=xy \]

Step 1: Separate variables

\[ \frac{dy}{y}=x dx \]

Step 2: Integrate

\[ \ln y=\frac{x^2}{2}+C \] Taking exponential: \[ y=Ce^{x^2/2} \]
\[ \boxed{ y=Ce^{x^2/2} } \]

Problem 3: Exact Differential Equation

Question:

\[ (2xy+y^2)dx+(x^2+2xy)dy=0 \] Let: \[ M=2xy+y^2 \] \[ N=x^2+2xy \] Check exactness: \[ \frac{\partial M}{\partial y} = 2x+2y \] \[ \frac{\partial N}{\partial x} = 2x+2y \] Therefore exact.

Integrate M with respect to x

\[ \int(2xy+y^2)dx \] \[ =x^2y+xy^2+\phi(y) \] Differentiate with respect to y: \[ x^2+2xy+\phi'(y) \] Compare with N: \[ \phi'(y)=0 \] Therefore:
\[ \boxed{ x^2y+xy^2=C } \]

Problem 4: Second Order Homogeneous ODE

Question:

\[ y''-5y'+6y=0 \]

Step 1: Auxiliary equation

\[ m^2-5m+6=0 \] \[ (m-2)(m-3)=0 \] Roots: \[ m=2,3 \]
\[ \boxed{ y=C_1e^{2x}+C_2e^{3x} } \]

Problem 5: Non-Homogeneous ODE (CF + PI)

Question:

\[ y''-4y'+4y=e^{2x} \]

CF

Auxiliary equation: \[ m^2-4m+4=0 \] \[ (m-2)^2=0 \] Therefore: \[ CF=(C_1+C_2x)e^{2x} \]

PI

Since \(e^{2x}\) repeats in CF, multiply trial by \(x^2\). Assume: \[ PI=Ax^2e^{2x} \] Substitution gives: \[ A=\frac12 \] Therefore:
\[ \boxed{ y=(C_1+C_2x)e^{2x} +\frac12x^2e^{2x} } \]

Problem 6: Cauchy-Euler Equation

Question:

\[ x^2y''-3xy'+4y=0 \] Assume: \[ y=x^m \] Derivatives: \[ xy'=mx^m \] \[ x^2y''=m(m-1)x^m \] Substitute: \[ m(m-1)-3m+4=0 \] \[ m^2-4m+4=0 \] \[ (m-2)^2=0 \]
\[ \boxed{ y=x^2(C_1+C_2\ln x) } \]

Problem 7: Laplace Transform ODE

Question:

\[ y'+3y=0 \] Given: \[ y(0)=5 \] Laplace: \[ sY(s)-5+3Y(s)=0 \] Therefore: \[ Y(s)=\frac5{s+3} \] Inverse:
\[ \boxed{ y=5e^{-3t} } \]

Problem 8: Second Order Initial Value Problem

Question:

\[ y''+4y=0 \] Given: \[ y(0)=1,\quad y'(0)=0 \] Solution form: \[ y=C_1\cos2x+C_2\sin2x \] Apply conditions: \[ C_1=1 \] \[ C_2=0 \]
\[ \boxed{ y=\cos2x } \]

Problem 9: Bernoulli Equation

Question:

\[ y'+y=y^2 \] Divide by \(y^2\): \[ y^{-2}y'+y^{-1}=1 \] Let: \[ v=y^{-1} \] Then: \[ v'-v=-1 \] Solving: \[ v=1+Ce^x \] Since: \[ v=\frac1y \]
\[ \boxed{ y=\frac1{1+Ce^x} } \]

Problem 10: Linear Differential Operator

Question:

\[ (D^2-3D+2)y=e^x \]

CF

\[ m^2-3m+2=0 \] \[ m=1,2 \] \[ CF=C_1e^x+C_2e^{2x} \]

PI

Because RHS \(e^x\) is repeated: \[ PI=Axe^x \] Substitution gives: \[ A=-1 \]
\[ \boxed{ y=C_1e^x+C_2e^{2x}-xe^x } \]

GATE Problem Bank - Partial Differential Equations (PDE)

Problem 11: Form PDE by Eliminating Constants

Question:

Given: \[ z=ax^2+by^2 \] Form the PDE by eliminating constants \(a,b\).

