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This NEET physics formula sheet lists the key formulas for all 20 units of the official NEET (UG) 2026 Physics syllabus, in the same order as the syllabus notified by the National Medical Commission (NMC). Each unit has a compact table and a short "how to use / common traps" note, because NEET physics marks are usually lost by using a formula outside its conditions, not by forgetting it. A final table flags formulas that older books still carry but the current syllabus does not name.
A formula sheet is a revision tool, not a first lesson. If whole units still feel unfamiliar, a NEET Physics tutor in Gurgaon can rebuild the concepts first, and this page then becomes your daily recall sheet. It is built to print cleanly from your browser.
Use the sheet for short daily recall, not as reading material. The unit list and order follow the Syllabus for NEET (UG) 2026, notified by NMC and published by NTA, which has 20 physics units, from Physics and Measurement to Experimental Skills. We compared it word for word with the NEET (UG) 2025 syllabus and found the same physics units and topics. No NEET (UG) 2027 syllabus had been published when we checked on 29 September 2026, so treat 2026 as the reference until NMC notifies the next one.
Units 1 to 10 are mostly Class 11 physics and Units 11 to 20 mostly Class 12. For how the paper itself is built (45 physics questions, marking and timing), see our guide to the NEET physics syllabus and exam pattern.
| 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 = ApBq/Cr → ΔZ/Z = pΔA/A + qΔB/B + rΔC/C |
| Least count | Smallest reading an instrument can measure; the maximum error of a single reading is usually taken as one least count |
| 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. 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 it cannot check an equation that adds terms of different forms. Trailing zeros after a decimal point are significant (2.50 has three significant figures); leading zeros are not (0.0025 has two).
| Result | Formula |
|---|---|
| Uniformly accelerated motion | 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 |
| Vectors | A·B = AB cosθ; |A × B| = AB sinθ; resultant R = √(A2 + B2 + 2AB cosθ) |
| Relative velocity | vAB = vA − vB |
| Projectile (level 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. Fix one sign convention (for example, up positive) before substituting, especially for a body thrown upwards from a tower. 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 but different heights and times.
| Result | Formula |
|---|---|
| Second law | F = dp/dt; F = ma for constant mass |
| Impulse | J = ∫F dt = Δp (area under the F–t graph) |
| Conservation of momentum | If net external force = 0, total p is constant (gun recoil: mbvb = MgVg) |
| Friction | Static: fs ≤ μsN; kinetic: fk = μkN; usually μr < μk < μs |
| Angle of repose | tan θ = μs |
| Equilibrium of concurrent forces | ΣF = 0; three forces: Lami's theorem F1/sin α = F2/sin β = F3/sin γ (each angle opposite its force) |
| Two masses over a light pulley (Atwood) | a = (m1 − m2)g/(m1 + m2); T = 2m1m2g/(m1 + m2) |
| Vehicle on a level circular 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) prevents slipping, so find the friction needed first and compare it with the limit. Draw a separate free-body diagram for each body before writing equations. "Centripetal force" is not an extra force on the diagram; it is the net inward force supplied by tension, friction, gravity or a normal reaction. In a lift accelerating upwards at a, the apparent weight is m(g + a).
| Result | Formula |
|---|---|
| Work | W = F·s = Fs cosθ (constant force); W = ∫F dx (variable force, area under F–x graph) |
| Work–energy theorem | Wnet = ΔK |
| Kinetic energy and momentum | K = ½mv2 = p2/(2m) |
| Spring potential energy | U = ½kx2 |
| Conservative force | F = −dU/dx; work is path-independent and zero round a closed path |
| Power | P = dW/dt = F·v |
| Vertical circle (string) | Minimum speed at top √(gr); minimum speed at bottom √(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 friction and drag do no work; otherwise use Wnet = ΔK, which also gives the stopping distance on a rough floor, s = v2/(2μg). In an elastic head-on collision between equal masses, the bodies simply exchange velocities.
