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By Ajay Vatsyayan Classes Home Tutors Team Reviewed by Ajay Vatsyayan Last reviewed: 29 Sep 2026

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JEE Physics Formula Sheet: All 20 JEE Main Units on One Printable Page

This JEE physics formula sheet gives the key formulas for all 20 units of the official JEE Main 2026 Physics syllabus, in the same order as the NTA syllabus. Each unit has a compact table followed by a short "how to use / common traps" note, because most lost marks come from using a formula outside its conditions, not from forgetting it. The page is designed to print cleanly: use your browser's Print option.

A formula sheet is a revision tool, not a way to learn physics for the first time. If whole units feel unfamiliar, start with a JEE Physics tutor in Gurgaon and come back to this page for recall practice. When you are ready to turn formulas into marks, our guide on how to score 70+ in JEE Main Physics gives a week-by-week plan.

How to use this JEE physics formula sheet

Use the sheet for daily recall, not as reading material. It works as a JEE Main physics formula sheet first, and as a physics formula sheet for JEE covering all chapters of the current Main syllabus; the topics that only JEE Advanced names are listed separately at the end. The unit list follows the official JEE (Main) 2026 syllabus published by NTA, which has 20 physics units, from Units and Measurements to Experimental Skills. NTA can revise the syllabus, so check the current version on the official JEE Main website before your exam.

  • Cover and recall. Cover the formula column and write each result from memory. Anything you miss goes into your error log.
  • Learn the conditions. Many JEE physics formulas hold only in a special case: constant acceleration, a thin lens, an ideal gas, a point far from a dipole. The trap notes point these out.
  • Check dimensions. If you are unsure of a formula in the exam, a quick dimension check catches most wrong versions.
  • Notation. Bold letters are vectors, k = 1/(4πε0), and "≈" means an approximation valid only under the stated condition.

Units that are mostly Class 11 (Units 1 to 10) and mostly Class 12 (Units 11 to 19) are both here, so the sheet works for both years of preparation.

1. Units and measurements

ResultFormula or fact
SI base quantities7: length (m), mass (kg), time (s), current (A), temperature (K), amount of substance (mol), luminous intensity (cd)
Common dimensionsForce [MLT−2]; energy [ML2T−2]; power [ML2T−3]; pressure [ML−1T−2]; G [M−1L3T−2]; h [ML2T−1]
Error in a sum or differenceZ = A ± B → ΔZ = ΔA + ΔB
Error in a product or quotientZ = AB or A/B → ΔZ/Z = ΔA/A + ΔB/B
Error in a powerZ = An → ΔZ/Z = |n| ΔA/A
Significant figuresAddition/subtraction: keep the fewest decimal places. Multiplication/division: keep the fewest significant figures.

How to use / common traps: errors always add, even when quantities are subtracted or divided. Example: in g = 4π2l/T2, a 1% error in l and a 2% error in T give 1 + 2 × 2 = 5% error in g. Dimensional analysis cannot find dimensionless constants (such as 2π) and cannot derive relations that involve a sum of terms.

2. Kinematics

ResultFormula
Constant accelerationv = u + at; s = ut + ½at2; v2 = u2 + 2as
Distance in the nth secondsn = u + (a/2)(2n − 1)
GraphsSlope of x–t = velocity; slope of v–t = acceleration; area under v–t = displacement
Relative velocityvAB = vA − vB
Projectile (ground to ground)T = 2u sinθ/g; H = u2sin2θ/(2g); R = u2sin 2θ/g; Rmax = u2/g at θ = 45°
Trajectoryy = x tanθ − gx2/(2u2cos2θ)
Uniform circular motionv = ωr; centripetal acceleration a = v2/r = ω2r

How to use / common traps: the three equations of motion hold only for constant acceleration; if a depends on time or position, use a = dv/dt or a = v dv/dx and integrate. Fix one sign convention before substituting. Check: u = 20 m/s at 30° with g = 10 m/s2 gives T = 2 s, H = 5 m and R = 20√3 ≈ 34.6 m. Angles θ and 90° − θ give the same range.