Step 1

Differentiate with respect to x: \[ \frac{\partial z}{\partial x}=2ax \] Therefore: \[ a=\frac{z_x}{2x} \] Differentiate with respect to y: \[ \frac{\partial z}{\partial y}=2by \] Therefore: \[ b=\frac{z_y}{2y} \]

Step 2

Substitute into original equation: \[ z= \frac{xz_x}{2} + \frac{yz_y}{2} \] Multiply by 2:
\[ \boxed{ 2z=xz_x+yz_y } \]

Problem 12: Form PDE by Eliminating Arbitrary Function

Question:

\[ z=f(x^2+y^2) \] Find PDE.

Step 1

Differentiate: \[ z_x=f'(x^2+y^2)2x \] \[ z_y=f'(x^2+y^2)2y \]

Step 2

Divide: \[ \frac{z_x}{2x} = \frac{z_y}{2y} \] Therefore:
\[ \boxed{ yz_x-xz_y=0 } \]

Problem 13: Lagrange First Order PDE

Question:

\[ x p+y q=z \] where \[ p=\frac{\partial z}{\partial x}, \quad q=\frac{\partial z}{\partial y} \]

Step 1

Lagrange form: \[ \frac{dx}{x} = \frac{dy}{y} = \frac{dz}{z} \]

Step 2

From first two: \[ \frac{dx}{x}=\frac{dy}{y} \] Integrate: \[ \ln x-\ln y=C \] Therefore: \[ \frac{x}{y}=C_1 \] From: \[ \frac{dx}{x}=\frac{dz}{z} \] \[ \ln x-\ln z=C \] Therefore: \[ \frac{x}{z}=C_2 \]
General solution: \[ \boxed{ F\left(\frac{x}{y},\frac{x}{z}\right)=0 } \]

Problem 14: PDE CF Only

Question:

\[ (D^2-4DD'+3D'^2)z=0 \]

Step 1: Auxiliary equation

\[ m^2-4m+3=0 \] \[ (m-1)(m-3)=0 \] Roots: \[ m=1,3 \]

Step 2: Complementary Function

\[ \boxed{ z=\phi_1(y+x)+\phi_2(y+3x) } \]

Problem 15: PDE CF + PI

Question:

\[ (D^2+3DD'+2D'^2)z=e^{x+2y} \]

Step 1: CF

Auxiliary equation: \[ m^2+3m+2=0 \] \[ (m+1)(m+2)=0 \] Therefore: \[ CF=\phi_1(y-x)+\phi_2(y-2x) \]

Step 2: PI

For exponential: \[ D=1,\quad D'=2 \] Substitute: \[ F(1,2)=1+6+8 \] \[ =15 \] Therefore: \[ PI=\frac1{15}e^{x+2y} \]
\[ \boxed{ z= \phi_1(y-x)+ \phi_2(y-2x) +\frac1{15}e^{x+2y} } \]

Problem 16: PDE Exponential Trial Function

Question:

Find \(\xi,\eta\) such that: \[ f_{xx}+2f_{xy}+f_{yy}=4f \] Assume: \[ f=e^{\xi x+\eta y} \]

Step 1

Convert derivatives: \[ f_{xx}=\xi^2f \] \[ f_{xy}=\xi\eta f \] \[ f_{yy}=\eta^2f \]

Step 2

Substitute: \[ (\xi^2+2\xi\eta+\eta^2)f=4f \] Cancel \(f\):
\[ \boxed{ (\xi+\eta)^2=4 } \]

Problem 17: Second Order PDE Classification

Question:

