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Constant Acceleration Formula

Kinematics formulasAP Physics 1Class 11Updated 1 Nov 2026

x=x0+v0t+12at2x = x_0 + v_0 t + \frac{1}{2}at^2
SI unit
m/s²
Dimensions
[M⁰ L¹ T⁻²]
where
  • x position at time t m
  • x₀ starting position m
  • v₀ initial velocity m/s
  • a constant acceleration m/s²
  • t time s

The constant acceleration formula used in AP Physics is x=x0+v0t+12at2x = x_0 + v_0 t + \frac{1}{2}at^2. It gives the position x of an object at time t when it starts at x0x_0 with velocity v0v_0 and its acceleration a never changes. Three partner equations complete the set, and together they are called the kinematic equations.

Indian books write the same ideas with u for v0v_0 and s for x−x0x - x_0, and call them the equations of motion. The physics is identical. What matters is the condition in the name: the acceleration may not grow, shrink or turn at any point in the interval, as in free fall or steady braking.

Quick facts

  • Position

    x=x0+v0t+12at2x = x_0 + v_0 t + \frac{1}{2}at^2
  • Velocity

    v=v0+atv = v_0 + at
  • No time

    v2=v02+2a(x−x0)v^2 = v_0^2 + 2a(x - x_0)
  • No acceleration

    x−x0=(v0+v)2tx - x_0 = \frac{(v_0 + v)}{2}t
  • Unit of a

    m/s², dimension [M⁰ L¹ T⁻²]
  • Graph sign

    Straight line on a velocity time graph

Constant acceleration formula physics: the four kinematic equations

The kinematic equations in two notations
US formIndian formMissing quantity
v=v0+atv = v_0 + atv=u+atv = u + atdisplacement
x=x0+v0t+12at2x = x_0 + v_0 t + \frac{1}{2}at^2s=ut+12at2s = ut + \frac{1}{2}at^2final velocity
v2=v02+2a(x−x0)v^2 = v_0^2 + 2a(x - x_0)v2=u2+2asv^2 = u^2 + 2astime
x−x0=(v0+v)2tx - x_0 = \frac{(v_0 + v)}{2}ts=(u+v)2ts = \frac{(u + v)}{2}tacceleration

Pick the equation that leaves out the quantity you neither know nor need. The x₀ term in the position form is a convenience: it lets you place the object anywhere on an axis, which helps when two objects start at different points.

How to tell the acceleration is constant

  • The net force on the object is constant, for example gravity alone near Earth's surface.
  • The velocity time graph is a straight line. Its slope is a.
  • The position time graph is a parabola, curving up for positive a and down for negative a.
  • The acceleration time graph is a flat horizontal line.

If none of these hold, as for a car with changing throttle or a falling object with strong air resistance, the kinematic equations give wrong answers.

Worked examples

Example 1: a cart on a track

A cart starts at x₀ = 2.0 m with v₀ = 3.0 m/s and a constant acceleration of −0.50 m/s². Where is it at t = 4.0 s?

x=2.0+3.0(4.0)+12(−0.50)(4.0)2=2.0+12−4.0=10 mx = 2.0 + 3.0(4.0) + \tfrac{1}{2}(-0.50)(4.0)^2 = 2.0 + 12 - 4.0 = 10\ \text{m}

Example 2: a road test quoted in km/h

A car goes from rest to 100 km/h in 8.0 s with steady acceleration. Find the acceleration and the distance covered.

100 ÷ 3.6 ≈ 27.8 m/s.

a=27.8−08.0≈3.47 m/s2a = \frac{27.8 - 0}{8.0} \approx 3.47\ \text{m/s}^2

x−x0=(0+27.8)2×8.0≈111 mx - x_0 = \frac{(0 + 27.8)}{2} \times 8.0 \approx 111\ \text{m}

Example 3: a ball thrown up from a height

A ball leaves a hand 1.5 m above the ground moving upward at 8.0 m/s. When does it land? Measure x upward from the ground.

0=1.5+8.0t−4.9t20 = 1.5 + 8.0t - 4.9t^2, so 4.9t2−8.0t−1.5=04.9t^2 - 8.0t - 1.5 = 0.

t=8.0+64+29.49.8=8.0+9.669.8≈1.80 st = \frac{8.0 + \sqrt{64 + 29.4}}{9.8} = \frac{8.0 + 9.66}{9.8} \approx 1.80\ \text{s}

The other root is negative and has no physical meaning here.

A dimension check on the position formula

Every term must be a length. x0x_0 is in m. v0tv_0 t is (m/s)(s) = m. 12at2\frac{1}{2}at^2 is (m/s²)(s²) = m. The ½ has no dimensions, so a dimension check cannot tell you whether it belongs there; only the derivation can. For the acceleration itself, the dimensions are [M⁰ L¹ T⁻²], as set out on the acceleration formula page.

Traps

  • Sign of g. If x increases upward, the acceleration is −9.8 m/s² throughout the flight, rising and falling alike.
  • Splitting the motion when you do not need to. One equation covers the up and down path as long as a stays constant.
  • Keeping the wrong root of a quadratic in t.
  • Mixing notations. Do not write u in one line and v₀ in the next.

The u and s versions live on the formula of motion page, v = v₀ + at gets its own treatment as the final velocity formula, and projectile uses are listed under kinematics formulas.

Frequently asked questions

What is the constant acceleration formula?

The main one is x = x₀ + v₀t + ½at². Its partners are v = v₀ + at, v² = v₀² + 2a(x − x₀) and x − x₀ = (v₀ + v)t / 2.

Is free fall an example of constant acceleration?

Yes, provided drag is negligible. The acceleration is g = 9.8 m/s² downward the whole time.

Can the velocity be zero while acceleration is constant?

Yes. A ball thrown upward has zero velocity at the top, but its acceleration is still g downward.

What does a constant acceleration look like on a graph?

Velocity against time is a tilted straight line, position against time is a parabola, and acceleration against time is level.

Are the kinematic equations the same as the equations of motion?

Yes. US courses call them kinematic equations and write v₀ and Δx. Indian courses call them equations of motion and write u and s.