3. Laws of motion

ResultFormula
Second lawF = dp/dt; F = ma for constant mass
ImpulseJ = ∫F dt = Δp
Conservation of momentumIf net external force = 0, total p is constant
FrictionStatic: fs ≤ μsN; kinetic: fk = μkN
Equilibrium of concurrent forcesΣF = 0; for three forces, Lami's theorem F1/sin α = F2/sin β = F3/sin γ (each angle is opposite its force)
Vehicle on a level roadvmax = √(μrg)
Banked roadNo friction needed at v = √(rg tanθ); with friction, vmax = √[rg(μ + tanθ)/(1 − μ tanθ)]

How to use / common traps: static friction is not always μsN. It takes whatever value (up to μsN) is needed to prevent slipping, so find the required friction first and compare. Draw a free-body diagram for each body in a connected system before writing equations. "Centripetal force" is not an extra force; it is the net inward force supplied by tension, friction, gravity or a normal reaction.

4. Work, energy and power

ResultFormula
WorkW = F·s = Fs cosθ (constant force); W = ∫F dx (variable force)
Work–energy theoremWnet = ΔK
Kinetic energy and momentumK = ½mv2 = p2/(2m)
Spring potential energyU = ½kx2
Conservative force and potential energyF = −dU/dx
PowerP = dW/dt = F·v
Vertical circle (string)Minimum speed at top √(gr); minimum speed at bottom to complete the circle √(5gr); Tbottom − Ttop = 6mg
1D elastic collisionv1 = [(m1 − m2)u1 + 2m2u2]/(m1 + m2); v2 = [(m2 − m1)u2 + 2m1u1]/(m1 + m2)
Coefficient of restitutione = (v2 − v1)/(u1 − u2); e = 1 elastic, e = 0 perfectly inelastic
KE lost, perfectly inelasticΔK = m1m2(u1 − u2)2/[2(m1 + m2)]

How to use / common traps: momentum is conserved in every collision, but kinetic energy only in elastic ones. In a 2D collision, conserve momentum separately along x and y. Mechanical energy is conserved only when non-conservative forces (friction, air drag) do no work; otherwise use Wnet = ΔK. For a rod or a mass on a rigid support, the minimum speed at the top of a vertical circle is zero, not √(gr).

5. Rotational motion

ResultFormula
Centre of massxcm = Σmixi/Σmi; for a rigid body xcm = ∫x dm/M
Torque and angular momentumτ = r × F; L = r × p; τ = dL/dt
Rigid body about a fixed axisL = Iω; τ = Iα; K = ½Iω2; W = τθ; P = τω
Conservation of angular momentumIf net external torque = 0: I1ω1 = I2ω2
Radius of gyrationI = Mk2
Parallel axes theoremI = Icm + Md2
Perpendicular axes theorem (plane lamina only)Iz = Ix + Iy
Standard moments of inertiaRing (axis) MR2; disc or solid cylinder (axis) ½MR2; solid sphere (2/5)MR2; hollow sphere (2/3)MR2; rod about centre ML2/12; rod about one end ML2/3; ring about a diameter ½MR2; disc about a diameter ¼MR2
Linear–rotational analogym ↔ I; v ↔ ω; a ↔ α; F ↔ τ; p ↔ L

How to use / common traps: the parallel axes theorem must start from the axis through the centre of mass; you cannot jump between two arbitrary parallel axes in one step. The perpendicular axes theorem works only for flat (planar) bodies. When angular momentum is conserved (a skater pulling in her arms), rotational kinetic energy is usually not conserved. Rolling without slipping (v = ωR) is not named in the Main 2026 syllabus; see the flagged list below.