| Result | Formula |
|---|---|
| Centre of mass | Two particles: xcm = (m1x1 + m2x2)/(m1 + m2); 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 |
| Equations of rotational motion (constant α) | ω = ω0 + αt; θ = ω0t + ½αt2; ω2 = ω02 + 2αθ |
| Conservation of angular momentum | If net external torque = 0: I1ω1 = I2ω2 |
| Radius of gyration | I = Mk2 |
| Parallel and perpendicular axes | I = Icm + Md2; 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 |
| Equilibrium of a rigid body | ΣF = 0 and Στ = 0 about any point |
How to use / common traps: the parallel axes theorem must start from the axis through the centre of mass. The perpendicular axes theorem works only for flat bodies. When angular momentum is conserved (a skater pulling in her arms), rotational kinetic energy usually is not: ω rises, and K = L2/(2I) rises with it. Rolling without slipping (v = ωR) is not named in the NEET (UG) 2026 syllabus; see the flagged list.
| Result | Formula |
|---|---|
| Universal law | F = Gm1m2/r2; G ≈ 6.67 × 10−11 N m2 kg−2 |
| g at the surface | g = GM/R2 = (4/3)πGρR |
| g at height h | gh = gR2/(R + h)2 ≈ g(1 − 2h/R) for h ≪ R |
| g at depth d | gd = g(1 − d/R); zero at the centre |
| Potential and potential energy | V = −GM/r; U = −GMm/r (r ≥ R) |
| Escape velocity | ve = √(2GM/R) = √(2gR) ≈ 11.2 km/s for the Earth |
| Orbital velocity and period | vo = √(GM/r); T = 2π√(r3/GM), with r = R + h |
| Kepler's laws | Elliptical orbits; equal areas in equal times (areal velocity L/2m constant); T2 ∝ a3 |
| 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 planet, not from the surface. The approximation g(1 − 2h/R) fails when h is comparable to R: at h = R/2 the exact value is 4g/9, while the approximation gives zero. Escape velocity does not depend on the mass of the body or the direction of projection. For planets of the same density, g and ve are both proportional to R, a common ratio question.
In the NEET (UG) 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), so ΔL = FL/(AY); bulk B = −ΔP/(ΔV/V); modulus of rigidity η = (F/A)/θ |
| Elastic potential energy | Energy per unit volume = ½ × stress × strain |
| Fluid pressure; Pascal's law | P = P0 + ρgh; hydraulic lift F1/A1 = F2/A2 |
| 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 (12 Pa for r = 1 cm and T = 0.03 N/m), while an air bubble inside water has one surface and 2T/r. Terminal velocity uses the density difference (ρ − σ), and it varies as r2, so doubling the radius makes it four times larger. In calorimetry with a change of state, check first whether enough heat is available: 10 g of water cooling from 30 °C to 0 °C gives out 300 cal, which melts only part of 10 g of ice (800 cal needed), so the final state is ice and water at 0 °C.
From our tutors: for Units 2 to 7 we ask students to write the condition next to each formula on their printed copy: "constant a only" beside the equations of motion, "one surface" beside 2T/r, "h ≪ R" beside g(1 − 2h/R). In our experience, NEET aspirants who are strong in biology rarely forget a mechanics formula. They lose the mark by using it in a situation where it does not hold.
| 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 = nR(T1 − T2)/(γ − 1) |
| Mayer's relation | Cp − Cv = R (molar) |
| P–V slopes | Adiabatic slope = γ × isothermal slope at the same point |
| Cyclic process | ΔU = 0; net Q = net W = area enclosed by the loop |
How to use / common traps: check the sign convention for work before applying the first law; this sheet uses work done by the gas as positive, as in NCERT. The syllabus names the second law and reversible and irreversible processes, but not heat engines or the Carnot cycle, so those are flagged below. Temperatures in every gas formula are in kelvin.
