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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.
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.
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.
| Result | Formula or fact |
|---|---|
| SI base quantities | 7: length (m), mass (kg), time (s), current (A), temperature (K), amount of substance (mol), luminous intensity (cd) |
| Common dimensions | Force [MLT−2]; energy [ML2T−2]; power [ML2T−3]; pressure [ML−1T−2]; G [M−1L3T−2]; h [ML2T−1] |
| Error in a sum or difference | Z = A ± B → ΔZ = ΔA + ΔB |
| Error in a product or quotient | Z = AB or A/B → ΔZ/Z = ΔA/A + ΔB/B |
| Error in a power | Z = An → ΔZ/Z = |n| ΔA/A |
| Significant figures | Addition/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.
| Result | Formula |
|---|---|
| Constant acceleration | v = u + at; s = ut + ½at2; v2 = u2 + 2as |
| Distance in the nth second | sn = u + (a/2)(2n − 1) |
| Graphs | Slope of x–t = velocity; slope of v–t = acceleration; area under v–t = displacement |
| Relative velocity | vAB = vA − vB |
| Projectile (ground to ground) | T = 2u sinθ/g; H = u2sin2θ/(2g); R = u2sin 2θ/g; Rmax = u2/g at θ = 45° |
| Trajectory | y = x tanθ − gx2/(2u2cos2θ) |
| Uniform circular motion | v = 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.
| Result | Formula |
|---|---|
| Second law | F = dp/dt; F = ma for constant mass |
| Impulse | J = ∫F dt = Δp |
| Conservation of momentum | If net external force = 0, total p is constant |
| Friction | Static: fs ≤ μsN; kinetic: fk = μkN |
| Equilibrium of concurrent forces | ΣF = 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 road | vmax = √(μrg) |
| Banked road | No 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.
| Result | Formula |
|---|---|
| Work | W = F·s = Fs cosθ (constant force); W = ∫F dx (variable force) |
| Work–energy theorem | Wnet = ΔK |
| Kinetic energy and momentum | K = ½mv2 = p2/(2m) |
| Spring potential energy | U = ½kx2 |
| Conservative force and potential energy | F = −dU/dx |
| Power | P = 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 collision | v1 = [(m1 − m2)u1 + 2m2u2]/(m1 + m2); v2 = [(m2 − m1)u2 + 2m1u1]/(m1 + m2) |
| Coefficient of restitution | e = (v2 − v1)/(u1 − u2); e = 1 elastic, e = 0 perfectly inelastic |
| KE lost, perfectly inelastic | ΔK = 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).
| Result | Formula |
|---|---|
| Centre of mass | xcm = Σmixi/Σmi; for a rigid body xcm = ∫x dm/M |
| Torque and angular momentum | τ = r × F; L = r × p; τ = dL/dt |
| Rigid body about a fixed axis | L = Iω; τ = Iα; K = ½Iω2; W = τθ; P = τω |
| Conservation of angular momentum | If net external torque = 0: I1ω1 = I2ω2 |
| Radius of gyration | I = Mk2 |
| Parallel axes theorem | I = Icm + Md2 |
| Perpendicular axes theorem (plane lamina only) | Iz = Ix + Iy |
| Standard moments of inertia | Ring (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 analogy | m ↔ 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.
| Result | Formula |
|---|---|
| Law of gravitation | F = Gm1m2/r2 |
| g at the surface | g = GM/R2 |
| g at height h | gh = g R2/(R + h)2 ≈ g(1 − 2h/R) for h ≪ R |
| g at depth d | gd = g(1 − d/R) |
| Potential and potential energy | V = −GM/r; U = −GMm/r (r ≥ R) |
| Escape velocity | ve = √(2GM/R) = √(2gR) |
| Orbital velocity and period | vo = √(GM/r); T = 2π√(r3/GM), with r = R + h |
| Kepler's third law | T2 ∝ a3 (a = semi-major axis) |
| Satellite energies | K = 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.