6. Gravitation

ResultFormula
Law of gravitationF = Gm1m2/r2
g at the surfaceg = GM/R2
g at height hgh = g R2/(R + h)2 ≈ g(1 − 2h/R) for h ≪ R
g at depth dgd = g(1 − d/R)
Potential and potential energyV = −GM/r; U = −GMm/r (r ≥ R)
Escape velocityve = √(2GM/R) = √(2gR)
Orbital velocity and periodvo = √(GM/r); T = 2π√(r3/GM), with r = R + h
Kepler's third lawT2 ∝ a3 (a = semi-major axis)
Satellite energiesK = GMm/(2r); U = −GMm/r; E = −GMm/(2r)

How to use / common traps: r in orbital formulas is measured from the centre of the Earth, not from the surface. The approximation g(1 − 2h/R) fails when h is comparable to R; use the exact form. Escape velocity does not depend on the direction of projection or the mass of the body. Near the surface, ve = √2 × vo.

7. Properties of solids and liquids

In the 2026 syllabus, this unit also contains heat, thermal expansion, calorimetry and heat transfer, so those formulas are listed here.

ResultFormula
Elastic moduliYoung's Y = (F/A)/(ΔL/L); bulk B = −ΔP/(ΔV/V); modulus of rigidity η = (F/A)/θ
Fluid pressureP = P0 + ρgh
Continuity and BernoulliA1v1 = A2v2; P + ½ρv2 + ρgh = constant along a streamline
Speed of efflux (Torricelli)v = √(2gh)
Stokes' law and terminal velocityF = 6πηrv; vt = 2r2(ρ − σ)g/(9η), ρ = sphere density, σ = fluid density
Reynolds number and critical velocityRe = ρvD/η; vc = Recη/(ρD)
Surface energyW = TΔA (a film has two surfaces, so ΔA doubles)
Excess pressureLiquid drop or air bubble in liquid: 2T/r; soap bubble in air: 4T/r
Capillary riseh = 2T cosθ/(ρgr)
Thermal expansionΔL = αLΔT; β ≈ 2α (area); γ ≈ 3α (volume)
Calorimetry and latent heatQ = mcΔT; Q = mL; heat lost = heat gained
ConductiondQ/dt = kAΔT/L; thermal resistance L/(kA), combined like electrical resistances

How to use / common traps: a soap bubble has two surfaces, so its excess pressure is 4T/r, while an air bubble inside water has one surface and 2T/r. In Stokes' law problems, the net driving force uses the difference in densities (ρ − σ), not ρ alone. In calorimetry with a change of state, first check whether enough heat is available to melt or boil everything; often the final state is a mixture at 0 °C or 100 °C.

From our tutors: for Units 2 to 7, we ask students to write the conditions next to each formula on their own copy of this sheet, such as "constant a only" beside the equations of motion or "one surface" beside 2T/r. In our experience, the formula is rarely the problem in mechanics. Applying it where it does not hold is.

8. Thermodynamics

ResultFormula
First lawΔQ = ΔU + ΔW (ΔW = work done by the gas)
Work by a gasW = ∫P dV = area under the P–V curve
Internal energy of an ideal gasΔU = nCvΔT for any process
IsobaricW = PΔV = nRΔT; Q = nCpΔT
IsochoricW = 0; Q = ΔU = nCvΔT
IsothermalΔU = 0; Q = W = nRT ln(V2/V1)
AdiabaticQ = 0; PVγ = constant; TVγ−1 = constant; W = (P1V1 − P2V2)/(γ − 1) = nR(T1 − T2)/(γ − 1)
Mayer's relationCp − Cv = R (molar)
P–V slopesAdiabatic slope = γ × isothermal slope at the same point
Efficiency of a heat engineη = W/QH = 1 − QC/QH

How to use / common traps: check which sign convention the question uses for work before applying the first law; this sheet uses NCERT's (work done by the gas is positive). In a cyclic process ΔU = 0, so net heat absorbed equals net work done (the area enclosed by the loop, positive if the loop runs clockwise on a P–V diagram). The Carnot efficiency 1 − TC/TH is not named in the Main 2026 syllabus; it is flagged below.

