Simple Harmonic Motion Formulas: Pick the Right One Fast
Simple harmonic motion formulas all follow from x = A cos(ωt + φ) and F = −kx. Choose by what the question gives you, then check sign, phase and ω against f.
By Rahul Jeewani, Founder · Updated 14 Oct 2026

Key takeaways
Find ω first (ω = 2π/T = 2πf), then use v_max = ωA, a_max = ω²A and v = ω√(A² − x²).
- The phase constant comes from the starting position and direction: cos φ = x₀/A, and sin φ has the opposite sign to the starting velocity.
- A spring change is a change in k. Cutting a spring in half doubles k, so the period falls to 0.707 of its original value.
- T = 2π√(L/g) is a small-angle result. It is 0.43% short at 15° and 18.0% short at 90°.
In this article
- 1What are the simple harmonic motion formulas, and which one fits your question?
- 2How do you solve an SHM problem? A worked example with A = 5 cm and T = 0.4 s
- 3What is the phase constant in SHM, and how do you find it?
- 4How are uniform circular motion and angular SHM linked to the same formulas?
- 5How does cutting or joining springs change the period of a mass on a spring?
- 6When does the pendulum period formula T = 2π√(L/g) stop being accurate?
- 7How does energy move in SHM, and what happens when amplitude or frequency changes?
- 8How should you practise for MHT-CET and board exams?
- 9Frequently asked questions
Most marks in a simple harmonic motion (SHM) question are decided before any arithmetic starts, at the moment you choose the formula. Examside's past-paper archive lists 220 SHM questions in MHT-CET (Maharashtra Common Entrance Test) papers from 2019 to 2026, so the topic is worth getting right.
A long column of formulas fails the moment a question says the amplitude is doubled and the frequency halved, because you still have to know which formula applies.
This page works from the other end. Take the formula from one table, organised by what the question gives you. The rows are the question types we would practise first, which is our recommendation rather than a count: speed at a displacement, spring changes, pendulums, energy ratios and phase from a graph. Three places where mistakes are easy to make (our view) get their own sections: the phase constant, spring changes and the pendulum's small-angle limit, with a number we calculated.
What are the simple harmonic motion formulas, and which one fits your question?
Every SHM formula comes from two facts: the displacement is x = A cos(ωt + φ), and the restoring force is F = −kx, which always pushes the object back towards the mean position (the equilibrium point, where the restoring force is zero). Learn those two, then pick from the table by what the question gives you.
The core set
- Displacement: x = A cos(ωt + φ)
- Velocity: v = −Aω sin(ωt + φ)
- Acceleration: a = −ω²x
- Spring: F = −kx, so ω = √(k/m)
- Period and frequency: T = 2π/ω = 1/f, so ω = 2πf
- Energy: K = ½k(A² − x²), U = ½kx², E = ½kA² = ½mω²A²
Here A is the amplitude (the largest displacement), ω the angular frequency in rad/s, f the frequency in hertz, T the period in seconds and k the spring constant in N/m. The chapter on Oscillations in the National Council of Educational Research and Training (NCERT) Class 11 Physics textbook writes the displacement as Eq. 13.4 and the total energy as Eq. 13.18.