In the 2026 syllabus, this unit also contains heat, thermal expansion, calorimetry and heat transfer, so those formulas are listed here.
| Result | Formula |
|---|---|
| Elastic moduli | Young's Y = (F/A)/(ΔL/L); bulk B = −ΔP/(ΔV/V); modulus of rigidity η = (F/A)/θ |
| Fluid pressure | P = P0 + ρgh |
| Continuity and Bernoulli | A1v1 = A2v2; P + ½ρv2 + ρgh = constant along a streamline |
| Speed of efflux (Torricelli) | v = √(2gh) |
| Stokes' law and terminal velocity | F = 6πηrv; vt = 2r2(ρ − σ)g/(9η), ρ = sphere density, σ = fluid density |
| Reynolds number and critical velocity | Re = ρvD/η; vc = Recη/(ρD) |
| Surface energy | W = TΔA (a film has two surfaces, so ΔA doubles) |
| Excess pressure | Liquid drop or air bubble in liquid: 2T/r; soap bubble in air: 4T/r |
| Capillary rise | h = 2T cosθ/(ρgr) |
| Thermal expansion | ΔL = αLΔT; β ≈ 2α (area); γ ≈ 3α (volume) |
| Calorimetry and latent heat | Q = mcΔT; Q = mL; heat lost = heat gained |
| Conduction | dQ/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.
| Result | Formula |
|---|---|
| First law | ΔQ = ΔU + ΔW (ΔW = work done by the gas) |
| Work by a gas | W = ∫P dV = area under the P–V curve |
| Internal energy of an ideal gas | ΔU = nCvΔT for any process |
| Isobaric | W = PΔV = nRΔT; Q = nCpΔT |
| Isochoric | W = 0; Q = ΔU = nCvΔT |
| Isothermal | ΔU = 0; Q = W = nRT ln(V2/V1) |
| Adiabatic | Q = 0; PVγ = constant; TVγ−1 = constant; W = (P1V1 − P2V2)/(γ − 1) = nR(T1 − T2)/(γ − 1) |
| Mayer's relation | Cp − Cv = R (molar) |
| P–V slopes | Adiabatic slope = γ × isothermal slope at the same point |
| Efficiency of a heat engine | η = 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.
| Result | Formula |
|---|---|
| Ideal gas equation | PV = nRT = NkBT |
| Pressure of a gas | P = ⅓ρvrms2 |
| Molecular speeds | vrms = √(3RT/M); vavg = √(8RT/πM); vmp = √(2RT/M), so vrms > vavg > vmp |
| Kinetic interpretation of temperature | Average translational KE per molecule = (3/2)kBT |
| Equipartition | ½kBT per degree of freedom per molecule; U = (f/2)nRT |
| Specific heats from f | Cv = (f/2)R; Cp = (f/2 + 1)R; γ = 1 + 2/f |
| Typical f | Monatomic f = 3 (γ = 5/3); diatomic at ordinary temperature f = 5 (γ = 7/5) |
| Mean free path | λ = 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.
| Result | Formula |
|---|---|
| SHM | x = A sin(ωt + φ); v = ω√(A2 − x2); a = −ω2x |
| Periods | Spring–mass T = 2π√(m/k); simple pendulum T = 2π√(l/g) (small angles) |
| Energy in SHM | E = ½kA2 = ½mω2A2; K = ½k(A2 − x2); U = ½kx2 |
| Springs | Series 1/k = 1/k1 + 1/k2; parallel k = k1 + k2 |
| Progressive wave | y = A sin(kx − ωt); k = 2π/λ; v = ω/k = fλ |
| Wave speed | String v = √(T/μ); sound in a gas v = √(γP/ρ) |
| String fixed at both ends; open pipe | fn = nv/(2L), n = 1, 2, 3 … (all harmonics) |
| Pipe closed at one end | f = (2n − 1)v/(4L) (odd harmonics only) |
| Beats | fbeat = |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.
