JEE PYQ: Motion in a Plane - Question ID a107e47ea3f0 (JEE Main 2025)

ID: a107e47ea3f0JEE Main 2025Single Correct MCQ

A particle is projected with velocity uu so that its horizontal range is three times the maximum height attained by it. The horizontal range of the projectile is given as nu225g\frac{n u^2}{25 g}, where value of nn is: (Given, ' gg ' is the acceleration due to gravity.)

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Step-by-step Explanation

Welcome, aspiring engineers! Let's dissect this classic projectile motion problem. It tests your fundamental understanding of range and maximum height and your proficiency with trigonometric identities.


Core Formula & Concept:

In projectile motion, when a particle is launched with an initial velocity uu at an angle θ\theta with the horizontal, its trajectory is a parabola under the influence of constant gravitational acceleration gg. The key physical quantities we'll use here are the horizontal range (RR) and the maximum height (HH) attained.

The standard formulas for these quantities are:

  • Horizontal Range (R): This is the total horizontal distance covered by the projectile from its launch point until it returns to the same horizontal level. R=u2sin(2θ)gR = \frac{u^2 \sin(2\theta)}{g}
  • Maximum Height (H): This is the greatest vertical distance reached by the projectile from its launch level. H=u2sin2θ2gH = \frac{u^2 \sin^2\theta}{2g}

The problem provides a relationship between these two quantities (R=3HR = 3H) and asks us to find a specific constant nn by comparing the derived range with a given expression.


Step-by-Step Derivation:

Step 1: Write down the expressions for Range and Maximum Height.

As per our core concepts:

R=u2sin(2θ)g(Equation 1)R = \frac{u^2 \sin(2\theta)}{g} \quad \text{(Equation 1)} H=u2sin2θ2g(Equation 2)H = \frac{u^2 \sin^2\theta}{2g} \quad \text{(Equation 2)}

Step 2: Apply the given condition relating Range and Maximum Height.

The problem states that the horizontal range is three times the maximum height:

R=3H(Equation 3)R = 3H \quad \text{(Equation 3)}

Step 3: Substitute the formulas from Equation 1 and Equation 2 into Equation 3.

Substituting the expressions for RR and HH into R=3HR = 3H:

u2sin(2θ)g=3(u2sin2θ2g)\frac{u^2 \sin(2\theta)}{g} = 3 \left( \frac{u^2 \sin^2\theta}{2g} \right)

Step 4: Simplify the equation to find the launch angle θ\theta.

We can cancel out the common terms u2u^2 and gg from both sides of the equation, assuming u0u \neq 0 and g0g \neq 0:

sin(2θ)=32sin2θ\sin(2\theta) = \frac{3}{2} \sin^2\theta

Now, we use the trigonometric identity sin(2θ)=2sinθcosθ\sin(2\theta) = 2\sin\theta\cos\theta:

2sinθcosθ=32sin2θ2\sin\theta\cos\theta = \frac{3}{2} \sin^2\theta

Assuming the particle is actually projected (i.e., sinθ0\sin\theta \neq 0), we can divide both sides by sinθ\sin\theta:

2cosθ=32sinθ2\cos\theta = \frac{3}{2} \sin\theta

Rearrange the terms to find tanθ\tan\theta:

sinθcosθ=2×23\frac{\sin\theta}{\cos\theta} = \frac{2 \times 2}{3} tanθ=43\tan\theta = \frac{4}{3}

Step 5: Determine sin(2θ)\sin(2\theta) from the value of tanθ\tan\theta.

Since tanθ=43\tan\theta = \frac{4}{3}, we can visualize a right-angled triangle where the opposite side is 4 units and the adjacent side is 3 units. Using the Pythagorean theorem, the hypotenuse would be 42+32=16+9=25=5\sqrt{4^2 + 3^2} = \sqrt{16+9} = \sqrt{25} = 5 units.

From this triangle, we can find sinθ\sin\theta and cosθ\cos\theta:

sinθ=OppositeHypotenuse=45\sin\theta = \frac{\text{Opposite}}{\text{Hypotenuse}} = \frac{4}{5} cosθ=AdjacentHypotenuse=35\cos\theta = \frac{\text{Adjacent}}{\text{Hypotenuse}} = \frac{3}{5}

Now, calculate sin(2θ)\sin(2\theta) using the identity sin(2θ)=2sinθcosθ\sin(2\theta) = 2\sin\theta\cos\theta:

sin(2θ)=2(45)(35)\sin(2\theta) = 2 \left( \frac{4}{5} \right) \left( \frac{3}{5} \right) sin(2θ)=2425\sin(2\theta) = \frac{24}{25}

Step 6: Substitute the value of sin(2θ)\sin(2\theta) back into the Range formula.

Using Equation 1 and the calculated value of sin(2θ)\sin(2\theta):

R=u2g(2425)R = \frac{u^2}{g} \left( \frac{24}{25} \right) R=24u225gR = \frac{24 u^2}{25 g}

Step 7: Compare the derived range with the given expression to find nn.

The problem states that the horizontal range is given as nu225g\frac{n u^2}{25 g}.

Comparing our derived expression R=24u225gR = \frac{24 u^2}{25 g} with the given form R=nu225gR = \frac{n u^2}{25 g}, we can clearly see that:

n=24n = 24

Thus, the value of nn is 24.


Common Traps & Exam Tip:
  • Trigonometric Identity Mix-up: A common mistake is to confuse sin(2θ)\sin(2\theta) with 2sinθ2\sin\theta or sin2θ\sin^2\theta. Always remember sin(2θ)=2sinθcosθ\sin(2\theta) = 2\sin\theta\cos\theta. Similarly, ensure you distinguish sin2θ\sin^2\theta (which is (sinθ)2(\sin\theta)^2) correctly.
  • Algebraic Errors: Be careful while simplifying the equation after substituting RR and HH. Dividing by sinθ\sin\theta is valid only if sinθ0\sin\theta \neq 0, which is true for a projectile with non-zero height.
  • Calculation of sin(2θ)\sin(2\theta) from tanθ\tan\theta: After finding tanθ=4/3\tan\theta = 4/3, some students might try to find θ\theta using an inverse tangent function and then calculate sin(2θ)\sin(2\theta). This is unnecessary and can lead to rounding errors. It's more accurate and faster to construct a right-angled triangle to find sinθ\sin\theta and cosθ\cos\theta directly, then use sin(2θ)=2sinθcosθ\sin(2\theta) = 2\sin\theta\cos\theta.

Exam Tip: For such problems, a systematic approach is crucial. First, write down all relevant formulas. Second, set up the relationship given in the problem. Third, use trigonometric identities to simplify and solve for the unknown angle or a related trigonometric function. Finally, substitute back to find the required quantity. Always double-check your calculations, especially trigonometric manipulations.