A particle of mass m is projected with a velocity u making an angle ${45^ \circ }$ with the horizontal from level ground. When the particle lands on the level ground the magnitude of the change in momentum will be:
A. $mu\sqrt 2 $
B. zero
C. $2mu$
D. $\dfrac{{mu}}{{\sqrt 2 }}$
Answer
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Hint: In this question,we are going to apply the concept of momentum and it is defined as the product of mass and velocity of a particle in motion. It is denoted by using letter p and its SI unit is $kgm{s^{ - 2}}$. It is a vector quantity (it has both magnitude and direction).
Complete step by step answer:
The particle’s initial vertical velocity is $u\sin 45 = \dfrac{u}{{\sqrt 2 }}$. Since the particle is coming back to its initial position (i.e. to the level ground) we can say that its final vertical velocity is also $\dfrac{u}{{\sqrt 2 }}$. But the final vertical velocity will be in a direction opposite to that of the initial vertical velocity.
The initial vertical velocity is $ + \dfrac{u}{{\sqrt 2 }}m{s^{ - 1}}$ whereas the final vertical velocity will be $ - \dfrac{u}{{\sqrt 2 }}m{s^{ - 1}}$.
Since this is a projectile motion, the horizontal component of the velocity remains constant.
Total change in momentum is the sum of change in momentum along the x and y axis.
$
\Delta p = \Delta {p_x} + \Delta {p_y} \\
\Rightarrow \Delta {p_y} = m\left( { + \dfrac{u}{{\sqrt 2 }}} \right) - m\left( { - \dfrac{u}{{\sqrt 2 }}} \right) \\
\Rightarrow \Delta {p_y} = 2m\left( {\dfrac{u}{{\sqrt 2 }}} \right) \\
\Rightarrow \Delta {p_y} = \sqrt 2 mu \\
\Delta {p_x} = m{u_x} - m{u_x} = 0 \\
\Rightarrow \Delta p = \Delta {p_x} + \Delta {p_y} \\
\Rightarrow \Delta p = 0 + \sqrt 2 mu \\
\therefore \Delta p = mu\sqrt 2 \\
$
Hence the net change in momentum in this case is $mu\sqrt 2 $.
Therefore the correct choice is option (A).
Note: Here we say that the horizontal velocity remains the same by ignoring the drag forces. If we consider the drag forces, then the horizontal velocity will vary and so will the horizontal momentum.
Complete step by step answer:
The particle’s initial vertical velocity is $u\sin 45 = \dfrac{u}{{\sqrt 2 }}$. Since the particle is coming back to its initial position (i.e. to the level ground) we can say that its final vertical velocity is also $\dfrac{u}{{\sqrt 2 }}$. But the final vertical velocity will be in a direction opposite to that of the initial vertical velocity.
The initial vertical velocity is $ + \dfrac{u}{{\sqrt 2 }}m{s^{ - 1}}$ whereas the final vertical velocity will be $ - \dfrac{u}{{\sqrt 2 }}m{s^{ - 1}}$.
Since this is a projectile motion, the horizontal component of the velocity remains constant.
Total change in momentum is the sum of change in momentum along the x and y axis.
$
\Delta p = \Delta {p_x} + \Delta {p_y} \\
\Rightarrow \Delta {p_y} = m\left( { + \dfrac{u}{{\sqrt 2 }}} \right) - m\left( { - \dfrac{u}{{\sqrt 2 }}} \right) \\
\Rightarrow \Delta {p_y} = 2m\left( {\dfrac{u}{{\sqrt 2 }}} \right) \\
\Rightarrow \Delta {p_y} = \sqrt 2 mu \\
\Delta {p_x} = m{u_x} - m{u_x} = 0 \\
\Rightarrow \Delta p = \Delta {p_x} + \Delta {p_y} \\
\Rightarrow \Delta p = 0 + \sqrt 2 mu \\
\therefore \Delta p = mu\sqrt 2 \\
$
Hence the net change in momentum in this case is $mu\sqrt 2 $.
Therefore the correct choice is option (A).
Note: Here we say that the horizontal velocity remains the same by ignoring the drag forces. If we consider the drag forces, then the horizontal velocity will vary and so will the horizontal momentum.
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