GATE GUIDE

GATE ME Formula Sheet 2027: Key Formulas by Subject

By MD ANISH AHAMADUpdated 4 Oct 20268 min read
GATE ME Formula Sheet 2027: Key Formulas by Subject

This GATE ME formula sheet collects the formulas mechanical engineering questions lean on most, grouped by subject, with the condition or trap to watch for beside each. It is a free selection from the last-minute sheet in the GATE ME 2027 book. Use it to test your recall, then practise each formula on previous-year questions.

In this guide
  1. Key takeaways
  2. How to read this sheet
  3. Engineering Mathematics
  4. Engineering Mechanics
  5. Mechanics of Materials
  6. Theory of Machines and Vibrations
  7. Machine Design
  8. Fluid Mechanics
  9. Heat Transfer
  10. Thermodynamics and Applications
  11. Materials, Manufacturing and Metrology
  12. Industrial Engineering
  13. General Aptitude essentials
  14. How to use a formula sheet in the exam
  15. Subject-wise formula sheets
  16. Quick revision

Key takeaways

How to read this sheet

SI units are used throughout, with g=9.81 m/s2g = 9.81\ \text{m/s}^2. ln⁡\ln is the natural logarithm, and angles inside formulas are in radians. Subscript 1 is an inlet or initial state; subscript 2 is an exit or final state.

The condition of a formula is what must be true for it to hold: steady flow, small damping, a constant failure rate. The Watch out for column gives that condition or the slip that most often costs marks. A formula used outside its condition gives a confident wrong answer.

Engineering Mathematics

Formula Watch out for
∑λi=trace⁡A\sum \lambda_i = \operatorname{trace} A, ∏λi=det⁡A\prod \lambda_i = \det A; AkA^k has λk\lambda^k, A−1A^{-1} has 1/λ1/\lambda Triangular matrix: eigenvalues sit on the diagonal
Ax=bAx = b has a unique solution iff rank⁡A=rank⁡ [A∣b]=n\operatorname{rank} A = \operatorname{rank}\,[A \mid b] = n Equal ranks below nn give infinitely many
rt−s2>0rt - s^2 > 0 and r>0r > 0: minimum; r<0r < 0: maximum (r=fxxr = f_{xx}, s=fxys = f_{xy}, t=fyyt = f_{yy}) rt−s2<0rt - s^2 < 0 is a saddle point
L{eat}=1s−a\displaystyle \mathcal{L}\{e^{at}\} = \frac{1}{s - a}; L{f′}=sF(s)−f(0)\mathcal{L}\{f'\} = sF(s) - f(0) Final value theorem needs every pole of sF(s)sF(s) in the left half-plane
∮f(z)z−a dz=2πi f(a)\displaystyle \oint \frac{f(z)}{z - a}\,dz = 2\pi i\,f(a) Only for aa inside the curve
Poisson P(k)=e−λλkk!\displaystyle P(k) = \frac{e^{-\lambda}\lambda^k}{k!}, mean == variance =λ= \lambda; Binomial mean npnp, variance np(1−p)np(1 - p) Sample variance divides by n−1n - 1
xn+1=xn−f(xn)f′(xn)\displaystyle x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)} Fails when f′f' is near zero
Simpson's rule h3[y0+4(y1+y3+⋯ )+2(y2+y4+⋯ )+yn]\displaystyle \frac{h}{3}\big[y_0 + 4(y_1 + y_3 + \cdots) + 2(y_2 + y_4 + \cdots) + y_n\big] nn must be even; exact for cubics

