Q.A man throws a ball to a maximum horizontal distance of 80 metres. Calculate the maximum height reached.
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Projectile Motion
Projectile Motion — From Intuition to Precision
Imagine you throw a ball to a friend. It doesn't travel in a straight line — it rises, slows down, then curves downward and falls. That curved path is a projectile's trajectory. The ball is a projectile: any object that is launched into the air and then moves only under the influence of gravity (and air resistance, which we ignore for now).
The key intuition: once the ball leaves your hand, the only force acting on it is gravity pulling it straight down. There is no forward force after release. The ball keeps moving forward because of inertia — it wants to keep going in a straight line at constant speed. But gravity keeps pulling it down, so the forward motion and downward acceleration combine to produce a curved path.
The Precise Statement
Projectile motion is the two-dimensional motion of an object launched into the air, subject only to the constant downward acceleration due to gravity (g≈9.8m/s2). Air resistance is neglected.
We break the motion into two independent components:
- Horizontal motion: No acceleration (ax=0). So horizontal velocity vx is constant.
- Vertical motion: Constant downward acceleration (ay=−g). So vertical velocity vy changes linearly with time.
The independence of these components is the central idea — what happens vertically does not affect what happens horizontally, and vice versa.
The Equations (for a projectile launched with initial speed u at angle θ above horizontal)
First, resolve the initial velocity:
ux=ucosθ,uy=usinθ
Horizontal motion (constant velocity):
x=uxt=(ucosθ)t
Vertical motion (constant acceleration −g):
vy=uy−gt=usinθ−gt
y=uyt−21gt2=(usinθ)t−21gt2
Key Results You Must Know
Time of flight T: total time the projectile stays in the air (until y=0 again).
T=g2usinθ
Maximum height H: the highest vertical position reached (when vy=0).
H=2gu2sin2θ
Range R: the horizontal distance covered when it returns to launch height.
R=gu2sin2θ
The range is maximum when sin2θ=1, i.e., θ=45∘. For a given speed, 45∘ gives the farthest throw.
The Trajectory Equation (Path Shape)
Eliminate t from the x and y equations to get y as a function of x:
y=xtanθ−2u2cos2θgx2
This is a parabola — the signature shape of projectile motion.
Common Mistake to Avoid …
[!TLDR] Maximum horizontal range occurs at a 45° launch angle, for which the maximum height reached is exactly one …
The maximum possible horizontal distance for a given launch speed u is achieved at θ=45°, where Rmax=gu2. Here Rmax=80 m, so u2=80g. At θ=45°, sinθ=cosθ=21, so the height reached is $H=\dfrac{u^2\sin^2\theta}{2g}=\dfrac{u^2(1/2)}{2g}=\dfrac{u^2}{ …
Recognise that 'maximum horizontal distance' implies the 45° launch angle that maximises range, then use H = u²sin …
Trying to solve for u and θ separately without recognising that 'maximum horizontal distance' already fixes θ = 45°, making t …
- CBSE 2026Set ANNUAL1 markMCQQ.The value of acceleration at the highest point of the projectile path is(a) zero(b) maximum(c) minimum(d) equal to g
›Reveal solutionSolution
Throughout projectile motion the acceleration equals g, so at the top it is also g. Answer (D).
In projectile motion (ignoring air resistance) the only force is gravity. Hence the acceleration is constant and equals g (about 9.8 m/s^2), pointing vertically downward, at all instants.
…
- CBSE 2025Set ANNUAL1 markMCQQ.The maximum limit (range) of a gun is 3920 m. What is the velocity of shoot? (A) 200 m/s (B) 196 m/s (C) 100 m/s (D) 150 m/s
›Reveal solutionSolution
The gun's muzzle speed is 196 m/s, found from the maximum-range formula of projectile motion.
The range of a projectile launched with speed u at angle θ is R=gu2sin2θ. The range is maximum when θ=45∘ (so sin2θ=1), giving:
Rmax=gu2
…
- CBSE 2024Set SET-AP55001 markQ.The path of projectile motion is ________.
›Reveal solutionSolution
The trajectory traced by a projectile (launched at an angle to the horizontal, under gravity alone) is a parabola.
For a projectile launched with initial speed u at angle θ, the horizontal motion has constant velocity u cos θ (no horizontal force, ignoring air resistance), so x = (u cos θ) t. The vertical motion is uniformly accelerated by gravity, so y = (u sin θ) t − ½gt^2.
Eliminating t (t = x / (u cos θ)) and substituting into the y-equation gives: …
- CBSE 2020Set ANNUAL1 markQ.Answer in one word/one sentence: Which quantity is constant in projectile motion?
›Reveal solutionSolution
Gravity gives the projectile a constant downward acceleration g, but no horizontal acceleration, so the horizontal velocity component vx stays fixed for the whole flight.
During projectile motion (ignoring air resistance), the only force acting is gravity, which acts vertically downward. This produces a constant downward acceleration g, changing the vertical velocity component continuously (vy = uy - gt). There is no horizontal force, so the horizontal acceleration is …
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