| Result | Formula |
|---|---|
| Ideal gas equation | PV = nRT = NkBT; NA ≈ 6.02 × 1023 mol−1 |
| Pressure of a gas | P = ⅓ρvrms2 |
| Molecular speeds | vrms = √(3RT/M); vavg = √(8RT/πM); vmp = √(2RT/M); 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 (0.032 for O2, not 32). Since vrms ∝ √T, doubling the rms speed needs four times the kelvin temperature: from 27 °C (300 K) to 1200 K, which is 927 °C, not 108 °C. For a gas mixture, γ is Cp,mix/Cv,mix with mole-weighted C values, not the average of the two γ values.
| Result | Formula |
|---|---|
| SHM | x = A sin(ωt + φ); v = ω√(A2 − x2); a = −ω2x; vmax = ωA; amax = ω2A |
| Periods | Spring–mass T = 2π√(m/k); simple pendulum T = 2π√(l/g) (small angles) |
| Energy in SHM | E = ½kA2; 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 and potential energy in SHM oscillate at twice the frequency of the motion. The pendulum period does not depend on mass; in a lift accelerating upwards replace g by (g + a). A closed pipe 0.5 m long with v = 340 m/s has fundamental 170 Hz, and its next overtone is 510 Hz (the third harmonic), not 340 Hz. Wax on a fork lowers its frequency; filing raises it. Decide which way the beat count moves before choosing f ± fbeat.
Knowing the formulas but still dropping marks in mechanics, heat or waves? Book a free NEET Physics demo class in Gurgaon. The tutor will test where the gap is: concept, condition or calculation.
Book a Free NEET Physics Demo +91 92204 75088| Result | Formula |
|---|---|
| Coulomb's law | F = kq1q2/r2; in a medium, F is divided by the dielectric constant K |
| Point charge | E = kq/r2; V = kq/r; 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; net force zero |
| 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 (same Q); parallel C = ΣCi (same V) |
| Energy stored | U = ½CV2 = Q2/(2C) = ½QV; energy density ½ε0E2 |
How to use / common traps: the dipole 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. Inside a charged conductor the field is zero but the potential is not.
| 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 |
| Electrical power and energy | P = VI = I2R = V2/R; energy = Pt (1 kWh = 3.6 × 106 J) |
| 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: a wire stretched to n times its length at constant volume has n2 times the resistance, because the area falls by the same factor as the length rises. In a balanced Wheatstone bridge the galvanometer arm carries no current and can be removed. Maximum power is delivered to an external resistor when R = r. Check which gap holds the known resistor before using the metre bridge ratio: with R = 2 Ω in the left gap and balance at 40 cm, X = 3 Ω.
| Result | Formula |
|---|---|
| Biot–Savart law | dB = (μ0/4π) I dl × r̂/r2; μ0 = 4π × 10−7 T m A−1 |
| Circular loop | Centre B = μ0I/(2R) (N turns: μ0NI/(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) = √(2mK)/(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 magnetic 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) |
| Magnetic materials | Diamagnetic χ small and negative; paramagnetic χ small and positive, χ ∝ 1/T (Curie's law); ferromagnetic χ large, becomes 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). A proton and an alpha particle with the same kinetic energy move on circles of the same radius in the same field, because √m/q is the same for both; with the same speed, the alpha particle's radius is twice as large.
| Result | Formula |
|---|---|
| Faraday and Lenz | ε = −N dΦ/dt, with Φ = B·A = BA cosθ |
| Motional emf | ε = Blv (rod ⊥ B, v ⊥ rod); rod rotating about one end: ε = ½Bωl2 |
| 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 in AC | 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, and AC meters read rms values. A step-down transformer lowers voltage but raises current; an ideal one does not change power.
| Result | Formula or fact |
|---|---|
| Displacement current | Id = ε0 dΦE/dt |
| Speed in vacuum | c = 1/√(μ0ε0) ≈ 3 × 108 m/s; E0/B0 = c |
| Nature | Transverse: E, B and the direction of travel are mutually perpendicular; 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: the electric and magnetic fields carry equal average energy, even though B0 is numerically far smaller than E0. The syllabus names applications of each band, so learn one use for each: for example, microwaves in radar and ovens, infrared in remote controls, ultraviolet in sterilisation, X-rays in medical imaging.
