JEE PYQ: Motion in a Plane - Question ID 31f017e8fa2e (JEE Main 2004)

ID: 31f017e8fa2eJEE Main 2004Single Correct MCQ
A projectile can have the same range 'R' for two angles of projection. If T1 and T2 be the time of flights in the two cases, then the product of the two time of flights is directly proportional to

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Step-by-step Explanation

Core Formula & Concept:

In projectile motion, an object is launched at an angle θ\theta with the horizontal and moves under the influence of gravity. Two key quantities are:

  • Range (RR): The horizontal distance traveled by the projectile before returning to the same vertical level. The formula for range is: R=u2sin2θgR = \frac{u^2 \sin 2\theta}{g} where uu is the initial speed, θ\theta is the projection angle, and gg is the acceleration due to gravity.
  • Time of Flight (TT): The total time the projectile remains in the air. It is given by: T=2usinθgT = \frac{2u \sin \theta}{g}

A crucial observation is that the range RR depends on sin2θ\sin 2\theta, which is symmetric about θ=45\theta = 45^\circ. This means that for a given initial speed uu, two different angles θ\theta and (90θ)(90^\circ - \theta) yield the same range. These are called complementary angles.

Let θ1=θ\theta_1 = \theta and θ2=90θ\theta_2 = 90^\circ - \theta. Then: sin2θ1=sin2θ,sin2θ2=sin(1802θ)=sin2θ\sin 2\theta_1 = \sin 2\theta, \quad \sin 2\theta_2 = \sin(180^\circ - 2\theta) = \sin 2\theta Hence, RR is the same for both angles.

The question asks about the product of the two times of flight, T1T_1 and T2T_2, corresponding to these two angles, and how it relates to RR.

Step-by-Step Derivation:

Let’s denote:

- T1T_1 = time of flight for angle θ\theta - T2T_2 = time of flight for angle (90θ)(90^\circ - \theta) Using the time of flight formula: T1=2usinθg,T2=2usin(90θ)g=2ucosθgT_1 = \frac{2u \sin \theta}{g}, \quad T_2 = \frac{2u \sin(90^\circ - \theta)}{g} = \frac{2u \cos \theta}{g} Now, compute the product T1T2T_1 \cdot T_2: T1T2=(2usinθg)(2ucosθg)=4u2sinθcosθg2T_1 \cdot T_2 = \left(\frac{2u \sin \theta}{g}\right) \left(\frac{2u \cos \theta}{g}\right) = \frac{4u^2 \sin \theta \cos \theta}{g^2} Recall the double-angle identity: sin2θ=2sinθcosθsinθcosθ=sin2θ2\sin 2\theta = 2 \sin \theta \cos \theta \Rightarrow \sin \theta \cos \theta = \frac{\sin 2\theta}{2} Substitute this into the product: T1T2=4u2g2sin2θ2=2u2sin2θg2T_1 \cdot T_2 = \frac{4u^2}{g^2} \cdot \frac{\sin 2\theta}{2} = \frac{2u^2 \sin 2\theta}{g^2} But from the range formula: R=u2sin2θgsin2θ=Rgu2R = \frac{u^2 \sin 2\theta}{g} \Rightarrow \sin 2\theta = \frac{Rg}{u^2} Substitute sin2θ\sin 2\theta back into the product: T1T2=2u2g2Rgu2=2RgT_1 \cdot T_2 = \frac{2u^2}{g^2} \cdot \frac{Rg}{u^2} = \frac{2R}{g} Thus: T1T2=2gRT_1 \cdot T_2 = \frac{2}{g} R This shows that the product of the two times of flight is directly proportional to RR, with the constant of proportionality being 2g\frac{2}{g}.

Hence, the correct option is A: RR. Common Traps & Exam Tip:

Students often make the following mistakes:

  • Ignoring the complementary angle relationship: They may try to compute T1T_1 and T2T_2 for arbitrary angles, not realizing that the two angles are complementary (90θ90^\circ - \theta). This leads to unnecessary complexity.
  • Misapplying trigonometric identities: Forgetting that sin(90θ)=cosθ\sin(90^\circ - \theta) = \cos \theta or not using sin2θ=2sinθcosθ\sin 2\theta = 2 \sin \theta \cos \theta can result in incorrect expressions.
  • Confusing proportionality with equality: The question asks for proportionality, not exact equality. Students may overlook the constant factor 2g\frac{2}{g} and think the product equals RR, which is conceptually correct in terms of proportionality but may cause confusion in numerical problems.
  • Assuming T1T2T_1 \cdot T_2 depends on R2R^2 or 1/R1/R: Without derivation, some guess that the product might involve R2R^2 or inverse relations, especially if they confuse time with velocity or acceleration.

Exam Tip: Always start by writing down known formulas and use trigonometric identities early. Recognize symmetry in projectile motion—complementary angles give the same range but different times of flight. This symmetry is a powerful tool in solving such problems efficiently.