Book a Free JEE Physics Demo +91 92204 75088| Result | Formula |
|---|---|
| Coulomb's law | F = kq1q2/r2; k = 1/(4πε0) ≈ 9 × 109 N m2 C−2 |
| Point charge | E = kq/r2; V = kq/r; E = −∇V (E = −dV/dr) |
| Dipole (r ≫ a), p = q × 2a | Axial E = 2kp/r3; equatorial E = kp/r3; V = kp cosθ/r2 |
| Dipole in a uniform field | τ = p × E; U = −p·E |
| Gauss's law | Φ = qenclosed/ε0 |
| Gauss's law results | Infinite line: λ/(2πε0r); infinite sheet: σ/(2ε0); thin shell: kQ/r2 outside, 0 inside |
| Potential energy of two charges | U = kq1q2/r |
| Parallel plate capacitor | C = ε0A/d; filled with dielectric C = Kε0A/d; slab of thickness t: C = ε0A/(d − t + t/K) |
| Combinations | Series 1/C = Σ1/Ci; parallel C = ΣCi |
| Energy stored | U = 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.
| Result | Formula |
|---|---|
| Drift velocity and current | I = neAvd; vd = eEτ/m; mobility μ = vd/E |
| Ohm's law and resistance | V = IR; R = ρl/A; conductivity σ = 1/ρ |
| Temperature dependence | RT = R0[1 + α(T − T0)] |
| Combinations | Series R = ΣRi; parallel 1/R = Σ1/Ri |
| Cell with internal resistance | I = E/(R + r); terminal voltage V = E − Ir while supplying current |
| Cells in series and parallel | Series: Eeq = ΣEi, req = Σri. Parallel: Eeq = (ΣEi/ri)/(Σ1/ri), 1/req = Σ1/ri |
| Power | P = VI = I2R = V2/R |
| Kirchhoff's laws | Junction: ΣI = 0; loop: sum of potential changes = 0 |
| Wheatstone bridge (balanced) | P/Q = R/S |
| Metre bridge | R/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.
| Result | Formula |
|---|---|
| Biot–Savart law | dB = (μ0/4π) I dl × r̂/r2 |
| Circular loop | Centre B = μ0I/(2R); on axis B = μ0IR2/[2(R2 + x2)3/2] |
| Ampere's law results | Long straight wire B = μ0I/(2πr); long solenoid B = μ0nI (n = turns per unit length) |
| Lorentz force | F = q(E + v × B) |
| Charge in uniform B (v ⊥ B) | r = mv/(qB); T = 2πm/(qB), independent of speed |
| Force on a wire; parallel wires | F = IL × B; force per unit length μ0I1I2/(2πd), attractive for currents in the same direction |
| Current loop as a dipole | m = NIA; τ = m × B; U = −m·B |
| Moving coil galvanometer | NIAB = kφ; current sensitivity φ/I = NAB/k; voltage sensitivity φ/V = NAB/(kG) |
| Conversion | Ammeter: 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 magnetism | Curie'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°.
| Result | Formula |
|---|---|
| Faraday and Lenz | ε = −N dΦ/dt, with Φ = B·A |
| Motional emf | ε = Blv (rod ⊥ B, v ⊥ rod) |
| Self-inductance | ε = −L dI/dt; long solenoid L = μ0n2Al; energy U = ½LI2 |
| Mutual inductance | ε2 = −M dI1/dt |
| AC generator | ε = NBAω sin ωt; peak ε0 = NBAω |
| RMS values (sinusoidal) | Irms = I0/√2; Vrms = V0/√2 |
| Reactance and impedance | XL = ωL; XC = 1/(ωC); Z = √[R2 + (XL − XC)2]; tanφ = (XL − XC)/R |
| Resonance (series LCR) | ω0 = 1/√(LC); Z = R, current maximum |
| Power | P = VrmsIrms cosφ; power factor cosφ = R/Z |
| Wattless current | Irms sinφ |
| Ideal transformer | Vs/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.
| Result | Formula or fact |
|---|---|
| Displacement current | Id = ε0 dΦE/dt |
| Speed in vacuum | c = 1/√(μ0ε0); E0/B0 = c |
| Nature | Transverse: 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 intensity | I = 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.
