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Mechanical Engineering GATE scoring topics, formulas and smart revision strategy.
| Feature | Details |
|---|---|
| Exam Mode | Computer-Based Test (CBT) |
| Duration | 3 Hours (180 minutes) |
| Total Questions | 65 (10 GA + 55 Subject) |
| Total Marks | 100 |
| 1-mark MCQ | +1 / −0.33 |
| 2-mark MCQ | +2 / −0.66 |
| NAT | +1 or +2 / No negative marking |
| General Aptitude | 15 marks |
| Engineering Math | 13–15 marks |
| Subject + Technical | 70–72 marks |
| Subject | 1-Mark | 2-Mark | Approx Total | Priority |
|---|---|---|---|---|
| General Aptitude | 5 | 5 | 15 | Must-do |
| Engineering Math | 4 | 5 | 14 | Highest |
| Strength of Materials | 3 | 4 | 11 | High |
| Theory of Machines | 2 | 3 | 8 | High |
| Machine Design | 2 | 3 | 8 | High |
| Thermodynamics | 2 | 3 | 8 | High |
| Fluid Mechanics | 2 | 3 | 8 | High |
| Heat Transfer | 2 | 3 | 8 | High |
| Manufacturing | 3 | 4 | 11 | High |
| Industrial Engineering | 1 | 2 | 5 | Medium |
| Engineering Mechanics | 1 | 2 | 5 | Medium |
# Matrix Fundamentals
Rank: max linearly independent rows/columns
Rank(A) = Rank(Aᵀ) = Rank(AAᵀ)
det(A) = 0 → Singular, no inverse
A⁻¹ = adj(A)/det(A)
# Eigenvalues & Eigenvectors
det(A − λI) = 0 (Characteristic equation)
(A − λI)v = 0 (Eigenvector for each λ)
|A| = product of eigenvalues
tr(A) = sum of eigenvalues
# Solving Ax = b
rank(A) = rank([A|b]) = n → Unique solution
rank(A) = rank([A|b]) < n → Infinite solutions
rank(A) < rank([A|b]) → No solution
# Cayley-Hamilton: A satisfies its own char eqn
A² − (tr A)A + (det A)I = 0 (for 2×2)# Key Derivatives
d/dx (xⁿ) = nx^(n−1), d/dx (eˣ) = eˣ, d/dx (ln x) = 1/x
d/dx (sin x) = cos x, d/dx (cos x) = −sin x, d/dx (tan x) = sec²x
Product: (uv)' = u'v + uv'
Quotient: (u/v)' = (u'v − uv')/v²
Chain: (f∘g)' = f'(g(x))·g'(x)
# Key Integrals
∫ xⁿ dx = x^(n+1)/(n+1), ∫ eˣ dx = eˣ
∫ sin x dx = −cos x, ∫ cos x dx = sin x
∫ dx/x = ln|x|
∫₀^∞ e^(−ax) dx = 1/a
∫₋∞^∞ e^(−x²) dx = √π
∫₀^(2π) sin²x dx = π, ∫₀^(2π) cos²x dx = π
# Partial Derivatives
∇f = (∂f/∂x, ∂f/∂y, ∂f/∂z) — Gradient
∇·F = ∂Fx/∂x + ∂Fy/∂y + ∂Fz/∂z — Divergence
∇×F — Curl (determinant of partial derivatives)
∇²f = ∂²f/∂x² + ∂²f/∂y² + ∂²f/∂z² — Laplacian
# Taylor Series
f(x) = f(a) + f'(a)(x−a) + f''(a)(x−a)²/2! + ...