Which formula for which question
| The question gives you | It asks for | Use | The trap |
|---|---|---|---|
| A and T (or f) | Maximum speed, maximum acceleration | ω = 2π/T; v_max = ωA; a_max = ω²A | Putting f where ω belongs, so the 2π goes missing |
| A and a displacement x | Speed at x | v = ω√(A² − x²) | This gives the size of the speed only; direction needs the sign of the motion |
| An equation such as x = 0.05 sin(8πt) | T, f, A | The coefficient of t is ω. Here ω = 8π, so T = 0.25 s and f = 4 Hz | Reading 8π as f, which gives T = 1/(8π) |
| Mass m and spring constant k | T | T = 2π√(m/k) | T does not depend on A or on g |
| A spring cut, or two springs joined | New T | Work out the new k first (spring table below) | Cutting a spring raises k, it does not lower it |
| Length L, small swing | T | T = 2π√(L/g) | Only valid for small angles; mass does not matter |
| A rigid body swinging about a pivot | T | T = 2π√(I/(mgd)), with I about the pivot and d the pivot-to-centre-of-mass distance | Using I about the centre of mass. See moment of inertia |
| A body twisted on a wire (angular SHM) | T | T = 2π√(I/C), with C the torsion constant (restoring torque per radian) | Using m and k, when angular SHM needs I and C |
| Amplitude or frequency changes | New total energy | E = 2π²mf²A², so E ∝ A²f² | Doubling A and halving f leaves E unchanged, not halved |
| Position and direction at t = 0 | Phase constant φ | cos φ = x₀/A; sin φ has the opposite sign to v₀ | Mixing sine and cosine forms |
How do you solve an SHM problem? A worked example with A = 5 cm and T = 0.4 s
Convert to SI (metric) units, find ω from T, and every other quantity follows from it. With A = 0.05 m and T = 0.4 s, ω = 15.71 rad/s, the maximum speed is 0.785 m/s and the maximum acceleration is 12.34 m/s².
- ω = 2π/T = 2π/0.4 = 15.71 rad/s.
- v_max = ωA = 15.71 × 0.05 = 0.785 m/s, at the mean position.
- a_max = ω²A = 246.7 × 0.05 = 12.34 m/s², at x = ±A.
- Speed at x = 3 cm: v = ω√(A² − x²) = 15.71 × √(0.05² − 0.03²) = 15.71 × 0.04 = 0.628 m/s.
Run a sanity check on step 4. The numbers 3, 4 and 5 form a right-angled triangle, so √(A² − x²) is exactly 4 cm and v is 0.8 × v_max. Pass: the speed is at most ωA (equal only at the mean position). Fail: a speed above ωA means you have used f instead of ω or forgotten to convert centimetres.
What is the phase constant in SHM, and how do you find it?
The phase constant φ is the value of the phase (ωt + φ) at t = 0, so it records where in its cycle the motion starts. It is not the initial position, but once you know A, cos φ = x₀/A gives the position. The NCERT chapter says φ can be determined from the displacement at t = 0 when A is known.
Position alone leaves two possible angles, so use the direction as well. Differentiating x = A cos(ωt + φ) gives v₀ = −Aω sin φ, so sin φ has the opposite sign to v₀.
| Motion at t = 0 | φ in x = A cos(ωt + φ) |
|---|---|
| At +A | 0 |
| At the mean position, moving towards +x | −π/2 |
| At −A | π |
| At the mean position, moving towards −x | +π/2 |
| At x = A/2, moving towards +x | −π/3 |
The Maharashtra Std 12 textbook writes the same motion as x = A sin(ωt + α), where α is the initial phase. Since sin θ = cos(θ − π/2), the two forms are linked by φ = α − π/2, or α = φ + π/2. The motion is identical; only the label on the starting angle changes. Pick one form and stay with it through the whole question.
From a graph, read x at t = 0 for cos φ, then look at whether the curve is rising or falling at t = 0 for the sign of sin φ.
How are uniform circular motion and angular SHM linked to the same formulas?
A particle moving in a circle of radius A at constant angular speed ω casts a shadow on a diameter, and that shadow performs SHM with amplitude A and angular frequency ω. The angle of the rotating radius at t = 0 is the phase constant φ.
This gives a quick check: the circular speed ωA is exactly the maximum speed v_max of the shadow, and the circular acceleration ω²A is a_max.
Angular SHM follows the same pattern with torque in place of force. A restoring torque τ = −Cθ gives Iα = −Cθ, so ω = √(C/I), θ = θ₀ cos(ωt + φ) and T = 2π√(I/C). To translate any linear result, swap x for θ, k for C and m for I.
How does cutting or joining springs change the period of a mass on a spring?
The period of a mass on a spring depends only on m and k, T = 2π√(m/k), so any change to a spring is a change to k. Cutting a spring in half doubles k, because each half is stiffer, and T becomes 1/√2 = 0.707 of the original.

