Answer
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Hint: Use the formula for the time of ascent of the projectile.
Also, use the kinematic equation relating initial velocity, final velocity, acceleration and time.
Formula used:
The time of ascent of the projectile is given by
\[t = \dfrac{{u\sin \theta }}{g}\] …… (1)
Here, \[t\] is the time of ascent of the projectile, \[u\] is the speed of projection, \[\theta \] is the angle
of projection and \[g\] is the acceleration due to gravity.
The kinematic equation relating the final vertical velocity \[{v_y}\], initial vertical velocity \[{u_y}\], acceleration \[g\] and time \[t\] of a particle in projectile motion is
\[{v_y} = {u_y} - gt\] …… (2)
The angle of projection \[\theta \] of the projectile is given by
\[\theta = {\tan ^{ - 1}}\left( {\dfrac{{{v_y}}}{{{v_x}}}} \right)\] …… (3)
Here, \[{v_x}\] and \[{v_y}\] are the horizontal and vertical components of velocity of the projectile at any time \[t\].
Complete step by step answer:
The particle projected in the air starts its projectile motion one second after the launch at an angle of projection \[45^\circ \] and attains the minimum speed two seconds after the projection.
The diagram representing the projectile motion of the particle is as follows:
In the above figure, \[\theta \] is the angle of projection, \[u\] is the speed of projection and \[{v_x}\] and \[{v_y}\] are the horizontal and vertical components of velocity at any time.
The particle has a minimum velocity after two seconds of the projection. The projectile has the minimum speed at the maximum height as the vertical speed of the projectile becomes zero at maximum height.
The time taken by the particle to reach the maximum height is known as time of ascent.
The velocity of the particle becomes minimum i.e. zero after two seconds of projection.
Hence, the time of ascent of the particle is two seconds.
Substitute \[2\,{\text{s}}\] for \[t\] in equation (1).
\[2\,{\text{s}} = \dfrac{{u\sin \theta }}{g}\]
\[ \Rightarrow u\sin \theta = 2g\]
The horizontal and vertical components of the initial velocity of the projectile are \[u\cos \theta \] and \[u\sin \theta \].
\[{u_x} = u\cos \theta \]
\[{u_y} = u\sin \theta \]
The horizontal component of the speed \[{v_x}\] of projectile remains the same throughout the projectile motion.
\[{v_x} = u\cos \theta \]
Calculate the vertical component of the velocity of the projectile at any time.
Substitute \[u\sin \theta \] for \[{u_y}\] in equation (2).
\[{v_y} = u\sin \theta - gt\]
Calculate the vertical component of velocity \[{v_y}\] at time one second after the projection.
Substitute \[2g\] for \[u\sin \theta \] and \[1\,{\text{s}}\] for \[t\] in the above equation.
\[{v_y} = 2g - g\left( {1\,{\text{s}}} \right)\]
\[ \Rightarrow {v_y} = g\]
Rewrite the equation for the angle of projection of the projectile one second after its projection.
Substitute \[45^\circ \] for \[\theta \], \[u\cos \theta \] for \[{v_x}\] and \[g\] for \[{v_y}\] in equation (3).
\[45^\circ = {\tan ^{ - 1}}\left( {\dfrac{g}{{u\cos \theta }}} \right)\]
\[ \Rightarrow \tan 45^\circ = \dfrac{g}{{u\cos \theta }}\]
\[ \Rightarrow u\cos \theta = g\]
Now calculate the angle of projection of the projectile.
Substitute \[u\sin \theta \] for \[{v_y}\] and \[u\cos \theta \] for \[{v_x}\] in equation (3).
\[\theta = {\tan ^{ - 1}}\left( {\dfrac{{u\sin \theta }}{{u\cos \theta }}} \right)\
Substitute \[2g\] for \[u\sin \theta \] and \[g\] for \[u\cos \theta \] in the above equation.
\[\theta = {\tan ^{ - 1}}\left( {\dfrac{{2g}}{g}} \right)\]
\[ \Rightarrow \theta = {\tan ^{ - 1}}\left( 2 \right)\]
Therefore, the angle of projection of the particle is \[{\tan ^{ - 1}}\left( 2 \right)\].
So, the correct answer is “Option B”.
Note:
\[u\sin \theta \] and \[u\cos \theta \] are the vertical and horizontal components of only initial velocity of projection. For the rest of the projectile motion, the vertical component of the velocity of the projectile changes continuously and the horizontal component remains the same. The projectile motion of the particle in the present example starts after the one second of projection.