Classify: \[ 3u_{xx}+4u_{xy}+u_{yy}=0 \] Compare: \[ Au_{xx}+Bu_{xy}+Cu_{yy}=0 \] Here: \[ A=3,\quad B=4,\quad C=1 \] Calculate: \[ B^2-4AC \] \[ =16-12 \] \[ =4 \]
Since: \[ B^2-4AC>0 \] \[ \boxed{\text{Hyperbolic PDE}} \]

Problem 18: Heat Equation Separation

Question:

\[ u_t=\alpha^2u_{xx} \] Assume: \[ u=X(x)T(t) \] Substitute: \[ XT'=\alpha^2X''T \] Separate: \[ \frac{T'}{\alpha^2T} = \frac{X''}{X} = -\lambda^2 \] Solutions: \[ T=e^{-\alpha^2\lambda^2t} \] \[ X=A\sin\lambda x+B\cos\lambda x \]
\[ \boxed{ u= (A\sin\lambda x+B\cos\lambda x) e^{-\alpha^2\lambda^2t} } \]

Problem 19: PDE PI Failure Case

Question:

\[ (D-D')z=e^{x+y} \] For PI: \[ D=1,D'=1 \] Denominator: \[ D-D'=0 \] Failure case.

Correction

Multiply by x: \[ PI=xe^{x+y} \]
\[ \boxed{ z=\phi(x+y)+xe^{x+y} } \]

Problem 20: Laplace Equation

Question:

Solve: \[ u_{xx}+u_{yy}=0 \] Assume: \[ u=X(x)Y(y) \] Substitute: \[ X''Y+XY''=0 \] Divide: \[ \frac{X''}{X} = -\frac{Y''}{Y} \] Set: \[ =-\lambda^2 \] Therefore: \[ X''+\lambda^2X=0 \] \[ Y''-\lambda^2Y=0 \]
General form: \[ \boxed{ u=(A\sin\lambda x+B\cos\lambda x) (Ce^{\lambda y}+De^{-\lambda y}) } \]

GATE Problem Bank - Fourier Series and Laplace Transform

Problem 21: Fourier Series of a Constant Function

Question:

Find Fourier series of: \[ f(x)=1,\quad -\piStep 1: Symmetry Constant function is even. Therefore: \[ b_n=0 \]

Step 2: Calculate \(a_0\)

\[ a_0= \frac1\pi \int_{-\pi}^{\pi}1dx \] \[ a_0=2 \] Therefore: \[ \frac{a_0}{2}=1 \]

Step 3

All cosine coefficients are zero.
\[ \boxed{ f(x)=1 } \]

Problem 22: Fourier Series of \(f(x)=x\)

Question:

Find Fourier series: \[ -\piStep 1: Symmetry Since: \[ f(-x)=-f(x) \] Function is odd. Therefore: \[ a_0=0,\quad a_n=0 \] Only sine terms exist.

Step 2

\[ b_n= \frac2\pi \int_0^\pi x\sin(nx)dx \] Integration: \[ b_n= \frac{2(-1)^{n+1}}n \]
\[ \boxed{ x= 2\sum_{n=1}^{\infty} \frac{(-1)^{n+1}}n \sin nx } \]

Problem 23: Even Function Fourier Series

Question:

Find Fourier series of: \[ f(x)=x^2 \] for: \[ -\piStep 1 \(x^2\) is even. Hence: \[ b_n=0 \]

Step 2

Coefficient: \[ a_n= \frac2\pi \int_0^\pi x^2\cos(nx)dx \] Result: \[ a_n= \frac{4(-1)^n}{n^2} \] Also: \[ a_0=\frac{2\pi^2}{3} \]
\[ \boxed{ x^2= \frac{\pi^2}{3} + 4\sum_{n=1}^{\infty} \frac{(-1)^n}{n^2}\cos nx } \]

Problem 24: Half Range Sine Series

Question:

Expand: \[ f(x)=x \] in sine series: \[ 0 \[ \boxed{ x= 2 \sum_{n=1}^{\infty} \frac{(-1)^{n+1}}n \sin nx } \]

Laplace Transform Problem Bank

Problem 25: Basic Laplace Transform

Question:

Find: \[ L\{e^{at}\} \] Formula: \[ L\{e^{at}\} = \int_0^\infty e^{-st}e^{at}dt \] Simplify: \[ = \int_0^\infty e^{-(s-a)t}dt \]
\[ \boxed{ L\{e^{at}\} = \frac1{s-a} } \]

Problem 26: Laplace of Derivative

Question:

Find: \[ L\{y'\} \] Using integration:
\[ \boxed{ L\{y'\}=sY(s)-y(0) } \]

Problem 27: Inverse Laplace

Question:

Find inverse Laplace: \[ Y(s)=\frac1{s(s+1)} \] Partial fractions: \[ \frac1{s(s+1)} = \frac1s-\frac1{s+1} \] Inverse:
\[ \boxed{ y=1-e^{-t} } \]

Problem 28: Second Order ODE Using Laplace

Question:

Solve: \[ y''+y=0 \] Conditions: \[ y(0)=0 \] \[ y'(0)=1 \] Laplace: \[ s^2Y-1+Y=0 \] Therefore: \[ Y=\frac1{s^2+1} \]
\[ \boxed{ y=\sin t } \]

Problem 29: Unit Step Function

Question:

Find Laplace: \[ u(t-a) \] where \(u\) is step function.
\[ \boxed{ L\{u(t-a)\} = \frac{e^{-as}}s } \]

Problem 30: Shift Property

Question:

Find: \[ L\{e^{at}f(t)\} \] Using shift:
\[ \boxed{ L\{e^{at}f(t)\}=F(s-a) } \]

Problem 31: Convolution Theorem

Question:

If: \[ F(s)=G(s)H(s) \] then:
\[ \boxed{ L^{-1}\{F(s)\} = g(t)*h(t) } \] where: \[ g*h= \int_0^t g(\tau)h(t-\tau)d\tau \]

Problem 32: Laplace Transform of Sine

Question:

Find: \[ L\{\sin at\} \]
\[ \boxed{ L\{\sin at\} = \frac{a}{s^2+a^2} } \]

Problem 33: Laplace Transform of Cosine

Question:

Find: \[ L\{\cos at\} \]
\[ \boxed{ L\{\cos at\} = \frac{s}{s^2+a^2} } \]

Problem 34: Initial Value Theorem

Question:

Find: \[ y(0) \] if: \[ Y(s)=\frac{5}{s+5} \] Formula: \[ y(0)=\lim_{s\to\infty}sY(s) \] Therefore: \[ = \lim_{s\to\infty} \frac{5s}{s+5} \]
\[ \boxed{ y(0)=5 } \]

Problem 35: Final Value Theorem

Question:

Find: \[ y(\infty) \] if: \[ Y(s)=\frac1{s(s+2)} \] Formula: \[ y(\infty)= \lim_{s\to0}sY(s) \] Therefore: \[ = \lim_{s\to0} \frac1{s+2} \]
\[ \boxed{ y(\infty)=\frac12 } \]

GATE Problem Bank - Heat, Wave and Laplace Equations

Problem 36: Classification of Second Order PDE

Question:

Classify: \[ u_{xx}+6u_{xy}+5u_{yy}=0 \] Compare: \[ Au_{xx}+Bu_{xy}+Cu_{yy}=0 \] Therefore: \[ A=1,\quad B=6,\quad C=5 \] Calculate: \[ B^2-4AC \] \[ =36-20 \] \[ =16 \]
Since: \[ B^2-4AC>0 \] \[ \boxed{\text{Hyperbolic PDE}} \]

Problem 37: Classification of Heat Equation

Question:

Classify: \[ u_t=\alpha^2u_{xx} \] Rewrite: \[ \alpha^2u_{xx}-u_t=0 \] Only one spatial second derivative exists.
\[ \boxed{\text{Parabolic PDE}} \]

Problem 38: Classification of Laplace Equation

Question:

Classify: \[ u_{xx}+u_{yy}=0 \] Here: \[ A=1,B=0,C=1 \] Therefore: \[ B^2-4AC = 0-4 \] \[ =-4 \]
\[ \boxed{\text{Elliptic PDE}} \]

Problem 39: Separation of Variables for Heat Equation

Question:

Solve: \[ u_t=\alpha^2u_{xx} \] Assume: \[ u=X(x)T(t) \] Substitute: \[ XT'=\alpha^2X''T \] Divide: \[ \frac{T'}{\alpha^2T} = \frac{X''}{X} \] Set: \[ =-\lambda^2 \]

Time equation

\[ T'+\alpha^2\lambda^2T=0 \] Solution: \[ T=e^{-\alpha^2\lambda^2t} \]

Space equation

\[ X''+\lambda^2X=0 \] Solution: \[ X=A\sin\lambda x+B\cos\lambda x \]
\[ \boxed{ u=(A\sin\lambda x+B\cos\lambda x) e^{-\alpha^2\lambda^2t} } \]

Problem 40: Heat Equation with Boundary Conditions

Question:

\[ u_t=\alpha^2u_{xx} \] Boundary: \[ u(0,t)=0 \] \[ u(L,t)=0 \]

Eigenvalue condition

\[ X(0)=0 \] gives: \[ B=0 \] and: \[ X(L)=0 \] gives: \[ \sin(\lambda L)=0 \] Therefore: \[ \lambda_n=\frac{n\pi}{L} \]
Solution: \[ \boxed{ u= \sum_{n=1}^{\infty} A_n \sin\frac{n\pi x}{L} e^{-\alpha^2(n\pi/L)^2t} } \]

Problem 41: Wave Equation

Question:

Solve: \[ u_{tt}=c^2u_{xx} \] Assume: \[ u=X(x)T(t) \] Substitute: \[ XT''=c^2X''T \] Separate: \[ \frac{T''}{c^2T} = \frac{X''}{X} = -\lambda^2 \] Equations: \[ X''+\lambda^2X=0 \] \[ T''+c^2\lambda^2T=0 \]
\[ \boxed{ u= (A\sin\lambda x+B\cos\lambda x) (C\sin c\lambda t+D\cos c\lambda t) } \]

Problem 42: Vibrating String Boundary Condition

Question:

String fixed at: \[ x=0,L \] Condition: \[ u(0,t)=u(L,t)=0 \] Eigenvalues: \[ \lambda_n=\frac{n\pi}{L} \]
Allowed modes: \[ \boxed{ \sin\frac{n\pi x}{L} } \]

Problem 43: Laplace Equation Separation

Question:

Solve: \[ u_{xx}+u_{yy}=0 \] Assume: \[ u=X(x)Y(y) \] Substitute: \[ X''Y+XY''=0 \] Divide: \[ \frac{X''}{X} = -\frac{Y''}{Y} \] Set: \[ =-\lambda^2 \] Therefore: \[ X''+\lambda^2X=0 \] \[ Y''-\lambda^2Y=0 \]
\[ \boxed{ u= (A\sin\lambda x+B\cos\lambda x) (Ce^{\lambda y}+De^{-\lambda y}) } \]

Problem 44: Steady State Heat Equation

Question:

Find steady temperature: \[ u_{xx}=0 \] Integrate: \[ u_x=A \] Again: \[ u=Ax+B \] Boundary: \[ u(0)=T_1 \] \[ u(L)=T_2 \] Solving constants:
\[ \boxed{ u=T_1+ \frac{T_2-T_1}{L}x } \]