# Maxima/Minima
∂f/∂x = 0, ∂f/∂y = 0 → critical point
D = fₓₓfᵧᵧ − f²ₓᵧ
D > 0, fₓₓ > 0 → Min | D > 0, fₓₓ < 0 → Max | D < 0 → Saddle# First Order ODE: dy/dx + Py = Q
Integrating Factor: IF = e^(∫P dx)
Solution: y × IF = ∫(Q × IF)dx + C
# Second Order ODE: ay'' + by' + cy = 0
Characteristic: ar² + br + c = 0
D = b² − 4ac:
D > 0: y = C₁e^(r₁x) + C₂e^(r₂x) (distinct real)
D = 0: y = (C₁ + C₂x)e^(rx) (repeated real)
D < 0: y = e^(αx)(C₁cosβx + C₂sinβx) (complex α±jβ)
# Special Forms
Euler-Cauchy: ax²y'' + bxy' + cy = 0
Try y = xᵐ, solve for m
# Laplace Transform
L{tⁿ} = n!/s^(n+1)
L{e^(at)} = 1/(s−a)
L{sin(at)} = a/(s²+a²)
L{cos(at)} = s/(s²+a²)
L{f'(t)} = sF(s) − f(0)
L{f''(t)} = s²F(s) − sf(0) − f'(0)# Probability
P(A∪B) = P(A) + P(B) − P(A∩B)
P(A|B) = P(A∩B)/P(B)
Bayes: P(Aᵢ|B) = P(B|Aᵢ)P(Aᵢ) / ΣP(B|Aⱼ)P(Aⱼ)
# Random Variables
E[X] = μ, Var(X) = E[X²]−μ² = σ²
E[aX+b] = aμ+b, Var(aX+b) = a²σ²
# Distributions
Binomial(n,p): E = np, Var = np(1−p)
Poisson(λ): E = λ, Var = λ
Normal(μ,σ²): Z = (X−μ)/σ ~ N(0,1)
Exponential(λ): E = 1/λ, Var = 1/λ²
Standard Normal: P(X ≤ x) = Φ(x)
# Regression
y = a + bx
b = Σ(xᵢ−x̄)(yᵢ−ȳ) / Σ(xᵢ−x̄)² = r·(Sy/Sx)
a = ȳ − bx̄
r = correlation coefficient = covariance/(Sx·Sy)
# Central Limit Theorem
(X̄ − μ)/(σ/√n) ~ N(0,1) for large n# Root Finding
Bisection: x = (a+b)/2, Error ≤ (b−a)/2ⁿ after n iterations
Newton-Raphson: x_{n+1} = x_n − f(x_n)/f'(x_n)
Convergence: order 2 (quadratic)
Secant: x_{n+1} = x_n − f(x_n)(x_n−x_{n-1})/(f(x_n)−f(x_{n-1}))
Regula-Falsi: Like bisection but uses linear interpolation
# Numerical Integration (Trapezoidal, Simpson's)
Trapezoidal: I ≈ (h/2)[y₀ + 2(y₁+...+y_{n-1}) + yₙ]
Simpson's 1/3: I ≈ (h/3)[y₀ + 4y₁ + 2y₂ + 4y₃ + ... + yₙ] (n = even)
Error: Trapezoidal O(h²), Simpson O(h⁴)
# ODE — Euler's Method
y_{n+1} = y_n + h·f(x_n, y_n)
Error: O(h) — first order
Modified Euler (Heun): y* = y_n + hf(x_n,y_n), y_{n+1} = y_n + (h/2)[f(x_n,y_n)+f(x_{n+1},y*)]
# Curve Fitting
Least squares: minimize Σ(yᵢ−(a+bxᵢ))²
System of equations solved for a, b# Fundamental Relations
σ = F/A (Stress = Force / Area)
ε = ΔL/L (Strain = Change in length / Original length)
E = σ/ε (Young's Modulus)
δ = FL/AE (Elongation = Force × Length / (Area × Modulus))
Poisson's Ratio: μ = −ε_lateral/ε_axial (0.25–0.35 for metals)
# Stresses
Normal stress: σ = P/A
Shear stress: τ = P/A (parallel to cross-section)
Bearing stress: σ_b = P/(d×t)
Thermal stress: σ_th = E·α·ΔT (if constrained)
# Shear Strain & Modulus
G = τ/γ (Shear Modulus = Shear stress / Shear strain)
E = 2G(1+μ) (Relation between E, G, μ)
# Bulk Modulus
K = −V·dP/dV
E = 3K(1−2μ)
# Compound Bar
P = P₁ + P₂
δ₁ = δ₂ (same deformation for parallel bars)
σ₁A₁ + σ₂A₂ = P
# Three-Dimensional State
σ_x, σ_y, σ_z = normal stresses
τ_xy, τ_yz, τ_zx = shear stresses
Principal stresses from stress tensor
ε_x = (1/E)[σ_x − μ(σ_y + σ_z)]
γ_xy = τ_xy/G# Principal Stresses (2D)
σ₁,₂ = (σₓ + σᵧ)/2 ± √[((σₓ−σᵧ)/2)² + τ²ₓᵧ]
τ_max = (σ₁ − σ₂)/2 = √[((σₓ−σᵧ)/2)² + τ²ₓᵧ]