9. Kinetic theory of gases

ResultFormula
Ideal gas equationPV = nRT = NkBT
Pressure of a gasP = ⅓ρvrms2
Molecular speedsvrms = √(3RT/M); vavg = √(8RT/πM); vmp = √(2RT/M), so vrms > vavg > vmp
Kinetic interpretation of temperatureAverage translational KE per molecule = (3/2)kBT
Equipartition½kBT per degree of freedom per molecule; U = (f/2)nRT
Specific heats from fCv = (f/2)R; Cp = (f/2 + 1)R; γ = 1 + 2/f
Typical fMonatomic f = 3 (γ = 5/3); diatomic at ordinary temperature f = 5 (γ = 7/5)
Mean free pathλ = 1/(√2 πd2n) = kBT/(√2 πd2P)

How to use / common traps: M must be in kg/mol (32 × 10−3 for O2, not 32). For a mixture of gases, Cv is the mole-weighted average, and so is internal energy; γ of the mixture is Cp,mix/Cv,mix, not the average of the two γ values. Temperature must be in kelvin everywhere in this unit.

10. Oscillations and waves

ResultFormula
SHMx = A sin(ωt + φ); v = ω√(A2 − x2); a = −ω2x
PeriodsSpring–mass T = 2π√(m/k); simple pendulum T = 2π√(l/g) (small angles)
Energy in SHME = ½kA2 = ½mω2A2; K = ½k(A2 − x2); U = ½kx2
SpringsSeries 1/k = 1/k1 + 1/k2; parallel k = k1 + k2
Progressive wavey = A sin(kx − ωt); k = 2π/λ; v = ω/k = fλ
Wave speedString v = √(T/μ); sound in a gas v = √(γP/ρ)
String fixed at both ends; open pipefn = nv/(2L), n = 1, 2, 3 … (all harmonics)
Pipe closed at one endf = (2n − 1)v/(4L) (odd harmonics only)
Beatsfbeat = |f1 − f2|

How to use / common traps: kinetic energy in SHM oscillates at twice the frequency of the motion. A closed pipe of length 0.5 m with v = 340 m/s has fundamental v/(4L) = 170 Hz, and its next overtone is 510 Hz (the third harmonic), not 340 Hz. For beats questions, check whether loading a fork with wax (lower frequency) or filing it (higher frequency) raises or lowers the beat count before choosing f1 + fb or f1 − fb.

Knowing the formulas but still dropping marks in mechanics or waves? Book a free JEE Physics demo class in Gurgaon. The tutor will test where the gap is: concept, condition or calculation.

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11. Electrostatics

ResultFormula
Coulomb's lawF = kq1q2/r2; k = 1/(4πε0) ≈ 9 × 109 N m2 C−2
Point chargeE = kq/r2; V = kq/r; E = −∇V (E = −dV/dr)
Dipole (r ≫ a), p = q × 2aAxial E = 2kp/r3; equatorial E = kp/r3; V = kp cosθ/r2
Dipole in a uniform fieldτ = p × E; U = −p·E
Gauss's lawΦ = qenclosed/ε0
Gauss's law resultsInfinite line: λ/(2πε0r); infinite sheet: σ/(2ε0); thin shell: kQ/r2 outside, 0 inside
Potential energy of two chargesU = kq1q2/r
Parallel plate capacitorC = ε0A/d; filled with dielectric C = Kε0A/d; slab of thickness t: C = ε0A/(d − t + t/K)
CombinationsSeries 1/C = Σ1/Ci; parallel C = ΣCi
Energy storedU = ½CV2 = Q2/(2C) = ½QV; energy density ½ε0E2

How to use / common traps: the dipole field formulas are approximations for points far from the dipole. When a dielectric slab is inserted with the battery connected, V stays fixed and Q rises; with the battery disconnected, Q stays fixed and V falls. Decide which case you are in before using any energy formula. Potential is a scalar, so add values with signs; field is a vector, so add components.

