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two bodies are projected from the top of a tower in opposite directions with velocities of u1 and u2 simultaneously. find the time when their velocities are mutually perpendicular.

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If two bodies are projected from the top of a tower in opposite directions with velocities of u₁ and u₂ simultaneously, the time when their velocities are mutually perpendicular is t = √(u₁u₂)/g

If two bodies are projected from the top of a tower in opposite directions with velocities of u₁ and u₂ simultaneously. To find the time when their velocities are mutually perpendicular, we proceed as follows

Since the bodies have initial velocities u₁ and u₂, their velcities at any point in vector form is using the equation of motion under gravity, v = u - gt

For body 1 v₁ = u₁ - gt

For body 2 v₂ = u₂ - gt

Now for the velocities of the bodies to be mutually perpendicular, their dot product must be zero.

So, v₁.v₂ = 0

(u₁ - gt).(u₂ - gt) = 0

u₁.u₂ - u₁.gt + u₂.(- gt) + (- gt).(-gt) = 0

u₁.u₂ - u₁.gt - u₂.(gt) + (gt).(gt) = 0

Now,

  • u₁.u₂ = u₁u₂cos180 = -u₁u₂(since they are projected in opposite directions and parallel and the angle between them is zero)
  • u₁.gt = 0 (since they are perpendicular)
  • u₂.(gt) = 0 (since they are perpendicular) and
  • (gt).(gt) = (gt)(gt)cos0 = g²t² (since they are parallel and the angle between them is zero)

Thus

u₁.u₂ - u₁.gt - u₂.(gt) + (gt).(gt) = 0

-u₁u₂ - 0 - 0 + g²t² = 0

-u₁u₂ - 0 + g²t² = 0

-u₁u₂ + g²t² = 0

-u₁u₂ = -g²t²

Dividing both sides by -g², we have that

-u₁u₂/-g² = -g²t²/-g²

t² = u₁u₂/g²

Taking square root of both sides, we have that

t² = u₁u₂/g²

√t² = √(u₁u₂/g²)

t = √(u₁u₂)/g

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