Given: Particle of mass \(m=5\,\text{kg}\) moves along the line \(y=x+4\) with speed \(3\sqrt{2}\,\text{m s}^{-1}\).
1) Position and velocity.
Any point on the line: \((x,\,x+4)\Rightarrow \vec r=x\,\hat i+(x+4)\,\hat j.\)
Direction of motion is along the line; slope \(dy/dx=1\Rightarrow\) direction vector \(\hat i+\hat j\). Unit direction \(=\dfrac{1}{\sqrt2}(\hat i+\hat j)\). Given speed \(3\sqrt2\), the velocity is \[ \vec v=3\sqrt2\cdot \frac{1}{\sqrt2}(\hat i+\hat j)=3\hat i+3\hat j. \]
2) Angular momentum.
\[ \vec L=m(\vec r\times \vec v),\qquad \vec r\times \vec v= \begin{vmatrix} \hat i & \hat j & \hat k\\ x & x+4 & 0\\ 3 & 3 & 0 \end{vmatrix} = \big(3x-3(x+4)\big)\hat k=-12\,\hat k. \] Thus \[ \vec L=5(-12)\hat k=-60\,\hat k\ \text{kg m}^2\text{s}^{-1}. \] \[ |\vec L|=60\ \text{kg m}^2\text{s}^{-1}. \]

A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure. 
The angular velocity of the system after the particle sticks to it will be:
