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Formulas/physics/Kinematics/Horizontal Projection — Time of Flight

Horizontal Projection — Time of Flight

Time for a horizontally projected body to fall height h.
Class 11Class JEE
Derivation

The situation

A body is projected horizontally — at angle θ=0°\theta = 0° — from a height hh above the ground. It has initial horizontal velocity uu and zero initial vertical velocity.

It travels forward while simultaneously falling under gravity. The question: how long before it hits the ground?

Key observation

Since the body is launched horizontally, it has no initial vertical velocity. The vertical motion is identical to a body simply dropped from height hh — the horizontal motion has no effect on how fast it falls.

Derivation

Take downward as positive for the vertical direction. The body starts at height hh above the ground, so it must fall a vertical distance hh.

Initial vertical velocity: uy=0u_y = 0 (horizontal launch)

Vertical acceleration: +g+g (downward)

Using the second equation of motion for vertical displacement:

h=uyT+12gT2h = u_y \cdot T + \frac{1}{2}gT^2

h=0T+12gT2h = 0 \cdot T + \frac{1}{2}gT^2

h=12gT2h = \frac{1}{2}gT^2

T2=2hgT^2 = \frac{2h}{g}

T=2hg\boxed{T = \sqrt{\frac{2h}{g}}}

What this tells us

The time of flight depends only on the height hh and gravity gg. It does not depend on the horizontal velocity uu at all.

A ball rolled off a table at 22 m/s and one rolled off at 2020 m/s both hit the ground at exactly the same time — provided the table is the same height.

This is a direct consequence of the independence of horizontal and vertical motions.

Comparison with free fall

A body dropped from rest from height hh also takes time T=2hgT = \sqrt{\frac{2h}{g}} to reach the ground. The horizontally projected body takes exactly the same time — it just lands further away.

This is one of the most striking results in kinematics.

BodyInitial vertical velocityTime to fall height hh
Dropped from rest002hg\sqrt{\frac{2h}{g}}
Projected horizontally002hg\sqrt{\frac{2h}{g}}
Projected at angle θ\theta upwardusinθ>0u\sin\theta > 0Longer than 2hg\sqrt{\frac{2h}{g}}
Projected at angle θ\theta downwardusinθ<0u\sin\theta < 0Shorter than 2hg\sqrt{\frac{2h}{g}}
Key Idea
A classic demonstration: fire a bullet horizontally and simultaneously drop another bullet from the same height. Both hit the ground at the same time. The horizontal velocity of the fired bullet does not affect its fall — only the height matters.