| Result | Formula |
|---|---|
| Mirror | 1/v + 1/u = 1/f; f = R/2; m = −v/u |
| Snell's law; critical angle | n1 sin i = n2 sin r; sin C = n2/n1 (light going from denser n1 to rarer n2) |
| Refraction at a spherical surface | n2/v − n1/u = (n2 − n1)/R |
| Thin lens | 1/v − 1/u = 1/f; m = v/u; power P = 1/f (f in metres, P in dioptres) |
| Lens maker's formula | 1/f = (n − 1)(1/R1 − 1/R2), n relative to the surrounding medium |
| Lenses in contact | 1/F = Σ1/fi; P = ΣPi |
| Prism | n = sin[(A + δm)/2]/sin(A/2); thin prism δ = (n − 1)A |
| Microscope and telescope | Simple 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 slit | Fringe width β = λD/d; bright: path difference nλ; dark: (2n − 1)λ/2 |
| Resultant intensity | I = I1 + I2 + 2√(I1I2) cosφ |
| Single slit | Minima: a sinθ = nλ (n ≠ 0); angular width of central maximum 2λ/a; linear width 2λD/a |
| Brewster's law | tan 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.
| Result | Formula |
|---|---|
| Photon energy and momentum | E = hν = hc/λ; p = h/λ; hc ≈ 1240 eV nm |
| Einstein's photoelectric equation | Kmax = hν − φ0 = eV0 (V0 = stopping potential) |
| Threshold | ν0 = φ0/h; λ0 = hc/φ0 |
| de Broglie wavelength | λ = h/p = h/√(2mK) |
| Electron accelerated through V volts | λ = 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.
| Result | Formula |
|---|---|
| Bohr's quantisation | mvr = nh/(2π) |
| Hydrogen-like atom | rn ≈ 0.529 n2/Z Å; En ≈ −13.6 Z2/n2 eV; vn ≈ 2.18 × 106 Z/n m/s |
| Spectral lines | 1/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 n | Maximum number of lines = n(n − 1)/2 |
| Distance of closest approach (alpha particle) | r0 = k(2e)(Ze)/K |
| Nuclear size | R = R0A1/3, R0 ≈ 1.2 fm; nuclear density is roughly the same for all nuclei |
| Mass–energy | E = mc2; 1 u ≈ 931.5 MeV |
| Mass defect and binding energy | Δm = [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.
| Result | Formula or fact |
|---|---|
| Diode bias | Forward bias: p to higher potential, current flows after the knee voltage. Reverse bias: tiny current until breakdown |
| Rectifier output frequency | Half-wave: f (same as input); full-wave: 2f |
| Zener regulator | Vload = VZ; Iseries = (Vin − VZ)/RS; IZ = Iseries − Iload |
| Optoelectronic devices | LED: forward bias, photon energy ≈ band gap (Eg ≈ hc/λ). Photodiode: reverse bias. Solar cell: no external bias |
| Logic gates | OR: 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.
The 2026 syllabus lists 18 experiments. These are the formulas behind them that questions most often need.
| Experiment | Formula |
|---|---|
| Vernier callipers | LC = 1 MSD − 1 VSD (= 1 MSD/N when N VSD = (N − 1) MSD); reading = MSR + (VSR × LC) − zero error |
| Screw gauge | LC = pitch/number of circular divisions; reading = MSR + (CSR × LC) − zero error |
| Simple pendulum | g = 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 wire | Y = MgL/(πr2Δl) |
| Resonance tube | v = 2f(l2 − l1); end correction e = (l2 − 3l1)/2 |
| Metre bridge resistivity | ρ = Xπd2/(4L) |
| Galvanometer, half-deflection | G = RS/(R − S) (≈ S when R ≫ S); figure of merit k = E/[(R + G)θ] |
| Prism i–δ graph | At minimum deviation i = e and the ray passes symmetrically |
| Glass slab (travelling microscope) | n = real thickness/apparent thickness |
| Method of mixtures | Heat 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.
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 formula | JEE Main 2026 syllabus | JEE 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 incline | Not named (only "rolling friction") | Named |
| Carnot engine: η = 1 − TC/TH | Not 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/λ | Not named | Named |
| X-rays and Moseley's law | Not named (X-rays appear only in the EM spectrum) | Named |
| Damped and forced oscillations | Not named | Named |
| RC and LR circuits with d.c. (growth and decay) | Not named | Named |
| Potentiometer | Not named (metre bridge only) | Not named |
| Transistors and communication systems | Not named | Not 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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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