| 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 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 | A = r1 + r2; 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 |
| Polarisation | Brewster: tan iB = n (reflected and refracted rays perpendicular); Malus: I = I0cos2θ |
How to use / common traps: use one sign convention (the Cartesian convention in NCERT) for mirrors and lenses, and put the sign of every given distance in before solving. A convex lens with f = 20 cm and an object at 30 cm gives v = +60 cm and m = −2 (real, inverted); move the object to 10 cm and v = −20 cm, m = +2 (virtual, erect). A lens in a liquid has (nlens/nliquid − 1) in place of (n − 1). In YDSE, immersing the set-up in water divides β by the refractive index. Our guide to modern physics and optics for NEET works through these units in more depth.
| Result | Formula |
|---|---|
| Photon energy and momentum | E = hν = hc/λ; p = h/λ; hc ≈ 1240 eV nm; h ≈ 6.63 × 10−34 J s |
| 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 and the intercept gives the threshold frequency. For the same kinetic energy, the lighter particle has the longer de Broglie wavelength.
| 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: in a Bohr orbit, kinetic energy equals −En and potential energy equals 2En; for hydrogen in the ground state that is +13.6 eV and −27.2 eV. From n = 4, up to 4 × 3/2 = 6 lines can appear. 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 and half-life are not named in the NEET (UG) 2026 syllabus; see the flagged list.
| Result | Formula or fact |
|---|---|
| Semiconductors | Intrinsic: ne = nh = ni; doped: nenh = ni2; n-type (pentavalent dopant), p-type (trivalent dopant) |
| Diode bias | Forward bias: p side at higher potential, current rises sharply 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 in breakdown: remove it and find the voltage across the load. With Vin = 15 V, RS = 500 Ω, RL = 2 kΩ and VZ = 10 V, the load alone would get 12 V, so the Zener conducts; then Iseries = 10 mA, Iload = 5 mA and IZ = 5 mA. This unit is worth extra care for board students: the CBSE 2026–27 Class 12 physics syllabus covers the diode as a rectifier but does not name Zener diodes, LEDs, photodiodes, solar cells or logic gates in its theory, while the NEET syllabus names all of them.
The NEET (UG) 2026 syllabus lists 18 experiments and asks for "familiarity with the basic approach and observations". These are the formulas behind them that questions most often need.
| Experiment | Formula or key idea |
|---|---|
| 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 scale divisions; reading = MSR + (CSR × LC) − zero error |
| Simple pendulum, dissipation of energy | Energy ∝ (amplitude)2, so a graph of A2 against time shows how energy is lost |
| Metre scale (principle of moments) | m1l1 = m2l2 about the pivot |
| Young's modulus of a wire | Y = MgL/(πr2Δl) |
| Surface tension by capillary rise | T = rhρg/(2 cosθ); detergent lowers T, so h falls |
| Viscosity by terminal velocity | η = 2r2(ρ − σ)g/(9vt) |
| Resonance tube | v = 2f(l2 − l1); end correction e = (l2 − 3l1)/2 |
| Specific heat by method of mixtures | Heat lost by hot body = heat gained by water and calorimeter |
| Metre bridge resistivity; Ohm's law | ρ = Xπd2/(4L); R = slope of the V–I graph |
| Galvanometer, half-deflection | G = RS/(R − S) (≈ S when R ≫ S); figure of merit k = E/[(R + G)θ] |
| Focal length (mirrors, convex lens) | Parallax method: no parallax between image and pin at the image position; use 1/v ± 1/u = 1/f with signs |
| Prism i–δ graph | At minimum deviation i = e and the ray passes symmetrically |
| Glass slab (travelling microscope) | n = real thickness/apparent thickness |
| Diode and Zener characteristics | Forward knee voltage; reverse current nearly zero until breakdown; Zener breakdown voltage read from the reverse curve |
How to use / common traps: zero error is subtracted with its sign, so a negative zero error is added back. Using l2 − l1 in the resonance tube removes the end correction: with f = 500 Hz, l1 = 16 cm and l2 = 50 cm, v = 340 m/s and e = 1 cm. 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 school practical work. We teach each experiment with its theory chapter instead: vernier and screw gauge with Unit 1, the capillary tube and falling-ball viscometer with Unit 7, the resonance tube with waves, and the metre bridge with current electricity. The formulas are short, and linking them to a chapter makes them far easier to recall under exam pressure.