Engineering Mechanics

Formula Watch out for
Belt or band T1T2=eμθ\displaystyle \frac{T_1}{T_2} = e^{\mu\theta} θ\theta in radians; T1T_1 is the tight side
Screw jack η=tan⁡αtan⁡(α+ϕ)\displaystyle \eta = \frac{\tan\alpha}{\tan(\alpha + \phi)}; self-locking iff ϕ>α\phi > \alpha Self-locking keeps η\eta below 50 per cent
Plane truss determinate and rigid when m=2j−3m = 2j - 3 Zero-force members at unloaded joints
Rolling down an incline a=gsin⁡θ1+k2/r2\displaystyle a = \frac{g\sin\theta}{1 + k^2/r^2} Disc 23gsin⁡θ\displaystyle \frac{2}{3}g\sin\theta, solid sphere 57gsin⁡θ\displaystyle \frac{5}{7}g\sin\theta
Irod, centre=mL212\displaystyle I_{\text{rod, centre}} = \frac{mL^2}{12}, Irod, end=mL23\displaystyle I_{\text{rod, end}} = \frac{mL^2}{3}; I=IG+md2I = I_G + md^2 Parallel axis only from the centroidal axis
e=v2′−v1′u1−u2\displaystyle e = \frac{v_2' - v_1'}{u_1 - u_2} e=1e = 1 elastic, e=0e = 0 plastic

Mechanics of Materials

Formula Watch out for
E=2G(1+ν)=3K(1−2ν)E = 2G(1 + \nu) = 3K(1 - 2\nu) 0≤ν≤0.50 \le \nu \le 0.5
σ1,2=σx+σy2±(σx−σy2)2+τxy2\displaystyle \sigma_{1,2} = \frac{\sigma_x + \sigma_y}{2} \pm \sqrt{\left(\frac{\sigma_x - \sigma_y}{2}\right)^2 + \tau_{xy}^2} Angle θ\theta on the element is 2θ2\theta on Mohr's circle
Thin cylinder: hoop pd2t\displaystyle \frac{pd}{2t}, longitudinal pd4t\displaystyle \frac{pd}{4t}; thin sphere pd4t\displaystyle \frac{pd}{4t} Thin wall only, tt below about d/20d/20
MI=σy=ER\displaystyle \frac{M}{I} = \frac{\sigma}{y} = \frac{E}{R}; TJ=τr=GθL\displaystyle \frac{T}{J} = \frac{\tau}{r} = \frac{G\theta}{L} I=πd464\displaystyle I = \frac{\pi d^4}{64} for bending, J=πd432\displaystyle J = \frac{\pi d^4}{32} for torsion
δ\delta: cantilever end load PL33EI\displaystyle \frac{PL^3}{3EI}; simply supported central load PL348EI\displaystyle \frac{PL^3}{48EI}, UDL 5wL4384EI\displaystyle \frac{5wL^4}{384EI} ww is load per length
Pcr=π2EILe2\displaystyle P_{cr} = \frac{\pi^2 EI}{L_e^2}; Le=L,2L,L2,L2\displaystyle L_e = L, 2L, \frac{L}{2}, \frac{L}{\sqrt{2}} Pinned, fixed–free, fixed–fixed, fixed–pinned; use the least II
τ=VQIb\displaystyle \tau = \frac{VQ}{Ib} Rectangle: maximum is 1.5 times the mean

Remember: hoop stress is twice longitudinal stress, and JJ is twice II for a circle. Halving or doubling the wrong one is the commonest slip in this subject.

Theory of Machines and Vibrations

Formula Watch out for
Kutzbach F=3(n−1)−2j1−j2F = 3(n - 1) - 2j_1 - j_2 nn counts the frame
Grashof s+l≤p+qs + l \le p + q for a fully rotating link Which link is fixed decides the inversion
Coriolis component 2ωv2\omega v Only with sliding on a rotating link
Flywheel ΔE=Iω2Cs\Delta E = I\omega^2 C_s, Cs=ωmax⁡−ωmin⁡ωmean\displaystyle C_s = \frac{\omega_{\max} - \omega_{\min}}{\omega_{\text{mean}}} ω\omega in rad/s, not rpm
ωn=k/m=g/δst\omega_n = \sqrt{k/m} = \sqrt{g/\delta_{st}}; ζ=c2km\displaystyle \zeta = \frac{c}{2\sqrt{km}}; ωd=ωn1−ζ2\omega_d = \omega_n\sqrt{1 - \zeta^2} Series springs add as reciprocals
δ=ln⁡x1x2=2πζ1−ζ2\displaystyle \delta = \ln\frac{x_1}{x_2} = \frac{2\pi\zeta}{\sqrt{1 - \zeta^2}} ζ≈δ/(2π)\zeta \approx \delta/(2\pi) only when small
TR=1+(2ζr)2(1−r2)2+(2ζr)2\displaystyle TR = \frac{\sqrt{1 + (2\zeta r)^2}}{\sqrt{(1 - r^2)^2 + (2\zeta r)^2}}, r=ω/ωnr = \omega/\omega_n New in 2027; isolation only for r>2r > \sqrt{2}
PID Gc(s)=Kp+Kis+Kds\displaystyle G_c(s) = K_p + \frac{K_i}{s} + K_d s; overshoot e−πζ/1−ζ2e^{-\pi\zeta/\sqrt{1 - \zeta^2}} New in 2027; integral action removes the step offset