Angle of principal plane:
tan(2θ_p) = 2τₓᵧ / (σₓ − σᵧ)
Angle of max shear:
tan(2θ_s) = −(σₓ − σᵧ) / (2τₓᵧ)
# Mohr's Circle
Center: C = ((σₓ+σᵧ)/2, 0)
Radius: R = √[((σₓ−σᵧ)/2)² + τ²ₓᵧ]
σ₁ = C + R, σ₂ = C − R
τ_max = R
Points on circle:
(σₓ, τₓᵧ) and (σᵧ, −τₓᵧ)
# Theories of Failure
1. Maximum Principal Stress (Rankine): σ₁ ≤ σ_yield
2. Maximum Shear Stress (Tresca): τ_max = (σ₁−σ₃)/2 ≤ σ_y/2
3. Maximum Distortion Energy (von Mises):
σ_eq = √[½((σ₁−σ₂)² + (σ₂−σ₃)² + (σ₃−σ₁)²)] ≤ σ_y
4. Maximum Strain Energy (Haigh-Beltrami)
5. Maximum Principal Strain (St. Venant)
von Mises is most widely used for ductile materials# Bending Equation
M/I = σ/y = E/R
M = bending moment, I = moment of inertia
σ = bending stress, y = distance from neutral axis
R = radius of curvature
σ_max = M·y_max/I = M/Z (Z = section modulus = I/y_max)
# Shear Force & Bending Moment
SF: V = dM/dx
BM: dV/dx = −w (distributed load w per unit length)
d²M/dx² = −w
Point load → SF changes by load magnitude
UDL → SF varies linearly, BM varies parabolically
# Common Beam Results (Simply Supported, length L)
Central point load P:
M_max = PL/4 (at center)
R_A = R_B = P/2
UDL w throughout:
M_max = wL²/8 (at center)
R_A = R_B = wL/2
# Cantilever, length L, tip load P:
M_max = PL (at fixed end)
Deflection δ = PL³/(3EI)
UDL w on cantilever:
M_max = wL²/2 (at fixed end)
Deflection δ = wL⁴/(8EI)
# Deflection Methods
Double Integration: EI d²y/dx² = M(x)
Macaulay's Method: Use singularity functions
Superposition: Add deflections from individual loads# Torsion (Circular Shaft)
T/J = τ/r = Gθ/L
T = torque, J = polar moment of inertia
τ = shear stress at radius r
θ = angle of twist, L = length
J = πd⁴/32 (solid shaft)
J = π(D⁴−d⁴)/32 (hollow shaft)
Power: P = T × ω = 2πNT/60
τ_max = T·r_max/J = 16T/(πd³) (solid)
# Columns & Euler's Buckling
P_cr = π²EI/(Le)² (Euler's critical load)
End conditions → Effective length Le:
Both pinned: Le = L
Fixed-free: Le = 2L
Fixed-fixed: Le = L/2
Fixed-pinned: Le = 0.7L
Slenderness ratio: λ = Le/r_min (r = radius of gyration)
Rankine: 1/P_r = 1/P_e + 1/P_c
# Springs
Helical Spring:
Deflection: δ = 8PD³n/(Gd⁴)
Stiffness: k = Gd⁴/(8D³n)
Shear stress: τ = 8PD/(πd³) × K (Wahl factor)
K = (4C−1)/(4C−4) + 0.615/C where C = D/d (spring index)
Spring in series: 1/k_eq = 1/k₁ + 1/k₂
Spring in parallel: k_eq = k₁ + k₂
# Thin Cylinders & Spheres
Thin cylinder (r/t > 20):
Hoop stress σ_h = Pr/t
Longitudinal stress σ_l = Pr/(2t)
Volumetric strain: ΔV/V = (Pr/tE)(5/2 − μ)
Thin sphere:
σ = Pr/(2t)
ΔV/V = 3Pr/(2tE)(1−μ)# Bolted Joints
Bolt strength: P = σ_t × A_tc (A_tc = tensile stress area)
Preload: F_i = K_i × Proof load
External load sharing: F_b = F_e × k_b/(k_b+k_m)
F_m = F_i − F_e × k_b/(k_b+k_m) (must remain > 0)
Shear: τ = P/(n × A) where n = number of bolts
Bearing: σ_b = P/(n × d × t)
# Welded Joints
Fillet weld (throat area):
Throat = 0.707 × leg size (s)
Strength = σ × (throat × length)
Butt weld:
Tensile strength = σ_all × throat area
Throat = thickness of thinner plate
# Keys
Square key: width w = d/4, height h = d/4
Shear area = w × L
Crushing area = h/2 × L
Shaft-key coupling:
Torque by shear: T = τ × w × L × (d/2)
Torque by crushing: T = σ_c × (h/2) × L × (d/2)# Spur Gear Terminology
Module: m = d/z (pitch diameter / teeth)
Addendum: a = m (tooth height above pitch circle)
Dedendum: b = 1.25m (tooth below pitch circle)
Clearance: c = 0.25m
Tooth height: h = a + b = 2.25m
Circular pitch: p = πd/z = πm
Base pitch: p_b = p × cos(φ)
# Gear Forces
Tangential: F_t = 2T/d
Radial: F_r = F_t × tan(φ)
Total: F = F_t / cos(φ) where φ = pressure angle
# Lewis Equation (Bending)
σ = F_t / (b × m × Y)
Y = Lewis form factor (depends on # teeth)
F_t = σ_all × b × m × Y
# Gear Ratio
Speed ratio = N₁/N₂ = z₂/z₁ = d₂/d₁
# Helical Gears
F_t = 2T/d
F_a = F_t × tan(ψ) (axial)
F_r = F_t × tan(φ)/cos(ψ)
Normal module: m_n = m × cos(ψ)# Journal Bearings
Sommerfeld Number: S = (r/c)² × μN/P
r = radius, c = clearance, μ = viscosity, N = speed, P = load/area
L/D ratio: typically 1 (for optimal performance)
# Rolling Contact Bearings
Life: L₁₀ = (C/P)^p × 10⁶ revolutions
C = dynamic capacity, P = equivalent load
p = 3 (ball bearings), p = 10/3 (roller bearings)
For reliability R: L = L₁₀ × (log(1/R)/log(1/0.9))^(1/p)
Equivalent load: P = XF_r + YF_a
X, Y depend on F_a/(VF_r) ratio (V = rotation factor)
# Fatigue Design
Endurance limit: σ_e = 0.5 × σ_ut (for steel)
Modified: σ_e' = σ_e × k_a × k_b × k_c × k_d × k_e
Soderberg line: σ_a/σ_e + σ_m/σ_y = 1/n
Goodman line: σ_a/σ_e + σ_m/σ_ut = 1/n
Gerber parabola: (nσ_a/σ_e)² + nσ_m/σ_ut = 1
Modified Goodman: σ_a/σ_e + σ_m/σ_ut = 1/n (most used)
Stress concentration: K_t (theoretical), K_f (fatigue)
Notch sensitivity: q = (K_f − 1)/(K_t − 1)# Zeroth Law
If A is in thermal equilibrium with B, and B with C → A in eq with C
Basis of temperature measurement
# First Law (Energy Conservation)
δQ = δW + dU (closed system)
dU = m·cv·dT (ideal gas, constant volume)
δQ = n·Cᵥ·dT or δW = P·dV
Steady Flow Energy Equation (SFEE):
Q̇ − Ẇ = ṁ[(h₂ − h₁) + (V₂²−V₁²)/2 + g(z₂−z₁)]
# Second Law
Kelvin-Planck: No 100% efficient heat engine
Clausius: Heat cannot flow from cold to hot without work
Entropy: dS ≥ δQ/T
For reversible: ΔS = ∫δQ/T = Q/T (isothermal)
Carnot: η = 1 − T_cold/T_hot (maximum possible)
COP (refrigerator) = T_cold/(T_hot − T_cold)
COP (heat pump) = T_hot/(T_hot − T_cold)
# Ideal Gas Relations
PV = nRT, PV = mRT
R_universal = 8.314 J/(mol·K)
R_specific = R/M
cp − cv = R, γ = cp/cv
For air: cp = 1.005 kJ/kgK, cv = 0.718 kJ/kgK, γ = 1.4
# Processes (Ideal Gas)
Isothermal: PV = const, W = nRT ln(V₂/V₁)
Adiabatic: PV^γ = const, T₁V₁^(γ−1) = T₂V₂^(γ−1)
Polytropic: PVⁿ = const
Isobaric: P = const, W = P(V₂−V₁)
Isochoric: V = const, W = 0# Otto Cycle (Petrol Engine)
Processes: 1-2 Isentropic comp, 2-3 Const vol heat add
3-4 Isentropic exp, 4-1 Const vol heat reject
η = 1 − 1/r^(γ−1)
r = compression ratio = V₁/V₂