Problem 45: Fourier Solution of Heat Equation

Question:

Initial condition: \[ u(x,0)=f(x) \] Solution: \[ u(x,t) = \sum A_n \sin\frac{n\pi x}{L} e^{-\alpha^2(n\pi/L)^2t} \] where: \[ A_n= \frac2L \int_0^L f(x) \sin\frac{n\pi x}{L}dx \]
\[ \boxed{ A_n = \frac2L \int_0^L f(x)\sin\frac{n\pi x}{L}dx } \]

Problem 46: Wave Equation General Form

Question:

Find solution form: \[ u_{tt}=c^2u_{xx} \]
D'Alembert solution: \[ \boxed{ u=f(x-ct)+g(x+ct) } \]

Problem 47: Separation Constant Meaning

Question:

Why choose: \[ \frac{X''}{X} = \frac{T'}{\alpha^2T} = -\lambda^2 \] Answer: Negative constant produces oscillatory spatial solutions: \[ X''+\lambda^2X=0 \] which satisfy physical boundary conditions.
\[ \boxed{ -\lambda^2 \text{ gives valid eigenfunctions} } \]

Problem 48: Boundary Condition Types

Type Condition
Dirichlet \[ u(0,t)=0 \]
Neumann \[ u_x(0,t)=0 \]
Mixed \[ u(0,t)=0,\ u_x(L,t)=0 \]
\[ \boxed{\text{Boundary conditions determine eigenvalues}} \]

Problem 49: Maximum Principle Idea

Question:

For Laplace equation: \[ \nabla^2u=0 \] The maximum temperature occurs:
\[ \boxed{ \text{On the boundary, not inside the region} } \]

Problem 50: Complete GATE PDE Recognition

Equation Method
\[ F(D,D')z=0 \] CF
\[ F(D,D')z=\phi(x,y) \] CF + PI
\[ u_t=\alpha^2u_{xx} \] Heat equation
\[ u_{tt}=c^2u_{xx} \] Wave equation
\[ u_{xx}+u_{yy}=0 \] Laplace equation
\[ \boxed{ \text{Identify the equation before solving} } \]

GATE Quick Practice Set (Problems 51-100)

Section A: ODE Practice

Problem 51

Solve:

\[ \frac{dy}{dx}=2x \]
\[ \boxed{y=x^2+C} \]

Problem 52

\[ y'+y=0 \] Solution: \[ \boxed{y=Ce^{-x}} \]

Problem 53

Solve: \[ y''+4y=0 \] Characteristic equation: \[ m^2+4=0 \]
\[ \boxed{ y=C_1\cos2x+C_2\sin2x } \]

Problem 54

\[ y''-9y=0 \] Roots: \[ m=\pm3 \]
\[ \boxed{ y=C_1e^{3x}+C_2e^{-3x} } \]

Problem 55

\[ (D^2-1)y=0 \]
\[ \boxed{ y=C_1e^x+C_2e^{-x} } \]

Problem 56

\[ (D^2+4)y=\sin2x \] RHS repeats in CF.
\[ \boxed{ PI=-\frac{x\cos2x}{4} } \]

Problem 57

Cauchy Euler: \[ x^2y''+xy'-y=0 \] Put: \[ y=x^m \] Equation: \[ m^2-1=0 \]
\[ \boxed{ y=C_1x+C_2x^{-1} } \]

Problem 58

Laplace: \[ L\{1\} \]
\[ \boxed{\frac1s} \]

Problem 59

\[ L\{t\} \]
\[ \boxed{\frac1{s^2}} \]

Problem 60

\[ L\{e^{-at}\} \]
\[ \boxed{ \frac1{s+a} } \]

Section B: PDE Practice

Problem 61

Given: \[ f=e^{ax+by} \] Find: \[ f_x \]
\[ \boxed{ f_x=af } \]

Problem 62

Find: \[ f_{xx} \] for: \[ f=e^{ax+by} \]
\[ \boxed{ f_{xx}=a^2f } \]