Machine Design

Formula Watch out for
Tresca σ1−σ3≤Sy/N\sigma_1 - \sigma_3 \le S_y/N; von Mises σ12−σ1σ2+σ22≤Sy/N\sqrt{\sigma_1^2 - \sigma_1\sigma_2 + \sigma_2^2} \le S_y/N Shear yield 0.5Sy0.5S_y against 0.577Sy0.577S_y
Shaft τmax⁡=16M2+T2πd3\displaystyle \tau_{\max} = \frac{16\sqrt{M^2 + T^2}}{\pi d^3} Equivalent moment uses 12[M+M2+T2]\displaystyle \frac{1}{2}\big[M + \sqrt{M^2 + T^2}\big]
Goodman σaSe+σmSut=1N\displaystyle \frac{\sigma_a}{S_e} + \frac{\sigma_m}{S_{ut}} = \frac{1}{N}; Soderberg uses SyS_y Soderberg is the most conservative
Kf=1+q(Kt−1)K_f = 1 + q(K_t - 1) 0≤q≤10 \le q \le 1
L10=(C/P)pL_{10} = (C/P)^p million revolutions p=3p = 3 ball, 10/310/3 roller
Spring δ=8FD3nGd4\displaystyle \delta = \frac{8FD^3 n}{Gd^4}; Kw=4C−14C−4+0.615C\displaystyle K_w = \frac{4C - 1}{4C - 4} + \frac{0.615}{C}, C=D/dC = D/d Wahl factor for stress, not deflection
Clutch, uniform wear T=μWR1+R22\displaystyle T = \mu W\frac{R_1 + R_2}{2} per friction surface Multiply by the number of surface pairs
Open belt L=π(D+d)2+2C+(D−d)24C\displaystyle L = \frac{\pi(D + d)}{2} + 2C + \frac{(D - d)^2}{4C} New in 2027; crossed belt uses (D+d)2(D + d)^2

This page gives a selection. The book's last-minute sheet covers every topic the 2027 syllabus names, each entry with its condition, plus a worked number recomputed before printing. It is part of the GATE ME 2027 book, alongside 942 questions with worked solutions and 10 full mock tests.

Fluid Mechanics

Formula Watch out for
F=ρghˉAF = \rho g\bar{h}A; centre of pressure at hˉ+IGsin⁡2θAhˉ\displaystyle \bar{h} + \frac{I_G\sin^2\theta}{A\bar{h}} hˉ\bar{h} is the depth of the centroid
GM=IV−BG\displaystyle GM = \frac{I}{V} - BG Stable only if GM>0GM > 0
pρg+V22g+z=constant\displaystyle \frac{p}{\rho g} + \frac{V^2}{2g} + z = \text{constant} Steady, incompressible, inviscid, along a streamline
Δp=32μVLD2\displaystyle \Delta p = \frac{32\mu VL}{D^2}; f=64Re\displaystyle f = \frac{64}{Re} Laminar only, below Re≈2000Re \approx 2000
hf=fLV22gD\displaystyle h_f = \frac{fLV^2}{2gD} ff is the Darcy factor
u=∂ψ∂y\displaystyle u = \frac{\partial\psi}{\partial y}, v=−∂ψ∂x\displaystyle v = -\frac{\partial\psi}{\partial x}; V⃗=∇ϕ\vec{V} = \nabla\phi New in 2027; ϕ\phi exists only for irrotational flow
T0T=1+γ−12M2\displaystyle \frac{T_0}{T} = 1 + \frac{\gamma - 1}{2}M^2; p∗p0=0.528\displaystyle \frac{p^*}{p_0} = 0.528 for γ=1.4\gamma = 1.4 New in 2027; a converging nozzle never exceeds M=1M = 1
dAA=(M2−1)dVV\displaystyle \frac{dA}{A} = (M^2 - 1)\frac{dV}{V} Supersonic flow speeds up in a diverging passage

