Verified Solution • 2025–26 Session moderate

QJEEM24Ph3831: JEE Main 2024 Physics - Class 11 JEEM24Ph3831 Solution: A body projected vertically upwards with a certain speed from…

A body projected vertically upwards with a certain speed from the top of a tower reaches the ground in t1t_1 . If it is projected vertically downwards from the same point with the same speed, it reaches the ground in t2t_2 . Time required to reach the ground, if it is dropped from the top of the tower, is :

Multiple Choice Options

  • A t1+t2\sqrt{\mathrm{t}_1+\mathrm{t}_2}
  • B t1t2\sqrt{\mathrm{t}_1 \mathrm{t}_2}
  • C t1t2\sqrt{\frac{\mathrm{t}_1}{\mathrm{t}_2}}
  • D t1−t2\sqrt{\mathrm{t}_1-\mathrm{t}_2}

Step-by-Step Verified Solution

To solve this problem, we'll use the equations of motion under constant acceleration due to gravity. Let's define:

hh : Height of the tower

uu : Initial speed of projection (same magnitude in both cases)

gg : Acceleration due to gravity (positive downward)

t1t_1 : Time taken to reach the ground when projected upwards

t2t_2 : Time taken to reach the ground when projected downwards

tt : Time taken to reach the ground when simply dropped

Case 1: Projectile Thrown Upwards

When the body is projected upwards from the top of the tower, its initial velocity is −u-u (since upward direction is negative), and it reaches the ground in time t1t_1 . The equation of motion is:

h=−ut1+12gt12h = -u t_1 + \frac{1}{2} g t_1^2

Case 2: Projectile Thrown Downwards

When the body is projected downwards from the top of the tower, its initial velocity is uu , and it reaches the ground in time t2t_2 . The equation is:

h=ut2+12gt22h = u t_2 + \frac{1}{2} g t_2^2

Case 3: Body Dropped

When the body is simply dropped, its initial velocity is 00 , and it reaches the ground in time tt :

h=12gt2h = \frac{1}{2} g t^2

Step 1: Equate the Heights

From cases 1 and 2, equate the expressions for hh :

−ut1+12gt12=ut2+12gt22-u t_1 + \frac{1}{2} g t_1^2 = u t_2 + \frac{1}{2} g t_2^2

Step 2: Solve for uu

Simplify the equation:

−ut1−ut2=12gt22−12gt12-u t_1 - u t_2 = \frac{1}{2} g t_2^2 - \frac{1}{2} g t_1^2

−u(t1+t2)=12g(t22−t12)-u (t_1 + t_2) = \frac{1}{2} g (t_2^2 - t_1^2)

−u(t1+t2)=12g(t2−t1)(t2+t1)-u (t_1 + t_2) = \frac{1}{2} g (t_2 - t_1)(t_2 + t_1)

Divide both sides by t1+t2t_1 + t_2 :

−u=12g(t2−t1)-u = \frac{1}{2} g (t_2 - t_1)

u=12g(t1−t2)u = \frac{1}{2} g (t_1 - t_2)

Step 3: Express hh in Terms of t1t_1 and t2t_2

Substitute uu back into one of the equations for hh :

h=−(12g(t1−t2))t1+12gt12h = -\left( \frac{1}{2} g (t_1 - t_2) \right) t_1 + \frac{1}{2} g t_1^2

Simplify:

h=12gt1t2h = \frac{1}{2} g t_1 t_2

Step 4: Equate the Height for the Dropped Case

From the dropped case:

h=12gt2h = \frac{1}{2} g t^2

Set the two expressions for hh equal to each other:

12gt2=12gt1t2\frac{1}{2} g t^2 = \frac{1}{2} g t_1 t_2

t2=t1t2t^2 = t_1 t_2

Step 5: Solve for tt

t=t1t2t = \sqrt{t_1 t_2}

Conclusion:

The time required for the body to reach the ground when dropped is the geometric mean of t1t_1 and t2t_2 :

Answer: Option B

t=t1 t2t = \sqrt{t_1 \, t_2}

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