| Setup (identical springs of constant k) | Effective k | T compared with one spring |
|---|---|---|
| One spring cut in half, one half used | 2k | × 0.707 |
| Two springs in parallel | 2k | × 0.707 |
| Two springs in series | k/2 | × 1.414 |
The frequency of the series pair is half that of the parallel pair, a ratio of 1 : 2. For unequal springs, parallel gives k = k₁ + k₂ and series gives 1/k = 1/k₁ + 1/k₂.
For a spring hung vertically, gravity only moves the equilibrium position down by mg/k. Measure x from that new equilibrium and T = 2π√(m/k) stays exactly as it was; g does not appear in it.
When does the pendulum period formula T = 2π√(L/g) stop being accurate?
The formula is a small-angle result: the derivation replaces sin θ with θ, which holds below about 15°. At 15° the exact period is only 0.43% longer than the formula gives. At 60° it is 7.3% longer and at 90° it is 18.0% longer. OpenStax gives the same 15° limit, and NCERT makes the sin θ ≈ θ step explicit.

| Amplitude | Exact period ÷ formula period | Exact period is longer by |
|---|---|---|
| 5° | 1.0005 | 0.05% |
| 10° | 1.0019 | 0.19% |
| 15° | 1.0043 | 0.43% |
| 30° | 1.0174 | 1.74% |
| 45° | 1.0400 | 4.0% |
| 60° | 1.0732 | 7.3% |
| 90° | 1.1803 | 18.0% |
Our calculation, October 2026. The exact period is T = 4√(L/g)·K(k), where k = sin(θ₀/2) and K is the complete elliptic integral of the first kind. We evaluated K with the arithmetic-geometric mean and divided by 2π√(L/g), which gives (2/π)K(k).
Use T = 2π√(L/g) whenever a question says "small oscillations", and do not expect it to be exact beyond that. The mass of the bob and the amplitude do not appear in it. L is measured to the centre of the bob. A 1 m pendulum has T = 2π√(1/9.8) ≈ 2.01 s. In a lift accelerating upwards at a, replace g with g + a.
How does energy move in SHM, and what happens when amplitude or frequency changes?
Total energy stays fixed at E = ½kA² = ½mω²A², while kinetic and potential energy swap. At the mean position all of it is kinetic, and at x = ±A all of it is potential. NCERT notes that kinetic and potential energy both repeat after T/2, so each peaks twice per cycle.
- Kinetic energy at x: K = ½k(A² − x²). Potential energy: U = ½kx².
- Kinetic and potential energy are equal where x = ±A/√2, about 0.707A.
- At x = A/2, K = ¾E and U = ¼E.
- Rewriting E with ω = 2πf gives E = 2π²mf²A². Doubling A alone multiplies E by 4. Doubling A and halving f multiplies E by 4 × ¼ = 1, so E is unchanged.
How should you practise for MHT-CET and board exams?
Practise by question type with one fixed routine, so the choice of formula becomes automatic. We recommend three steps: write down what is given in SI units, find ω first, then test the answer against the ceilings v ≤ ωA and a ≤ ω²A. In Maharashtra, SHM sits in the Higher Secondary Certificate (HSC) Standard (Std) 12 Oscillations chapter, and NCERT places it in Class 11 Chapter 13.
Drill each row of the table in turn: speed at x, a spring change, a pendulum, an energy ratio, a phase from a graph. Our plan for MHT-CET Physics previous-year questions (PYQs) shows how to organise past papers chapter by chapter, and our HSC Physics formula sheet keeps the Maharashtra formulas in one place.
RG Lectures, founded by Rahul Jewaani (RG Sir) in May 2018, teaches Physics online. Padhna Aasaan Hai. We post free lectures on our YouTube channel, and Class 11 students can start with our MHT-CET 2028 Class 11 Physics batch. For MHT-CET 2027, our Long Term Batch is ₹1,632 as of October 2026.
Practise SHM with RG Lectures
Frequently asked questions
Sources
- 1.NCERT Class 11 Physics, Chapter 13 Oscillations
- 2.OpenStax Physics, 5.5 Simple Harmonic Motion
- 3.Examside, MHT-CET SHM questions 2019 to 2026
- 4.Our calculations (October 2026)
- 5.RG Lectures MHT-CET 2027 batches, October 2026