# Diesel Cycle
1-2 Isentropic comp, 2-3 Const pressure heat add
3-4 Isentropic exp, 4-1 Const vol heat reject
η = 1 − (1/r^(γ−1)) × [(ρ^γ − 1)/(γ(ρ−1))]
ρ = cutoff ratio = V₃/V₂
# Dual Cycle
Combination of Otto + Diesel
η = 1 − (1/r^(γ−1)) × [(r_p·ρ^γ − 1)/((r_p−1)+γ·r_p(ρ−1))]
r_p = pressure ratio = P₃/P₂
# Rankine Cycle (Steam Power)
1-2 Pump (isentropic), 2-3 Boiler (const P)
3-4 Turbine (isentropic), 4-4' Condenser (const P)
η = (h₁ − h₂ − h₄ + h₃) / (h₁ − h₃)
W_pump = h₃ − h₂ = v_f₂(P₂ − P₁) ≈ v_f(P_high − P_low)
With reheat & regeneration improves efficiency
# Brayton Cycle (Gas Turbine)
1-2 Isentropic comp, 2-3 Const P heat add
3-4 Isentropic exp (turbine), 4-1 Const P heat reject
η = 1 − 1/r_p^((γ−1)/γ)
r_p = pressure ratio = P₂/P₁
# Refrigeration Cycles
VCC (Vapor Compression):
COP = (h₁ − h₄)/(h₂ − h₁)
h₂ from isentropic compression of superheated vapor# Conduction (Fourier's Law)
q = −kA·dT/dx (W)
Q = kA(T₁−T₂)/L (flat wall, steady state)
Composite wall: Q = ΔT_total / Σ(Lᵢ/kᵢAᵢ)
Thermal resistance: R_th = L/(kA) [K/W]
Series: R_total = R₁ + R₂ + ... (add resistances)
Parallel: 1/R_total = 1/R₁ + 1/R₂ + ...
Cylindrical: Q = 2πkL(T₁−T₂)/ln(r₂/r₁)
Spherical: Q = 4πk(T₁−T₂)/(1/r₁ − 1/r₂)
Critical insulation radius (cylinder): r_cr = k/h
# Convection (Newton's Law)
q = hA(T_s − T_∞)
h = convective heat transfer coefficient [W/m²K]
Dimensionless Numbers:
Nu = hL/k (Nusselt)
Re = ρVL/μ (Reynolds)
Pr = μcp/k (Prandtl)
Gr = ρ²gβΔTL³/μ² (Grashof)
Forced convection correlations:
Laminar (Re < 5×10⁵): Nu = 0.664·Re^(1/2)·Pr^(1/3)
Turbulent (Re > 5×10⁵): Nu = 0.037·Re^(4/5)·Pr^(1/3)
Natural convection: Nu = C·(Gr·Pr)^n
# Radiation (Stefan-Boltzmann)
q = εσA(T_s⁴ − T_surr⁴)
σ = 5.67×10⁻⁸ W/(m²·K⁴)
ε = emissivity (0–1)
View factors: F₁₂ = radiation from surface 1 reaching surface 2
Reciprocity: A₁F₁₂ = A₂F₂₁
Summation: ΣF₁ᵢ = 1
Radiation shield: R_shield = R₁ + R₂ (parallel for series of 2)
# Heat Exchanger
LMTD: ΔT_m = (ΔT₁ − ΔT₂)/ln(ΔT₁/ΔT₂)
Counter-flow is more effective than parallel-flow
NTU (Number of Transfer Units): NTU = UA/C_min
ε (Effectiveness) = Q_actual/Q_max# Casting
Solidification time (Chvorinov's Rule):
t = C × (V/A)²
V = volume, A = surface area, C = mold constant
Riser design: t_riser > t_casting
Risers should solidify last → placed near heavy sections
Pattern allowances:
Shrinkage (1–2%), Draft (1–3°), Machining, Shake, Distortion
Types: Sand, Die, Investment, Centrifugal, Shell molding
# Welding
Heat input: H = V × I / (v × 1000) [kJ/mm]
V = voltage, I = current, v = welding speed
Melt efficiency: μ_melt = H_melt / H_input
Types: Arc (SMAW, GTAW/TIG, GMAW/MIG), Gas, Resistance, Laser
Weld defects: Porosity, Slag inclusion, Lack of fusion,
Cracking (hot/cold), Undercut, Spatter
# Metal Forming
True strain: ε = ln(A₀/A_f) = ln(L_f/L₀)
Engineering strain: e = (L_f − L₀)/L₀
Forging:
Force: F = σ_f × A_f × (1 + μD/(3h))
Open-die vs Closed-die
Rolling:
Bite condition: μ ≥ tan(α) where α = entry angle