12. Current electricity

ResultFormula
Drift velocity and currentI = neAvd; vd = eEτ/m; mobility μ = vd/E
Ohm's law and resistanceV = IR; R = ρl/A; conductivity σ = 1/ρ
Temperature dependenceRT = R0[1 + α(T − T0)]
CombinationsSeries R = ΣRi; parallel 1/R = Σ1/Ri
Cell with internal resistanceI = E/(R + r); terminal voltage V = E − Ir while supplying current
Cells in series and parallelSeries: Eeq = ΣEi, req = Σri. Parallel: Eeq = (ΣEi/ri)/(Σ1/ri), 1/req = Σ1/ri
PowerP = VI = I2R = V2/R
Kirchhoff's lawsJunction: ΣI = 0; loop: sum of potential changes = 0
Wheatstone bridge (balanced)P/Q = R/S
Metre bridgeR/X = l/(100 − l), with R in the left gap and balance at l cm from the left end

How to use / common traps: if a wire is stretched to n times its length at constant volume, its resistance becomes n2 times, because A falls by the same factor as l rises. In a balanced Wheatstone bridge, the middle (galvanometer) arm carries no current and can be removed. For parallel cells, reverse the sign of Ei for any cell connected the other way round.

13. Magnetic effects of current and magnetism

ResultFormula
Biot–Savart lawdB = (μ0/4π) I dl × r̂/r2
Circular loopCentre B = μ0I/(2R); on axis B = μ0IR2/[2(R2 + x2)3/2]
Ampere's law resultsLong straight wire B = μ0I/(2πr); long solenoid B = μ0nI (n = turns per unit length)
Lorentz forceF = q(E + v × B)
Charge in uniform B (v ⊥ B)r = mv/(qB); T = 2πm/(qB), independent of speed
Force on a wire; parallel wiresF = IL × B; force per unit length μ0I1I2/(2πd), attractive for currents in the same direction
Current loop as a dipolem = NIA; τ = m × B; U = −m·B
Moving coil galvanometerNIAB = kφ; current sensitivity φ/I = NAB/k; voltage sensitivity φ/V = NAB/(kG)
ConversionAmmeter: shunt S = IgG/(I − Ig) in parallel. Voltmeter: series R = V/Ig − G
Bar magnet (r ≫ size)Axial B = (μ0/4π)(2m/r3); equatorial B = (μ0/4π)(m/r3)
Temperature and magnetismCurie's law for paramagnets: χ ∝ 1/T; ferromagnets become paramagnetic above the Curie temperature

How to use / common traps: the magnetic force does no work, so it changes the direction of velocity but not the speed. If v has a component along B, the path is a helix, and only the perpendicular component goes into r = mv/(qB). For a finite wire, B = μ0I/(4πr)(sinθ1 + sinθ2); the "long wire" result is the special case θ1 = θ2 = 90°.

14. Electromagnetic induction and alternating currents

ResultFormula
Faraday and Lenzε = −N dΦ/dt, with Φ = B·A
Motional emfε = Blv (rod ⊥ B, v ⊥ rod)
Self-inductanceε = −L dI/dt; long solenoid L = μ0n2Al; energy U = ½LI2
Mutual inductanceε2 = −M dI1/dt
AC generatorε = NBAω sin ωt; peak ε0 = NBAω
RMS values (sinusoidal)Irms = I0/√2; Vrms = V0/√2
Reactance and impedanceXL = ωL; XC = 1/(ωC); Z = √[R2 + (XL − XC)2]; tanφ = (XL − XC)/R
Resonance (series LCR)ω0 = 1/√(LC); Z = R, current maximum
PowerP = VrmsIrms cosφ; power factor cosφ = R/Z
Wattless currentIrms sinφ
Ideal transformerVs/Vp = Ns/Np = Ip/Is

How to use / common traps: in a series LCR circuit, add voltages as phasors, not as numbers: V = √[VR2 + (VL − VC)2]. At resonance VL and VC can each be larger than the supply voltage. The I0/√2 rule applies only to sinusoidal waveforms.