Heat Transfer

Formula Watch out for
R=LkA\displaystyle R = \frac{L}{kA}; cylinder ln⁡(r2/r1)2πkL\displaystyle \frac{\ln(r_2/r_1)}{2\pi kL}; convection 1hA\displaystyle \frac{1}{hA} Series resistances add
Critical radius rc=k/hr_c = k/h (cylinder), 2k/h2k/h (sphere) Below rcr_c, insulation raises heat loss
m=hPkAc\displaystyle m = \sqrt{\frac{hP}{kA_c}}; q=hPkAc θbtanh⁡(mL)q = \sqrt{hPkA_c}\,\theta_b\tanh(mL) Insulated tip; correct the length for a convecting tip
T−T∞Ti−T∞=e−t/τ\displaystyle \frac{T - T_\infty}{T_i - T_\infty} = e^{-t/\tau}, τ=ρVchAs\displaystyle \tau = \frac{\rho Vc}{hA_s} Lumped only if Bi<0.1Bi < 0.1
Nu=0.023 Re0.8PrnNu = 0.023\,Re^{0.8}Pr^{n} n=0.4n = 0.4 heating the fluid, 0.30.3 cooling
ΔTlm=ΔT1−ΔT2ln⁡(ΔT1/ΔT2)\displaystyle \Delta T_{lm} = \frac{\Delta T_1 - \Delta T_2}{\ln(\Delta T_1/\Delta T_2)}; ε=NTU1+NTU\displaystyle \varepsilon = \frac{NTU}{1 + NTU} (counterflow, Cr=1C_r = 1) NTU=UA/Cmin⁡NTU = UA/C_{\min}
λmax⁡T=2898 μm K\lambda_{\max}T = 2898\ \mu\text{m K}; plates q=σ(T14−T24)1/ε1+1/ε2−1\displaystyle q = \frac{\sigma(T_1^4 - T_2^4)}{1/\varepsilon_1 + 1/\varepsilon_2 - 1} Kelvin only

Boiling and condensation, new in 2027, are mostly read off the pool-boiling curve: nucleate boiling gives the highest useful hh, and dropwise condensation beats filmwise.

Thermodynamics and Applications

Formula Watch out for
Q−W=ΔUQ - W = \Delta U; steady flow Q˙−W˙=m˙[Δh+ΔV22+gΔz]\displaystyle \dot{Q} - \dot{W} = \dot{m}\big[\Delta h + \frac{\Delta V^2}{2} + g\Delta z\big] Throttling: h2=h1h_2 = h_1
Polytropic W=p1V1−p2V2n−1\displaystyle W = \frac{p_1V_1 - p_2V_2}{n - 1}; isothermal p1V1ln⁡V2V1\displaystyle p_1V_1\ln\frac{V_2}{V_1} Absolute pressures
Δs=cpln⁡T2T1−Rln⁡p2p1\displaystyle \Delta s = c_p\ln\frac{T_2}{T_1} - R\ln\frac{p_2}{p_1} Kelvin inside the logarithm
ηCarnot=1−TLTH\displaystyle \eta_{\text{Carnot}} = 1 - \frac{T_L}{T_H}; COPHP=COPR+1COP_{HP} = COP_R + 1 Kelvin
Otto η=1−1rγ−1\displaystyle \eta = 1 - \frac{1}{r^{\gamma - 1}}; Brayton η=1−1rp(γ−1)/γ\displaystyle \eta = 1 - \frac{1}{r_p^{(\gamma - 1)/\gamma}} rr is a volume ratio, rpr_p a pressure ratio
CxHy+(x+y4)(O2+3.76N2)\displaystyle C_xH_y + \left(x + \frac{y}{4}\right)(O_2 + 3.76N_2); ϕ=(A/F)stoich(A/F)actual\displaystyle \phi = \frac{(A/F)_{\text{stoich}}}{(A/F)_{\text{actual}}} New in 2027; ϕ<1\phi < 1 is lean
COP=h1−h4h2−h1\displaystyle COP = \frac{h_1 - h_4}{h_2 - h_1}, with h4=h3h_4 = h_3 Throttle is isenthalpic
ω=0.622pvp−pv\displaystyle \omega = 0.622\frac{p_v}{p - p_v} Use total pressure pp
Turbine Ns=NPH5/4\displaystyle N_s = \frac{N\sqrt{P}}{H^{5/4}}; pump Ns=NQH3/4\displaystyle N_s = \frac{N\sqrt{Q}}{H^{3/4}} Pump characteristics are new in 2027

