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Motion in a Plane - Projectile Motion

Grade 11CBSEPhysics

Review the key concepts, formulae, and examples before starting your quiz.

🔑Concepts

Projectile motion is a form of motion experienced by an object or particle (a projectile) that is thrown near the Earth's surface and moves along a curved path under the action of gravity only.

The motion of a projectile is a two-dimensional motion that can be resolved into two independent one-dimensional motions: a horizontal motion with constant velocity and a vertical motion with constant acceleration (gg).

Horizontal component of velocity remains constant throughout the motion: ux=ucosθu_x = u \cos \theta, because horizontal acceleration ax=0a_x = 0.

Vertical component of velocity changes linearly with time: uy=usinθgtu_y = u \sin \theta - gt, because vertical acceleration ay=ga_y = -g.

The trajectory of a projectile is a parabola, represented by the equation y=xtanθgx22u2cos2θy = x \tan \theta - \frac{gx^2}{2u^2 \cos^2 \theta}.

The horizontal range RR is the same for two angles of projection θ\theta and (90θ)(90^\circ - \theta), provided the initial velocity uu is the same.

Range is maximum when the angle of projection θ=45\theta = 45^\circ.

📐Formulae

ux=ucosθu_x = u \cos \theta

uy=usinθu_y = u \sin \theta

T=2usinθgT = \frac{2u \sin \theta}{g}

H=u2sin2θ2gH = \frac{u^2 \sin^2 \theta}{2g}

R=u2sin2θgR = \frac{u^2 \sin 2\theta}{g}

y=xtanθgx22u2cos2θy = x \tan \theta - \frac{gx^2}{2u^2 \cos^2 \theta}

v=vx2+vy2=(ucosθ)2+(usinθgt)2v = \sqrt{v_x^2 + v_y^2} = \sqrt{(u \cos \theta)^2 + (u \sin \theta - gt)^2}

💡Examples

Problem 1:

A cricket ball is thrown with a velocity of 28 m/s28 \text{ m/s} at an angle of 3030^\circ above the horizontal. Calculate (a) the maximum height, (b) the time taken by the ball to return to the same level, and (c) the distance from the thrower to the point where the ball returns to the same level. (Take g=9.8 m/s2g = 9.8 \text{ m/s}^2)

Solution:

Given: u=28 m/su = 28 \text{ m/s}, θ=30\theta = 30^\circ, g=9.8 m/s2g = 9.8 \text{ m/s}^2. (a) Maximum height: H=u2sin2θ2g=282×sin2302×9.8=784×0.2519.6=10 mH = \frac{u^2 \sin^2 \theta}{2g} = \frac{28^2 \times \sin^2 30^\circ}{2 \times 9.8} = \frac{784 \times 0.25}{19.6} = 10 \text{ m}. (b) Time of flight: T=2usinθg=2×28×sin309.8=56×0.59.82.86 sT = \frac{2u \sin \theta}{g} = \frac{2 \times 28 \times \sin 30^\circ}{9.8} = \frac{56 \times 0.5}{9.8} \approx 2.86 \text{ s}. (c) Horizontal range: R=u2sin2θg=282×sin609.8=784×0.8669.869.3 mR = \frac{u^2 \sin 2\theta}{g} = \frac{28^2 \times \sin 60^\circ}{9.8} = \frac{784 \times 0.866}{9.8} \approx 69.3 \text{ m}.

Explanation:

We use the standard formulae for projectile motion. The maximum height depends on the vertical component of velocity, while the range depends on both components and the total time the object stays in the air.

Problem 2:

Show that for a projectile, the angle of projection θ\theta for which the horizontal range and the maximum height are equal is given by θ=tan1(4)\theta = \tan^{-1}(4).

Solution:

Condition: R=HR = H. u2sin2θg=u2sin2θ2g\frac{u^2 \sin 2\theta}{g} = \frac{u^2 \sin^2 \theta}{2g} 2u2sinθcosθg=u2sin2θ2g\frac{2u^2 \sin \theta \cos \theta}{g} = \frac{u^2 \sin^2 \theta}{2g} 2cosθ=sinθ22 \cos \theta = \frac{\sin \theta}{2} 4=sinθcosθ4 = \frac{\sin \theta}{\cos \theta} tanθ=4    θ=tan1(4)\tan \theta = 4 \implies \theta = \tan^{-1}(4).

Explanation:

By equating the expressions for Horizontal Range (RR) and Maximum Height (HH), we simplify the trigonometric terms to find the specific ratio of sinθ\sin \theta to cosθ\cos \theta.

Projectile Motion - Revision Notes & Key Formulas | CBSE Class 11 Physics