15. Electromagnetic waves

ResultFormula or fact
Displacement currentId = ε0 dΦE/dt
Speed in vacuumc = 1/√(μ0ε0); E0/B0 = c
NatureTransverse: E, B and the direction of travel are mutually perpendicular, and the wave travels along E × B
Spectrum (increasing frequency)Radio → microwaves → infrared → visible → ultraviolet → X-rays → gamma rays
Average intensityI = ½cε0E02

How to use / common traps: electric and magnetic fields carry equal average energy in an EM wave, even though B0 is numerically much smaller than E0. Learn one use for each band in the spectrum, since the syllabus lists applications.

16. Optics

ResultFormula
Mirror1/v + 1/u = 1/f; f = R/2; m = −v/u
Snell's law; critical anglen1 sin i = n2 sin r; sin C = n2/n1 (light going from denser n1 to rarer n2)
Refraction at a spherical surfacen2/v − n1/u = (n2 − n1)/R
Thin lens1/v − 1/u = 1/f; m = v/u; power P = 1/f (f in metres, P in dioptres)
Lens maker's formula1/f = (n − 1)(1/R1 − 1/R2), n relative to the surrounding medium
Lenses in contact1/F = Σ1/fi; P = ΣPi
Prismn = sin[(A + δm)/2]/sin(A/2); thin prism δ = (n − 1)A
Microscope and telescopeSimple microscope m = 1 + D/f (image at D); compound microscope m ≈ (L/fo)(D/fe); telescope in normal adjustment m = fo/fe, length fo + fe
Young's double slitFringe width β = λD/d; bright: path difference nλ; dark: (2n − 1)λ/2
Resultant intensityI = I1 + I2 + 2√(I1I2) cosφ
Single slitMinima: a sinθ = nλ (n ≠ 0); angular width of central maximum 2λ/a; linear width 2λD/a
Brewster's lawtan iB = n; reflected and refracted rays are perpendicular

How to use / common traps: use one sign convention (the Cartesian convention in NCERT) for both mirrors and lenses, and put the sign of every given distance in before solving. A lens immersed in a liquid changes its focal length because (n − 1) becomes (nlens/nliquid − 1); it can even change from converging to diverging. In YDSE, placing the apparatus in water divides β by the refractive index.

17. Dual nature of matter and radiation

ResultFormula
Photon energy and momentumE = hν = hc/λ; p = h/λ; hc ≈ 1240 eV nm
Einstein's photoelectric equationKmax = hν − φ0 = eV0 (V0 = stopping potential)
Thresholdν0 = φ0/h; λ0 = hc/φ0
de Broglie wavelengthλ = h/p = h/√(2mK)
Electron accelerated through V voltsλ = h/√(2meV) ≈ 1.227/√V nm

How to use / common traps: intensity changes the number of photoelectrons (the saturation current), not their maximum kinetic energy; frequency changes Kmax. A 620 nm photon carries 1240/620 = 2.0 eV, so it cannot eject electrons from a metal with a work function above 2.0 eV, however bright the light. In a graph of V0 against ν, the slope is h/e for every metal.

18. Atoms and nuclei

ResultFormula
Bohr's quantisationmvr = nh/(2π)
Hydrogen-like atomrn ≈ 0.529 n2/Z Å; En ≈ −13.6 Z2/n2 eV; vn ≈ 2.18 × 106 Z/n m/s
Spectral lines1/λ = RZ2(1/n12 − 1/n22); R ≈ 1.097 × 107 m−1
Series (hydrogen)Lyman n1 = 1 (ultraviolet); Balmer n1 = 2 (visible); Paschen n1 = 3 (infrared)
Lines from level nMaximum number of lines = n(n − 1)/2
Distance of closest approach (alpha particle)r0 = k(2e)(Ze)/K
Nuclear sizeR = R0A1/3, R0 ≈ 1.2 fm; nuclear density is roughly the same for all nuclei
Mass–energyE = mc2; 1 u ≈ 931.5 MeV
Mass defect and binding energyΔm = [Zmp + (A − Z)mn] − Mnucleus; BE = Δm c2

How to use / common traps: kinetic energy in a Bohr orbit equals −En and potential energy equals 2En. Binding energy per nucleon, not total binding energy, decides stability; it peaks near iron, which is why fission of heavy nuclei and fusion of light nuclei both release energy. Radioactive decay (half-life, decay constant) is not named in the Main 2026 syllabus; see the flagged list.