Trap: a turbine's isentropic efficiency is actual over ideal work, but a compressor's or pump's is ideal over actual. Inverting one gives a wrong answer that still looks plausible.

Materials, Manufacturing and Metrology

Formula Watch out for
Packing: BCC 0.68, FCC and HCP 0.74 BCC a=4r/3a = 4r/\sqrt{3}, FCC a=22ra = 2\sqrt{2}r
σt=σ(1+e)\sigma_t = \sigma(1 + e), εt=ln⁡(1+e)\varepsilon_t = \ln(1 + e) Valid up to necking only
Chvorinov ts=C(VA)2\displaystyle t_s = C\left(\frac{V}{A}\right)^2 Riser must freeze after the casting
Merchant 2ϕ+β−α=90∘2\phi + \beta - \alpha = 90^\circ; tan⁡ϕ=rcos⁡α1−rsin⁡α\displaystyle \tan\phi = \frac{r\cos\alpha}{1 - r\sin\alpha} r=t/tcr = t/t_c is below 1
Taylor VTn=CVT^n = C; least-cost life T=(1n−1)(tc+CtCm)\displaystyle T = \left(\frac{1}{n} - 1\right)\left(t_c + \frac{C_t}{C_m}\right) Maximum production drops the Ct/CmC_t/C_m term
Peak-to-valley roughness f28r\displaystyle \frac{f^2}{8r} rr is the nose radius
Tolerance unit i=0.45D1/3+0.001Di = 0.45D^{1/3} + 0.001D DD is a geometric mean, in mm
CNC step =pitch×step angle360∘\displaystyle = \frac{\text{pitch} \times \text{step angle}}{360^\circ}; cylinder force pApA out, p(A−a)p(A - a) in New in 2027

Industrial Engineering

Formula Watch out for
Q∗=2DSH\displaystyle Q^* = \sqrt{\frac{2DS}{H}}; EPQ Q∗=2DSH(1−d/p)\displaystyle Q^* = \sqrt{\frac{2DS}{H(1 - d/p)}} At Q∗Q^* ordering cost equals holding cost
Standard time == normal time ×(1+allowance)\times (1 + \text{allowance}) Work study is new in 2027
Ft+1=αDt+(1−α)FtF_{t+1} = \alpha D_t + (1 - \alpha)F_t Larger α\alpha responds faster
M/M/1: L=λμ−λ\displaystyle L = \frac{\lambda}{\mu - \lambda}, W=1μ−λ\displaystyle W = \frac{1}{\mu - \lambda}; L=λWL = \lambda W Needs λ<μ\lambda < \mu
PERT te=a+4m+b6\displaystyle t_e = \frac{a + 4m + b}{6}, σ=b−a6\displaystyle \sigma = \frac{b - a}{6} Add variances, not standard deviations
Series R=∏RiR = \prod R_i; parallel R=1−∏(1−Ri)R = 1 - \prod(1 - R_i); R(t)=e−λtR(t) = e^{-\lambda t} Constant failure rate only
DPMO=defects×106units×opportunities\displaystyle \text{DPMO} = \frac{\text{defects} \times 10^6}{\text{units} \times \text{opportunities}} New in 2027

General Aptitude essentials

The General Aptitude preparation guide covers the verbal and data interpretation side.

