Find the components along the $x, y, z$ axes of the angular momentum $l$ of a particle. whose position vector is $r$ with components $x, y, z$ and momentum is $p$ with components $p_{ r }, p_{ y }$ and $p_{z} .$ Show that if the particle moves only in the $x -y$ plane the angular momentum has only a $z-$component.
$l_{ x }=y p_{ z }-z p_{ y } l_{ y }$
$=z p_{ x }- x p_{ z } l_{ z }$
$=x p_{y}-y p_{x}$
Linear momentum of the particle, $\vec{p}=p_{ x } \hat{ i }+p_{y} \hat{ j }+p_{2} \hat{ k }$
Position vector of the particle, $\vec{r}=x \hat{ i }+y \hat{ j }+z \hat{ k }$
Angular momentum, $\vec{l}=\vec{r} \times \vec{p}$
$=(x \hat{ i }+y \hat{ j }+z \hat{ k }) \times\left(p_{x} \hat{ i }+p_{y} \hat{ j }+p_{z} \hat{ k }\right)$
$=\left|\begin{array}{ccc}\hat{ i } & \hat{ j } & \hat{ k } \\ x & y & z \\ p_{x} & p_{y} & p_{z}\end{array}\right|$
$l_{ x } \hat{ i }+l_{ y } \hat{ j }+l_{ z } \hat{ k }$$=\hat{ i }\left(y p_{z}-z p_{ y }\right)-\hat{ j }\left(x p_{z}-z p_{ x }\right)+\hat{ k }\left(x p_{y}-z p_{ x }\right)$
Comparing the coefficients of $\hat{ i }, \hat{ j },$ and $\hat{ k },$ we get:
$\left.\begin{array}{l}l_{ x }=y p_{ z }-z p_{ y } \\ l_{ y }=x p_{ z }-z p_{ x } \\ l_{z}=x p_{y}-y p_{ x }\end{array}\right\}$ $\dots(i)$
The particle moves in the $x$ $-y$ plane. Hence, the $z$ -component of the position vector
and linear momentum vector becomes zero, i.e., $z=p_{z}=0$
Thus, equation ( $i$ ) reduces to:
$l_{x}=0$
$l_{y}=0$
$l_{z}=x p_{y}-y p_{x}$
Therefore, when the particle is confined to move in the $x-y$ plane, the direction of angular momentum is along the $z$ -direction.
A particle of mass $m$ is moving along the side of a square of side '$a$', with a uniform speed $v$ in the $x-y$ plane as shown in the figure
Which of the following statement is false for the angular momentum $\vec L$ about the origin ?
A particle of mass $m$ moves along line $PC$ with velocity $v$ as shown. What is the angular momentum of the particle about $O$
A particle of mass $20\,g$ is released with an initial velocity $5\,m/s$ along the curve from the point $A,$ as shown in the figure. The point $A$ is at height $h$ from point $B.$ The particle slides along the frictionless surface. When the particle reaches point $B,$ its angular momentum about $O$ will be ......... $kg - m^2/s$. [Take $g = 10\,m/s^2$ ]
Two thin circular discs of mass $m$ and $4 m$, having radii of $a$ and $2 a$, respectively, are rigidly fixed by a massless, rigid rod of length $l=\sqrt{24} a$ through their centers. This assembly is laid on a firm and flat surface, and set rolling without slipping on the surface so that the angular speed about the axis of the rod is $\omega$. The angular momentum of the entire assembly about the point ' $O$ ' is $\vec{L}$ (see the figure). Which of the following statement($s$) is(are) true?
($A$) The center of mass of the assembly rotates about the $z$-axis with an angular speed of $\omega / 5$
($B$) The magnitude of angular momentum of center of mass of the assembly about the point $O$ is $81 m a^2 \omega$
($C$) The magnitude of angular momentum of the assembly about its center of mass is $17 \mathrm{ma}^2 \mathrm{\omega} / 2$
($D$) The magnitude of the $z$-component of $\vec{L}$ is $55 \mathrm{ma}^2 \omega$
A particle of mass $1 kg$ is subjected to a force which depends on the position as $\vec{F}=-k(x \hat{i}+y \hat{j}) kgms ^{-2}$ with $k=1 kgs ^{-2}$. At time $t=0$, the particle's position $\vec{r}=\left(\frac{1}{\sqrt{2}} \hat{i}+\sqrt{2} \hat{j}\right) m$ and its velocity $\vec{v}=\left(-\sqrt{2} \hat{i}+\sqrt{2} \hat{j}+\frac{2}{\pi} \hat{k}\right) m s^{-1}$. Let $v_x$ and $v_y$ denote the $x$ and the $y$ components of the particle's velocity, respectively. Ignore gravity. When $z=0.5 m$, the value of $\left(x v_y-y v_x\right)$ is. . . . . $m^2 s^{-1}$