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Systems of Particles and Rotational Motion

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Question : 6 of 33
Marks: +1, -0
Find the components along the x, y, z axes of the angular momentum L⃗\vec{L} of a particle, whose position vector is r⃗\vec{r} with components x, y, z and momentum is p⃗\vec{p} with components px,py and pzp_x, p_y \text{ and } p_z. Show that if the particle moves only in the x-y plane the angular momentum has only a z-component.
Solution:  
(a) Angular momentum,
L⃗=r⃗×p⃗\vec{L} = \vec{r} \times \vec{p}
It is a vector quantity and its direction is given by right hand rule for vector product. As r⃗\vec{r} and p⃗\vec{p} here lie in xoy plane, so L⃗\vec{L} acts along Z axis.
In cartesian co-ordinates,
and r⃗=xi^+yj^+zk^p⃗=pxi^+pyj^+pzk^\begin{array}{l} \vec{r} = x \hat{i} + y \hat{j} + z \hat{k} \\ \vec{p} = p_x \hat{i} + p_y \hat{j} + p_z \hat{k} \end{array}...(ii)
∴ From (i) and (ii), we get
L⃗=(xi^+yj^+zk^)×(pxi^+pyj^+pzk^)\vec{L} = (x \hat{i} + y \hat{j} + z \hat{k}) \times (p_x \hat{i} + p_y \hat{j} + p_z \hat{k})
=∣i^j^k^xyzpxpypz∣= \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ x & y & z \\ p_x & p_y & p_z \end{vmatrix}
or Lxi^+Lyj^+Lzk^=i^(ypz−zpy)+j^(zpx−xpz)+k^(xpy−ypx)L_x \hat{i} + L_y \hat{j} + L_z \hat{k} = \hat{i}(y p_z - z p_y) + \hat{j}(z p_x - x p_z) + \hat{k}(x p_y - y p_x)
On comparing, we get
Lx=ypz−zpyLy=zpx−xpzLz=xpy−ypx...(iii)\begin{array}{l} L_x = y p_z - z p_y \\ L_y = z p_x - x p_z \\ L_z = x p_y - y p_x \end{array} \quad \text{...(iii)}
Equation (iii) gives the required components of LL along x,yx, y and zz axes.
(b) As the particle moves in x−yx-y plane, then
z=0z=0 and pz=0p_z = 0
Hence, L⃗=k^(xpy−ypx)=Lzk^\vec{L} = \hat{k} (x p_y - y p_x) = L_z \hat{k}
Hence angular momentum has only z-component.
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