How to use a formula sheet in the exam

Read the sheet daily in the final two weeks. For each line, say its condition aloud before you use it. In the exam, write your five most fragile formulas on the rough sheet in the first five minutes; the exam-day rules guide explains what you may and may not carry.

Carry full precision on the GATE virtual calculator and round only the final NAT answer. Negative marks apply to MCQs only, as the marking scheme guide, written for CSE but common to every paper, explains.

In one line: a formula is worth a mark only when you know its units, its condition and its usual trap.

Subject-wise formula sheets

Each of these goes deeper on one part of the GATE ME paper, with a worked example and the trap for every formula:

Quick revision

  1. Convert rpm to rad/s with ω=2πN60\displaystyle \omega = \frac{2\pi N}{60}; MPa is N/mm2\text{N/mm}^2.
  2. Use kelvin inside any temperature ratio, power or exponential.
  3. Use absolute pressure in the ideal-gas law, isentropic ratios and choking.
  4. I=πd464\displaystyle I = \frac{\pi d^4}{64} for bending, J=πd432\displaystyle J = \frac{\pi d^4}{32} for torsion.
  5. Hoop stress pd2t\displaystyle \frac{pd}{2t} is twice longitudinal stress pd4t\displaystyle \frac{pd}{4t}.
  6. Isolation needs r>2r > \sqrt{2}; resonance amplitude is F0/k2ζ\displaystyle \frac{F_0/k}{2\zeta}.
  7. Lumped analysis only when Bi<0.1Bi < 0.1.
  8. EOQ 2DS/H\sqrt{2DS/H}; M/M/1 needs λ<μ\lambda < \mu.

Frequently asked questions

Can I take a formula sheet into the GATE ME exam?

No. Candidates cannot carry paper, a calculator, a phone or a watch into the exam hall. The exam provides a virtual calculator, rough sheets and a pen. A useful habit is to write a few easily forgotten formulas on the rough sheet in the first five minutes. Confirm the current exam-day rules at gate2027.iitm.ac.in before the exam.

What are the hoop and longitudinal stresses in a thin cylinder?

For a thin cylinder of diameter dd, wall thickness tt and internal pressure pp, the hoop stress is pd2t\displaystyle \frac{pd}{2t} and the longitudinal stress is pd4t\displaystyle \frac{pd}{4t}, half the hoop value. A thin sphere carries pd4t\displaystyle \frac{pd}{4t} in every direction. The results hold only for a thin wall, with tt below about d/20d/20.

When does a spring mounting isolate vibration?

Only when the frequency ratio r=ω/ωnr = \omega/\omega_n is greater than 2\sqrt{2}. Below that, the transmissibility ratio is above 1 and the mount passes on more force than it receives. At r=2r = \sqrt{2} it equals 1 for every damping ratio. Above 2\sqrt{2}, extra damping raises the transmitted force, so isolators use soft springs and light damping.

Which GATE ME 2027 topics are new and need formulas?

The 2027 syllabus names several topics for the first time. They include velocity potential and converging-diverging nozzles, transmissibility ratio, PID controllers and transfer functions, belt drives, boiling and condensation, combustion with air-fuel and equivalence ratio, pump characteristics, additive manufacturing, CNC and actuators, programmable logic controllers, work study and six sigma. Each has at least one formula or rule worth knowing.

How should I revise formulas before GATE ME?

Read a compact formula sheet once a day in the final two weeks and once more on the exam morning. For each formula, know the condition it needs and the trap built around it. Write the unit next to every number, use kelvin inside any temperature ratio, carry full precision and round only the final numerical answer.

Sources

Dates, fees and the syllabus are set by the GATE 2027 organising institute and can change. Always confirm at gate2027.iitm.ac.in.

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