Two particles are simultaneously projected in the horizontal direction from a point P at a certain height. The initial velocities of the particles are oppositely directed to each other and have magnitude v each. The separation between the particles at a time when their position vectors (drawn from the point P) are mutually perpendicular, is
A. $\dfrac{{{v^2}}}{{2g}}$
B. $\dfrac{{{v^2}}}{g}$
C. $\dfrac{{4{v^2}}}{g}$
D. $\dfrac{{2{v^2}}}{g}$
Answer
624k+ views
Hint: When two vectors are $\overrightarrow A $and $\overrightarrow B $are perpendicular to each other then, $\overrightarrow A \,.\,\overrightarrow B = 0$. The rate at which the two particles separate is known as velocity of separation.
Complete step by step solution:
Let two particles named (1) and (2) respectively, are projected direction from point P with same velocity v but opposite in direction. Let after time `t’ the position vector of particle (1) and (2) are perpendicular with respect to point `P’ then the horizontal velocity tends to separate them and gravity moves in downward direction. So the position vector of particle (i) is given by,
$\overrightarrow {{r_1}} = {\overrightarrow r _{x1}} + {\overrightarrow r _{y1}}$
Where ${\overrightarrow r _{x1}}$ is displacement covered by particle $1$in horizontal/$x$ direction and ${\overrightarrow r _{y1}}$ is displacement covered by particle $1$ in vertical/$y$ direction.
$\overrightarrow {{r_1}} = vt\left( { - \widehat i} \right) + \left( {0 \times t + \dfrac{1}{2}g{t^2}} \right)\left( { - \widehat j} \right)$
$\overrightarrow {{r_1}} = - vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j......\left( i \right)$
Now the position vector of second particle is given by,
$\overrightarrow {{r_2}} = {\overrightarrow r _{x2}} + {\overrightarrow r _{y2}}$
Where ${\overrightarrow r _{x2}} \to $displacement of particle $2$ in horizontal/$x$ direction and ${\overrightarrow r _{y2}} \to $ Displacement of particle $2$ in vertical/$y$ direction.
So, $\overrightarrow {{r_2}} = vt\left( { + \widehat i} \right) + \left( {0 + \dfrac{1}{2}g{t^2}} \right)\left( { - \widehat j} \right)$
$\overrightarrow {{r_2}} = vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j$
If \[{\overrightarrow r _1} + {\overrightarrow r _2}\] after time ‘t’ then\[{\overrightarrow r _1} - {\overrightarrow r _2} = 0\]
$ \Rightarrow \left( { - vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j} \right)\left( {vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j} \right) = 0$
$ \Rightarrow {\left( {vt} \right)^2} + {\left( {\dfrac{1}{2}g{t^2}} \right)^2} = 0$
$ \Rightarrow {\left( {\dfrac{1}{2}g{t^2}} \right)^2} = {\left( {vt} \right)^2}$taking underfoot of both sides,
$ \Rightarrow \sqrt {{{\left( {\dfrac{1}{2}g{t^2}} \right)}^2}} = \sqrt {{{\left( {vt} \right)}^2}} $
$ \Rightarrow \dfrac{1}{2}g{t^2} = vt$
$ \Rightarrow \dfrac{{gt}}{2} = v \Rightarrow t = \dfrac{{2v}}{g}$
Now the velocity of separation of the particle (1) and (2)
$ = v + v = 2v$ so the separation between the particles at a time when their position vectors (drawn from the point P) are mutually perpendicular, is
AB $ = $Velocity of separation $ \times $time
AB \[ = \left( {2v} \right) \times t = 2v \times \dfrac{{2v}}{g}\]
AB $ = \dfrac{{4{v^2}}}{g}$
Hence, option (C) is correct.
Additional Information: The velocity of separation or approach is a component of relative velocity of one particle with respect to another.
Note: In this question the horizontal velocity makes effort to move the horizontal direction and that of gravity in downward direction so the displacement into particles is due to both.
Complete step by step solution:
Let two particles named (1) and (2) respectively, are projected direction from point P with same velocity v but opposite in direction. Let after time `t’ the position vector of particle (1) and (2) are perpendicular with respect to point `P’ then the horizontal velocity tends to separate them and gravity moves in downward direction. So the position vector of particle (i) is given by,
$\overrightarrow {{r_1}} = {\overrightarrow r _{x1}} + {\overrightarrow r _{y1}}$
Where ${\overrightarrow r _{x1}}$ is displacement covered by particle $1$in horizontal/$x$ direction and ${\overrightarrow r _{y1}}$ is displacement covered by particle $1$ in vertical/$y$ direction.
$\overrightarrow {{r_1}} = vt\left( { - \widehat i} \right) + \left( {0 \times t + \dfrac{1}{2}g{t^2}} \right)\left( { - \widehat j} \right)$
$\overrightarrow {{r_1}} = - vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j......\left( i \right)$
Now the position vector of second particle is given by,
$\overrightarrow {{r_2}} = {\overrightarrow r _{x2}} + {\overrightarrow r _{y2}}$
Where ${\overrightarrow r _{x2}} \to $displacement of particle $2$ in horizontal/$x$ direction and ${\overrightarrow r _{y2}} \to $ Displacement of particle $2$ in vertical/$y$ direction.
So, $\overrightarrow {{r_2}} = vt\left( { + \widehat i} \right) + \left( {0 + \dfrac{1}{2}g{t^2}} \right)\left( { - \widehat j} \right)$
$\overrightarrow {{r_2}} = vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j$
If \[{\overrightarrow r _1} + {\overrightarrow r _2}\] after time ‘t’ then\[{\overrightarrow r _1} - {\overrightarrow r _2} = 0\]
$ \Rightarrow \left( { - vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j} \right)\left( {vt\widehat i - \dfrac{1}{2}g{t^2}\widehat j} \right) = 0$
$ \Rightarrow {\left( {vt} \right)^2} + {\left( {\dfrac{1}{2}g{t^2}} \right)^2} = 0$
$ \Rightarrow {\left( {\dfrac{1}{2}g{t^2}} \right)^2} = {\left( {vt} \right)^2}$taking underfoot of both sides,
$ \Rightarrow \sqrt {{{\left( {\dfrac{1}{2}g{t^2}} \right)}^2}} = \sqrt {{{\left( {vt} \right)}^2}} $
$ \Rightarrow \dfrac{1}{2}g{t^2} = vt$
$ \Rightarrow \dfrac{{gt}}{2} = v \Rightarrow t = \dfrac{{2v}}{g}$
Now the velocity of separation of the particle (1) and (2)
$ = v + v = 2v$ so the separation between the particles at a time when their position vectors (drawn from the point P) are mutually perpendicular, is
AB $ = $Velocity of separation $ \times $time
AB \[ = \left( {2v} \right) \times t = 2v \times \dfrac{{2v}}{g}\]
AB $ = \dfrac{{4{v^2}}}{g}$
Hence, option (C) is correct.
Additional Information: The velocity of separation or approach is a component of relative velocity of one particle with respect to another.
Note: In this question the horizontal velocity makes effort to move the horizontal direction and that of gravity in downward direction so the displacement into particles is due to both.
Recently Updated Pages
Master Class 12 Economics: Engaging Questions & Answers for Success

Master Class 12 English: Engaging Questions & Answers for Success

Master Class 12 Social Science: Engaging Questions & Answers for Success

Master Class 12 Maths: Engaging Questions & Answers for Success

Master Class 12 Physics: Engaging Questions & Answers for Success

Master Class 11 Social Science: Engaging Questions & Answers for Success

Trending doubts
One Metric ton is equal to kg A 10000 B 1000 C 100 class 11 physics CBSE

Difference Between Prokaryotic Cells and Eukaryotic Cells

Find the value of the expression given below sin 30circ class 11 maths CBSE

Two of the body parts which do not appear in MRI are class 11 biology CBSE

Draw a diagram of nephron and explain its structur class 11 biology CBSE

10 examples of friction in our daily life