19. Electronic devices

ResultFormula or fact
Diode biasForward bias: p to higher potential, current flows after the knee voltage. Reverse bias: tiny current until breakdown
Rectifier output frequencyHalf-wave: f (same as input); full-wave: 2f
Zener regulatorVload = VZ; Iseries = (Vin − VZ)/RS; IZ = Iseries − Iload
Optoelectronic devicesLED: forward bias, photon energy ≈ band gap (Eg ≈ hc/λ). Photodiode: reverse bias. Solar cell: no external bias
Logic gatesOR: Y = A + B; AND: Y = A·B; NOT: Y = Ā; NAND: Y = (A·B)‾ ; NOR: Y = (A + B)‾

How to use / common traps: in Zener questions, first check that the Zener is actually in breakdown: remove it, find the voltage across the load, and only if that exceeds VZ does the regulator formula apply. For combined gate circuits, write the truth table column by column rather than simplifying in your head. NAND and NOR are universal gates.

20. Experimental skills

The 2026 syllabus lists 18 experiments. These are the formulas behind them that questions most often need.

ExperimentFormula
Vernier callipersLC = 1 MSD − 1 VSD (= 1 MSD/N when N VSD = (N − 1) MSD); reading = MSR + (VSR × LC) − zero error
Screw gaugeLC = pitch/number of circular divisions; reading = MSR + (CSR × LC) − zero error
Simple pendulumg = 4π2l/T2; slope of an l–T2 graph = g/4π2
Metre scale (principle of moments)m1l1 = m2l2 about the pivot
Young's modulus of a wireY = MgL/(πr2Δl)
Resonance tubev = 2f(l2 − l1); end correction e = (l2 − 3l1)/2
Metre bridge resistivityρ = Xπd2/(4L)
Galvanometer, half-deflectionG = RS/(R − S) (≈ S when R ≫ S); figure of merit k = E/[(R + G)θ]
Prism i–δ graphAt minimum deviation i = e and the ray passes symmetrically
Glass slab (travelling microscope)n = real thickness/apparent thickness
Method of mixturesHeat lost by hot body = heat gained by cold body (include the calorimeter)

How to use / common traps: zero error is subtracted with its sign: a negative zero error is added back. Using the difference l2 − l1 in the resonance tube removes the end correction, which is why that method is preferred. In the Young's modulus experiment, the error in the radius counts twice, because r is squared.

From our tutors: students often skip Unit 20 because it feels like "practical" work. We teach it alongside the matching theory chapter instead: vernier and screw gauge with Unit 1, the resonance tube with waves, the metre bridge with current electricity. The formulas are short, and linking each experiment to its chapter makes them much easier to remember.

Formulas not listed in the JEE Main 2026 syllabus

These topics appear in many older formula sheets and books, but the JEE Main 2026 Physics syllabus does not name them. We have compared them with the JEE (Advanced) 2026 syllabus, which is printed in the JEE (Advanced) 2026 Information Brochure. If you are preparing only for JEE Main, give these lower priority; if you are also taking JEE Advanced, learn those it names.

