The problem requires calculating the Lorentz contraction of a rod moving at $\frac{c}{2}$ m/s, where $c=3 \times 10^8$ m/s. The rod's proper length is 3 m, and its angle with the x-axis is 30°.
To calculate Lorentz contraction, use the formula for the length contraction:
$$ L = L_0\sqrt{1-\frac{v^2}{c^2}} $$
where \( L_0 \) is the proper length and \( v \) is the velocity.
First, find the component of the velocity along the rod's axis. Given the speed is \( \frac{c}{2} \) and the angle is 30°, only the parallel component affects contraction:
$$ v_{\parallel} = v\cos(30°) = \frac{c}{2}\cos(30°) = \frac{c\sqrt{3}}{4} $$
Plug this component into the length contraction formula:
$$ L = 3\sqrt{1-\left(\frac{(\frac{c\sqrt{3}}{4})^2}{c^2}\right)} = 3\sqrt{1-\frac{3c^2}{16c^2}} = 3\sqrt{1-\frac{3}{16}} $$
Simplifying further:
$$ 3\sqrt{\frac{16-3}{16}} = 3\sqrt{\frac{13}{16}} = 3 \times \frac{\sqrt{13}}{4} $$
Calculating \( \frac{\sqrt{13}}{4} \approx 0.901 \):
Thus, contracted length \( L \) is:
$$ 3 \times 0.901 \approx 2.703 \ m $$
The change in length due to contraction: \( 3 - 2.703 = 0.297 \ m \).
In order to achieve the static equilibrium of the see-saw about the fulcrum \( P \), shown in the figure, the weight of Box B should be _________ kg, if the weight of Box A is 50 kg.

A particle of mass 1kg, initially at rest, starts sliding down from the top of a frictionless inclined plane of angle \(\frac{𝜋}{6}\)\(\frac{\pi}{6}\) (as schematically shown in the figure). The magnitude of the torque on the particle about the point O after a time 2seconds is ______N-m. (Rounded off to nearest integer) 
(Take g = 10m/s2)