Also, use the kinematic equation relating initial velocity, final velocity, acceleration and time.
Formula used:
The time of ascent of the projectile is given by
\[t = \dfrac{{u\sin \theta }}{g}\] …… (1)
Here, \[t\] is the time of ascent of the projectile, \[u\] is the speed of projection, \[\theta \] is the angle
of projection and \[g\] is the acceleration due to gravity.
The kinematic equation relating the final vertical velocity \[{v_y}\], initial vertical velocity \[{u_y}\], acceleration \[g\] and time \[t\] of a particle in projectile motion is
\[{v_y} = {u_y} - gt\] …… (2)
The angle of projection \[\theta \] of the projectile is given by
\[\theta = {\tan ^{ - 1}}\left( {\dfrac{{{v_y}}}{{{v_x}}}} \right)\] …… (3)
Here, \[{v_x}\] and \[{v_y}\] are the horizontal and vertical components of velocity of the projectile at any time \[t\].
Complete step by step answer:
The particle projected in the air starts its projectile motion one second after the launch at an angle of projection \[45^\circ \] and attains the minimum speed two seconds after the projection.
The diagram representing the projectile motion of the particle is as follows:
In the above figure, \[\theta \] is the angle of projection, \[u\] is the speed of projection and \[{v_x}\] and \[{v_y}\] are the horizontal and vertical components of velocity at any time.
The particle has a minimum velocity after two seconds of the projection. The projectile has the minimum speed at the maximum height as the vertical speed of the projectile becomes zero at maximum height.
The time taken by the particle to reach the maximum height is known as time of ascent.
The velocity of the particle becomes minimum i.e. zero after two seconds of projection.
Hence, the time of ascent of the particle is two seconds.
Substitute \[2\,{\text{s}}\] for \[t\] in equation (1).
\[2\,{\text{s}} = \dfrac{{u\sin \theta }}{g}\]
\[ \Rightarrow u\sin \theta = 2g\]
The horizontal and vertical components of the initial velocity of the projectile are \[u\cos \theta \] and \[u\sin \theta \].
\[{u_x} = u\cos \theta \]
\[{u_y} = u\sin \theta \]
The horizontal component of the speed \[{v_x}\] of projectile remains the same throughout the projectile motion.
\[{v_x} = u\cos \theta \]
Calculate the vertical component of the velocity of the projectile at any time.
Substitute \[u\sin \theta \] for \[{u_y}\] in equation (2).
\[{v_y} = u\sin \theta - gt\]
Calculate the vertical component of velocity \[{v_y}\] at time one second after the projection.
Substitute \[2g\] for \[u\sin \theta \] and \[1\,{\text{s}}\] for \[t\] in the above equation.
\[{v_y} = 2g - g\left( {1\,{\text{s}}} \right)\]
\[ \Rightarrow {v_y} = g\]
Rewrite the equation for the angle of projection of the projectile one second after its projection.
Substitute \[45^\circ \] for \[\theta \], \[u\cos \theta \] for \[{v_x}\] and \[g\] for \[{v_y}\] in equation (3).
\[45^\circ = {\tan ^{ - 1}}\left( {\dfrac{g}{{u\cos \theta }}} \right)\]
\[ \Rightarrow \tan 45^\circ = \dfrac{g}{{u\cos \theta }}\]
\[ \Rightarrow u\cos \theta = g\]
Now calculate the angle of projection of the projectile.
Substitute \[u\sin \theta \] for \[{v_y}\] and \[u\cos \theta \] for \[{v_x}\] in equation (3).
\[\theta = {\tan ^{ - 1}}\left( {\dfrac{{u\sin \theta }}{{u\cos \theta }}} \right)\
Substitute \[2g\] for \[u\sin \theta \] and \[g\] for \[u\cos \theta \] in the above equation.
\[\theta = {\tan ^{ - 1}}\left( {\dfrac{{2g}}{g}} \right)\]
\[ \Rightarrow \theta = {\tan ^{ - 1}}\left( 2 \right)\]
Therefore, the angle of projection of the particle is \[{\tan ^{ - 1}}\left( 2 \right)\].
So, the correct answer is “Option B”.
Note:
\[u\sin \theta \] and \[u\cos \theta \] are the vertical and horizontal components of only initial velocity of projection. For the rest of the projectile motion, the vertical component of the velocity of the projectile changes continuously and the horizontal component remains the same. The projectile motion of the particle in the present example starts after the one second of projection.
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