These topics still appear in many older NEET books and formula sheets, but the NEET (UG) 2026 Physics syllabus text does not name them. We checked each one against the syllabus text and against the CBSE 2026–27 Physics syllabus, since most NEET aspirants also sit board exams. Give them the lowest priority for NEET, but learn any that your board syllabus names.
| Topic and key formula | NEET (UG) 2026 syllabus | CBSE 2026–27 syllabus |
|---|---|---|
| Doppler effect in sound: f′ = f(v ± vo)/(v ∓ vs) | Not named (Unit 10 ends at beats) | Not named |
| Rolling without slipping: v = ωR; a = g sinθ/(1 + k2/R2) | Not named (only "rolling friction") | Not named in theory |
| Heat engines and Carnot cycle: η = 1 − TC/TH | Not named (second law, reversible and irreversible processes are) | Not named |
| Stefan's law (E = σT4); Wien's law (λmT = b) | Not named (radiation is listed only as a mode of heat transfer) | Named (qualitative ideas of black-body radiation) |
| Newton's law of cooling | Not named | Not named |
| Radioactive decay: N = N0e−λt; T½ = ln 2/λ | Not named | Not named |
| Damped and forced oscillations | Not named | Not named |
| Growth and decay in RC and LR circuits | Not named | Not named |
| Potentiometer | Not named (metre bridge only) | Listed only among practical apparatus to identify |
| 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 NMC can revise the syllabus, so check the notified version each year. For how the paper is set, including the number of physics questions and the marking scheme, read our NEET physics syllabus and exam pattern guide.
Formulas are only half the job; the other half is using them without slips when there is no calculator. Our step-by-step method for NEET physics numericals shows how, with worked examples from across the syllabus.
It covers the key formulas in all 20 units of the NEET (UG) 2026 Physics syllabus, but formulas alone do not earn marks. NEET tests whether you can choose the right formula, check its conditions and calculate quickly without a calculator, so pair this sheet with NCERT, previous-year questions and timed practice.
We do not offer a separate download. The page is designed to print: use your browser's Print option and choose "Save as PDF" if you want a copy on your device.
The NEET (UG) 2026 Information Bulletin does not describe any formula sheet for candidates, and it lists calculators, slide rules and log tables among items not allowed in the examination hall. Some questions state the constants to use. Always read the current bulletin for exam-day rules.
Twenty, from Physics and Measurement to Experimental Skills. This sheet follows the same order, with heat, calorimetry and heat transfer placed under Unit 7 (Properties of Solids and Liquids), as in the official syllabus.
Start with the units that the rest of physics depends on: kinematics, laws of motion, and work and energy, followed by electrostatics and current electricity for Class 12. After that, give priority to the units where your mock-test accuracy is lowest, rather than the ones you already find comfortable.
No. Unit 10 (Oscillations and Waves) ends at beats, and the syllabus text does not name the Doppler effect. Radioactive decay, the Carnot engine and Newton's law of cooling are also absent. They are listed in the flagged table above so you can decide how much time to give them.
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 NEET Physics one-to-one at home across Gurgaon (Gurugram) and online, with male and female tutors available.
Want a tutor to turn this NEET physics formula sheet into marks? Book a free NEET 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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