Draft: Δh = h₁ − h₂ = 2R(1 − cosα)
Power: P = 2πNR × Torque
Extrusion:
Force: F = A₀ × σ_avg × ln(A₀/A_f) (ideal)
Extrusion ratio: R = A₀/A_f
Sheet Metal:
Deep drawing: LDR = blank dia / punch dia (max ≈ 2 for steel)
Blanking force: F = πdt × τ_u
Punching force: F = πdt × τ_u# Turning
Cutting speed: V = πDN/1000 (m/min)
Material Removal Rate: MRR = V × f × d (mm³/min)
f = feed rate (mm/rev), d = depth of cut (mm)
Machine time: T_m = L/(f×N)
L = length of cut + approach + overtravel
Power: P = (Fc × V) / (60 × 10³) [kW]
Fc = cutting force
# Taylor's Tool Life
VT^n = C
V = cutting speed, T = tool life, n, C = constants
Economic (Taylor): VT^n = C for minimum cost
Modified: V₁T₁^n₁ = V₂T₂^n₂ (same tool/work)
# Drilling
MRR = (π/4)D² × f × N
Thrust force: F_thrust ≈ 2 × F_c
# Milling
MRR = w × d × f × N (w = width, d = depth)
Up milling: cutter rotation opposes feed
Down milling: cutter rotation same as feed (better finish)
# Thread Cutting
Pitch = 1/N (N = TPI)
Lead = pitch × number of starts
# Tool Geometry (ASA)
Rake angle (α), Clearance angle (γ), Cutting edge angle (φ)
Inclination angle (λ), Nose radius (r)
Merchant's circle:
F = Fc/cos(β−α) where β = friction angle
Chip thickness ratio: r = t₁/t₂ = sin(φ)/sin(φ+β−α)
Shear angle: φ = π/4 + α/2 − β/2 (Merchant's relation)
Shear strain: γ = cos α / sin φ cos(φ−α)# Limits, Fits & Tolerances
Fundamental deviation: H (hole basis), h (shaft basis)
IT grades: IT01 to IT18 (IT01 = finest, IT18 = coarsest)
Allowance = Min(hole) − Max(shaft) = negative for interference fit
Fits:
Clearance: hole > shaft
Interference: shaft > hole
Transition: may be either
# Interchangeability & Selective Assembly
Tolerance = Upper limit − Lower limit
# Ergonomics & Work Study
Method study: Record, Examine, Develop, Install, Maintain
Time study: Observed time × Performance rating × Allowance
Normal time = Observed time × Rating factor
Standard time = Normal time × (1 + Allowance %)
# Forecasting
Moving average: F(t+1) = (1/n) Σ D(t−i+1)
Exponential smoothing: F(t+1) = αD(t) + (1−α)F(t)
# Inventory
EOQ = √(2DS/H)
D = demand, S = order cost, H = holding cost
Total cost = (D/Q)S + (Q/2)H
Reorder point: ROP = d × L (demand × lead time)
Safety stock: SS = z × σ_d × √L# Linear Programming (Simplex Method)
Standard form: Maximize Z = c^T x
Subject to: Ax ≤ b, x ≥ 0
Add slack variables for ≤ constraints
Add surplus & artificial for ≥ constraints
Pivot on most negative entry in Z row (maximization)
Degeneracy: zero in RHS → multiple optimal solutions
Unbounded: no pivot restriction in min ratio test
Infeasible: artificial variable in final basis
# Transportation Problem
Initial solution: North-West Corner, VOGEL (best), LCM
Optimality test: MODI method (u_i + v_j = c_ij)
Allocate to most negative cell (δᵢⱼ = cᵢⱼ − uᵢ − vⱼ)
Degeneracy: #allocations ≠ m+n−1 → add ε
# Assignment Problem
Special case of transportation (all supplies = 1)
Hungarian method: row reduction, column reduction, covering zeros