Problem 63

Given: \[ af_x+bf_y=f \] Condition:
\[ \boxed{ a\xi+b\eta=1 } \]

Problem 64

For: \[ f_{xy} \] where: \[ f=e^{\xi x+\eta y} \]
\[ \boxed{ f_{xy}=\xi\eta f } \]

Problem 65

PDE: \[ (D-D')z=0 \]
\[ \boxed{ z=\phi(x+y) } \]

Problem 66

PDE: \[ (D+D')z=0 \]
\[ \boxed{ z=\phi(y-x) } \]

Problem 67

Classification: \[ u_{xx}+u_{yy}=0 \]
\[ \boxed{\text{Elliptic}} \]

Problem 68

Classification: \[ u_t=u_{xx} \]
\[ \boxed{\text{Parabolic}} \]

Problem 69

Classification: \[ u_{tt}=u_{xx} \]
\[ \boxed{\text{Hyperbolic}} \]

Problem 70

Heat equation separation: \[ u=X(x)T(t) \]
\[ \boxed{ T=e^{-\lambda^2t} } \]

Section C: Fourier and Laplace Practice

Problem 71

Odd function property:
\[ \boxed{ a_n=0 } \]

Problem 72

Even function property:
\[ \boxed{ b_n=0 } \]

Problem 73

Fourier coefficient: \[ a_0 \] represents:
\[ \boxed{ \text{average value} } \]

Problem 74

\[ L\{\sin at\} \]
\[ \boxed{ \frac{a}{s^2+a^2} } \]

Problem 75

\[ L\{\cos at\} \]
\[ \boxed{ \frac{s}{s^2+a^2} } \]

Problem 76

Initial value theorem: \[ y(0)=? \]
\[ \boxed{ \lim_{s\to\infty}sY(s) } \]

Problem 77

Final value theorem:
\[ \boxed{ \lim_{s\to0}sY(s) } \]

Problem 78

Unit step: \[ u(t-a) \]
\[ \boxed{ \frac{e^{-as}}s } \]

Problem 79

Convolution:
\[ \boxed{ L^{-1}(FG)=f*g } \]

Problem 80

Laplace derivative:
\[ \boxed{ L(y')=sY-y(0) } \]

Section D: Final GATE Concepts

Problems 81-100: Rapid Revision

Concept Answer
Non-zero RHS PDE CF + PI
Zero RHS PDE CF only
Exponential trial D → constant
Heat equation Parabolic
Wave equation Hyperbolic
Laplace equation Elliptic
Odd Fourier function Sine terms
Even Fourier function Cosine terms
Repeated PI root Multiply by x
Second repeated root ODE \(xe^{mx}\)
Laplace of derivative \(sY-y(0)\)
Laplace of second derivative \(s^2Y-sy(0)-y'(0)\)
Fourier coefficient Projection integral
Boundary conditions Determine constants/eigenvalues
Separation constant Eigenvalue
CF meaning Homogeneous solution
PI meaning Forced response
ODE order Number of constants
PDE order Highest derivative order
GATE strategy Identify method first




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Frequency Shift Keying (FSK) Theoretical Foundations: Frequency Shift Keying (FSK) is a discrete frequency modulation scheme wherein the digital information is encoded via instantaneous shifts in the carrier signal's frequency. The fundamental implementation is Binary FSK (BFSK), which maps binary data onto two distinct, discrete spectral states. A binary '1' (the "mark" state) is represented by a carrier frequency \( f_1 \), while a binary '0' (the "space" state) corresponds to frequency \( f_2 \). Each symbol is sustained for a bit interval denoted by \( T_b \). FSK Transmitter Characterization: The mathematical model for the modulated BFSK output \( s(t) \) is defined as: \[ s(t) = \begin{cases} A_c \cos(2\pi f_1 t), & \text{for } m = 1 \\ A_c \cos(2\pi f_2 t), & \text{for } m = 0 \end{cases} \] ...

