Verified Solution • 2025–26 Session moderate

QJEEM25Ph55a4: JEE Main 2025 Physics - Class 11 JEEM25Ph55a4 Solution: An object of mass ' m ' is projected from origin in a vertical…

An object of mass ' m ' is projected from origin in a vertical xy plane at an angle 45∘45^{\circ} with the x−\mathrm{x}- axis with an initial velocity v0\mathrm{v}_0 . The magnitude and direction of the angular momentum of the object with respect to origin, when it reaches at the maximum height, will be [ g is acceleration due to gravity]

Multiple Choice Options

  • A mvo322g\frac{m v_o{ }^3}{2 \sqrt{2} g} along negative zz -axis
  • B mvo322g\frac{m v_o^3}{2 \sqrt{2} g} along positive zz -axis
  • C mvo342g\frac{m v_o^3}{4 \sqrt{2} g} along positive zz -axis
  • D mvo342g\frac{m v_o^3}{4 \sqrt{2} g} along negative z-axis

Step-by-Step Verified Solution

v0⃗=v02 i^+v02 j^.\vec{v_0} = \frac{v_0}{\sqrt{2}}\,\hat{i} + \frac{v_0}{\sqrt{2}}\,\hat{j}.

At maximum height, the vertical component of the velocity becomes zero. Setting the vertical velocity to zero:

v02−g t=0⟹t=v0g2.\frac{v_0}{\sqrt{2}} - g\,t = 0 \quad \Longrightarrow \quad t = \frac{v_0}{g\sqrt{2}}.

The coordinates at this time are:

x=v02 t=v02⋅v0g2=v022g,x = \frac{v_0}{\sqrt{2}}\,t = \frac{v_0}{\sqrt{2}} \cdot \frac{v_0}{g\sqrt{2}} = \frac{v_0^2}{2g},

y=v02 t−12g t2=v022g−12g v022g2=v022g−v024g=v024g.y = \frac{v_0}{\sqrt{2}}\,t - \frac{1}{2}g\,t^2 = \frac{v_0^2}{2g} - \frac{1}{2}g\,\frac{v_0^2}{2g^2} = \frac{v_0^2}{2g} - \frac{v_0^2}{4g} = \frac{v_0^2}{4g}.

Thus, the position vector at maximum height is:

r⃗=v022g i^+v024g j^.\vec{r} = \frac{v_0^2}{2g}\,\hat{i} + \frac{v_0^2}{4g}\,\hat{j}.

At maximum height, the only nonzero component of velocity is the horizontal one:

v⃗=v02 i^.\vec{v} = \frac{v_0}{\sqrt{2}}\,\hat{i}.

The angular momentum about the origin is given by:

L⃗=m r⃗×v⃗.\vec{L} = m\,\vec{r} \times \vec{v}.

Writing out the cross product:

r⃗×v⃗=(v022g i^+v024g j^)×v02 i^.\vec{r} \times \vec{v} = \left(\frac{v_0^2}{2g}\,\hat{i} + \frac{v_0^2}{4g}\,\hat{j}\right) \times \frac{v_0}{\sqrt{2}}\,\hat{i}.

Since the cross product of i^\hat{i} with itself is zero and:

j^×i^=−k^,\hat{j} \times \hat{i} = -\hat{k},

we have:

r⃗×v⃗=v024g⋅v02 (−k^)=−v0342g k^.\vec{r} \times \vec{v} = \frac{v_0^2}{4g} \cdot \frac{v_0}{\sqrt{2}}\, (-\hat{k}) = -\frac{v_0^3}{4\sqrt{2}g}\,\hat{k}.

Thus, the angular momentum is:

L⃗=−m v0342g k^.\vec{L} = -\frac{m\,v_0^3}{4\sqrt{2}g}\,\hat{k}.

This means the magnitude is:

m v0342g,\frac{m\,v_0^3}{4\sqrt{2}g},

and its direction is along the negative k^\hat{k} (or negative zz -axis).

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