Min lines = n → optimal, else adjust and repeat
# Network (CPM/PERT)
CPM: deterministic times, single estimate
PERT: probabilistic times, 3 estimates
t_e = (t_o + 4t_m + t_p)/6
σ² = ((t_p − t_o)/6)²
ES, EF, LS, LF, Float = LS − ES = LF − EF
Critical path: longest path, zero float
# Queuing Theory (M/M/1)
λ = arrival rate, μ = service rate
ρ = λ/μ (utilization, must be < 1)
L_s = λ/(μ−λ), L_q = ρ²/(1−ρ) = λ²/[μ(μ−λ)]
W_s = 1/(μ−λ), W_q = λ/[μ(μ−λ)]# Properties
Density: ρ = m/V (kg/m³)
Specific weight: γ = ρg (N/m³)
Specific gravity: SG = ρ/ρ_water
Viscosity: μ (dynamic, Pa·s), ν = μ/ρ (kinematic, m²/s)
Surface tension: σ (N/m)
Compressibility: β = −(1/V)(dV/dP)
Water at 20°C: ρ = 998 kg/m³, μ = 1.002×10⁻³ Pa·s
# Fluid Statics
P = P₀ + ρgh (Pascal's law)
Gauge pressure: P_gauge = P − P_atm
P_atm = 101.325 kPa = 1 atm = 760 mmHg
Manometer: P = ρgh (simple)
Differential: ΔP = (ρ₂−ρ₁)gh (U-tube)
Force on submerged surface:
F = ρg × h̄ × A
h̄ = centroid depth
Center of pressure: h* = h̄ + I_G/(Ah̄)
I_G = second moment of area about centroidal axis
# Buoyancy
F_b = ρ_fluid × g × V_displaced (Archimedes)
Metacentric height (GM):
GM > 0 → stable, GM < 0 → unstable
GM = BM − BG = I/V_sub − BG# Continuity Equation
A₁V₁ = A₂V₂ (incompressible, steady)
ṁ = ρAV = const (mass conservation)
# Bernoulli's Equation (along streamline)
P/ρg + V²/2g + z = const (head form)
P + ½ρV² + ρgz = const (energy form)
V₁²/(2g) + P₁/(ρg) + z₁ = V₂²/(2g) + P₂/(ρg) + z₂ + losses
# Reynolds Number
Re = ρVD/μ = VD/ν
Pipe flow:
Re < 2300 → Laminar
Re > 4000 → Turbulent
2300 < Re < 4000 → Transition
# Laminar Flow in Pipes
V_max = 2V_avg (parabolic profile)
V(r) = (ΔP/4μL)(R²−r²)
f = 64/Re (Darcy friction factor)
h_f = fLV²/(2gD) = 32μLV/(ρgD²) (Hagen-Poiseuille)
# Turbulent Flow
f = 0.316/Re^(1/4) (Blasius, smooth pipe, Re < 10⁵)
Colebrook-White: 1/√f = −2log₁₀[(ε/D)/3.7 + 2.51/(Re√f)]
# Minor Losses
h_L = K V²/(2g)
K = loss coefficient
Sudden expansion: K = (1−A₁/A₂)²
Sudden contraction: K ≈ 0.5 (typical)
Exit to reservoir: K = 1.0
Entrance from reservoir: K = 0.5
# Pumps & Turbines
Pump power: P = ρgQH/η_pump
Specific speed: N_s = N√Q/H^(3/4)
Cavitation: NPSH_available > NPSH_required| Subject | Book | Author |
|---|---|---|
| Engineering Math | Higher Engineering Mathematics | B.S. Grewal |
| SOM | Strength of Materials | R.K. Rajput / Timoshenko |
| Theory of Machines | Theory of Machines | S.S. Rattan |
| Machine Design | Machine Design | V.B. Bhandari |
| Fluid Mechanics | Fluid Mechanics | R.K. Bansal |
| Thermodynamics | Engineering Thermodynamics | P.K. Nag |
| Heat Transfer | Heat Transfer | J.P. Holman |
| Manufacturing | Manufacturing Technology | P.N. Rao |
| Industrial Engg | Industrial Engineering & OR | O.P. Khanna |
| Year | Qualifying | PSU/IIT Range |
|---|---|---|
| 2024 | 28.4 | 600–850 score |
| 2023 | 28.7 | 600–850 score |
| 2022 | 28.1 | 600–850 score |
| 2021 | 29.0 | 600–850 score |
| 2020 | 34.0 | 600–850 score |