Topic and key formulaJEE Main 2026 syllabusJEE Advanced 2026 syllabus
Doppler effect in sound: f′ = f(v ± vo)/(v ∓ vs)Not named (Unit 10 stops at beats)Named
Rolling without slipping: v = ωR; a = g sinθ/(1 + k2/R2) on an inclineNot named (only "rolling friction")Named
Carnot engine: η = 1 − TC/THNot named (second law and reversibility are)Named
Newton's law of cooling; Stefan's law (E = σT4); Wien's law (λmT = b)Not named (heat transfer by radiation is listed in general terms)Named
Radioactive decay: N = N0e−λt; T½ = ln 2/λNot namedNamed
X-rays and Moseley's lawNot named (X-rays appear only in the EM spectrum)Named
Damped and forced oscillationsNot namedNamed
RC and LR circuits with d.c. (growth and decay)Not namedNamed
PotentiometerNot named (metre bridge only)Not named
Transistors and communication systemsNot namedNot named

"Not named" means the topic is absent from the syllabus text. It does not guarantee that no question will ever touch the idea, and NTA can revise the syllabus. For how often each unit actually appears in papers, see our JEE Main physics chapter-wise weightage analysis.

Printing tips

  • Use your browser's Print option. The table of contents and booking boxes are hidden when you print, so the sheet prints as formulas and notes only.
  • Print on both sides and keep the pages with your error log. Add your own conditions and mistakes in the margins.
  • Replace the printout when NTA publishes the next syllabus.

Formulas are only half of the job; the other half is using them without slips in numerical questions. Our guide to common mistakes in JEE physics numericals covers units, signs and rounding.

Frequently asked questions

Is this JEE physics formula sheet enough for JEE Main?

It covers the key formulas in all 20 units of the JEE Main 2026 Physics syllabus, but formulas alone will not get the marks. JEE Main tests whether you can pick the right formula, check its conditions and calculate accurately, so pair the sheet with previous-year questions and timed practice.

Can I download this as a PDF?

We do not offer a separate download. The page is built to print: use your browser's Print option, and choose "Save as PDF" if you want a copy on your device.

Does JEE Main give a formula sheet in the exam?

The JEE Main 2026 Information Bulletin does not describe any formula sheet for candidates, and it lists calculators and log tables as prohibited items. Some questions state the constants to use, and NTA advises using the constants given. Always read the current bulletin for exam-day rules.

How many units are in the JEE Main 2026 physics syllabus?

Twenty, from Units and Measurements to Experimental Skills. This sheet follows the same order, with heat and thermal expansion placed under Unit 7 (Properties of Solids and Liquids), as in the official syllabus.

Is this a physics formula sheet for JEE with all chapters?

It covers every chapter in the 20 units of the JEE Main 2026 Physics syllabus. Topics that appear in older sheets but not in the 2026 Main syllabus, such as the Doppler effect and radioactive decay, are listed in a separate flagged table with their key formulas. Both are named in the JEE Advanced 2026 syllabus, so learn them if you are taking Advanced.

Which JEE physics formulas should I learn first?

Start with the units that the rest of physics depends on: kinematics, laws of motion, and work and energy. Electrostatics and current electricity underpin most Class 12 units. After that, prioritise the units where your mock-test accuracy is lowest.

How should I revise JEE physics formulas each day?

A short daily session of 10 to 15 minutes, covering two or three units in rotation, works better than one long session a week. Cover the formula column, write from memory, and then solve two or three questions that use the formulas you missed.

Can a home tutor help with physics formulas?

A tutor helps most by showing where each formula comes from and when it fails, which makes recall much easier. Ajay Vatsyayan Classes tutors teach JEE Physics one-to-one at home across Gurgaon (Gurugram) and online.

Want a tutor to turn this JEE physics formula sheet into marks? Book a free JEE Physics demo with Ajay Vatsyayan Classes, Saraswati kunj II, Wazirabad, Sector 52, Gurugram, Haryana 122003. Male and female tutors are available, at home or online.

Book a Free JEE Physics Demo +91 92204 75088

About this guide

Written by the Ajay Vatsyayan Classes Home Tutors Team, a Gurgaon home-tuition service with 12+ years of experience and 25,000+ students taught.

Reviewed by Ajay Vatsyayan (Founder; B.Tech; IB and Cambridge IGCSE experienced).

Exam facts are checked against official NTA, CBSE and CISCE documents. Always confirm dates and rules in the current official bulletin.