RMS Delay Spread, Excess Delay Spread and Multi-path ...(with MATLAB + Simulator)

📘 Overview of Delay Spread and Multi-path 🧮 Excess Delay spread 🧮 Power delay Profile 🧮 RMS Delay Spread 📚 Further Reading 📂 Other Topics on RMS Delay Spread, Excess Delay ... 🧮 Multipath Components or MPCs 🧮 Online Simulator for Calculating RMS Delay Spread 🧮 Why is there significant multipath in the case of very high frequencies? 🧮 Why RMS Delay Spread is essential for wireless communication? 🧮 Why the Power Delay Profile is essential? 🧮 MATLAB Codes for Calculating Different Types of delay Spreads Delay Spread, Excess Delay Spread, and Multipath (MPCs) The fundamental distinction between wireless and wired connections is that in wireless connections signal reaches at receiver thru multipath signal propagation rather than directed transmission like co-axial cable. Wireless Communication has no set communication path between the transmitter and the receiver. The line...

OFDM Symbols and Subcarriers Explained

This article explains how OFDM (Orthogonal Frequency Division Multiplexing) symbols and subcarriers work. It covers modulation, mapping symbols to subcarriers, subcarrier frequency spacing, IFFT synthesis, cyclic prefix, and transmission. Step 1: Modulation First, modulate the input bitstream. For example, with 16-QAM , each group of 4 bits maps to one QAM symbol. Suppose we generate a sequence of QAM symbols: s0, s1, s2, s3, s4, s5, …, s63 Step 2: Mapping Symbols to Subcarriers Assume N sub = 8 subcarriers. Each OFDM symbol in the frequency domain contains 8 QAM symbols (one per subcarrier): Mapping (example) OFDM symbol 1 → s0, s1, s2, s3, s4, s5, s6, s7 OFDM symbol 2 → s8, s9, s10, s11, s12, s13, s14, s15 … OFDM sym...

Orthogonal Time Frequency Space (OTFS) (with MATLAB)

In OTFS (Orthogonal Time Frequency Space) modulation — a scheme designed for high-Doppler and time-varying wireless channels — the terms ISFFT and SFFT are key mathematical transformations used to move between different representation domains. Figure: OTFS block diagram 1. ISFFT — Inverse Symplectic Finite Fourier Transform Purpose: Transforms data symbols from the delay-Doppler domain to the time-frequency domain . \[ X[n, m] = \frac{1}{\sqrt{NM}} \sum_{k=0}^{N-1} \sum_{l=0}^{M-1} x[k, l] \, e^{j2\pi \left( \frac{nk}{N} - \frac{ml}{M} \right)} \] Here, \( N \) is the number of Doppler bins (time slots), and \( M \) is the number of delay bins (subcarriers). The ISFFT maps each data symbol from the delay-Doppler grid (where the channel is sparse and easier to equalize) to the time-frequency grid (where standard multicarrier modulation like OFDM can be applied). 2. SFFT — Symplectic Finite Fourier Transform Purpose: Performs the reverse operation ...

UGC NET Electronic Science Previous Year Question Papers with Solutions

Home / Engineering & Other Exams / UGC NET 2026 PYQ ⬇️ Download Papers and Solutions 📋 Exam Pattern 💡 Preparation Tips ❓ FAQs 📊 Exam Highlights: Electronic Science (88) Feature Details Junior Research Fellowship (JRF) ₹37,000 + HRA per month Eligibility M.Sc/M.Tech in Electronics (55%) Validity of Certificate JRF (3 Years) | Lectureship (Lifetime) 📥 Download UGC NET Electronics PDFs Complete collection of previous year question papers, answer keys and explanations for Subject Code 88. Start Downloading 📂 View All Question Papers June 2025 - Question Paper Download PDF June 2025 - Solved Paper + Explanation ...