MHB Motion of Particles in Uniform Gravitational Field

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Two particles in a uniform gravitational field move horizontally with initial velocities of 3 m/s and 4 m/s in opposite directions. Their vertical components of velocity increase due to gravity, and they become perpendicular after a time \( t \) calculated as \( t = \frac{\sqrt{v_1 v_2}}{g} \). The horizontal distances covered by each particle during this time are \( x_1 = v_1 t \) and \( x_2 = v_2 t \). The total separation between the particles when their velocities are perpendicular is given by \( x_1 + x_2 = (v_1 + v_2) \frac{\sqrt{v_1 v_2}}{g} \). This analysis provides a clear understanding of the motion of particles in a uniform gravitational field.
DrunkenOldFool
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Two particles move in a uniform gravitational field with an acceleration $g$. At the initial moment the particles were located at one point and moved with velocities $v_1 = 3 \text{ms}^{-1}$ and $v_1 = 4 \text{ms}^{-1}$ horizontally in opposite directions. Find distance between the particles when their velocities become mutually perpendicular.
 
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DrunkenOldFool said:
Two particles move in a uniform gravitational field with an acceleration $g$. At the initial moment the particles were located at one point and moved with velocities $v_1 = 3 \text{ms}^{-1}$ and $v_1 = 4 \text{ms}^{-1}$ horizontally in opposite directions. Find distance between the particles when their velocities become mutually perpendicular.
The two horizontal components of velocity are constant, and the vertical components are always equal. Now draw a velocity diagram for when the two velocities are perpendicular, and solve the diagram for the vertical component of velocity (it should come to \(2 \sqrt{3}\) m/s if my scratch algebra and arithmetic are correct).

Now you can find the time \(t\) it took the vertical component to reach this value, and the separation is \(7t\) m.

CB
 
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Let the velocities of the particles (say $\vec{v_{1}}'$ and $\vec{v_2 }'$) become perpendicular after time $t$. By equation of motion,

$$ \vec{v_{1}'}=\vec{v_{1}}+\vec{g}t \\ \vec{v_{2}'}=\vec{v_{2}}+\vec{g}t$$

As $\vec{v_1 ' }$ and $\vec{v_2 '}$ are perpendicular, we can write

$$ \begin{align*} \vec{v_1 ' } \cdot \vec{v_2 ' } &=0 \\ (\vec{v_{1}}+\vec{g}t) \cdot (\vec{v_{2}}+\vec{g}t) &= 0 \\ -v_1 v_2 +g^2 t^2 &=0 \\ t &= \frac{\sqrt{v_1 v_2}}{g}\end{align*}$$

Let $x_1$ and $x_2$ be the horizontal distances covered by particles 1 and 2 in time $t$ respectively. Note that the acceleration in horizontal direction is zero.

$$x_1 = v_1 t = v_1 \frac{\sqrt{v_1 v_2}}{g} \\ x_2 = v_2 t = v_2 \frac{\sqrt{v_1 v_2}}{g}$$

The total separation between the particles is

$$x_1+x_2= (v_1+v_2)\frac{\sqrt{v_1 v_2}}{g}$$
 
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This is my try.

View attachment 277

considering the triangle $ABC$,

$$\begin{align*}
\alpha &=90^\circ - \beta \\
\tan{\alpha} &= \tan (90^\circ -\beta ) \\
\tan{\alpha} &= \cot \beta \\
\frac{gt}{v_1}&=\frac{v_2}{gt}\\
g^2t^2 &=v_1\times v_2\\
\therefore t &= \frac{\sqrt{v_1v_2}}{g} \qquad since \; t>0 \\ \end{align*}

$$

the rest is as same as sbhatnagar's
 

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Thank You!:)
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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