Rod $R_1$ has rest length 1 m and rod $R_2$ has rest length 2 m. $R_1$ and $R_2$ move with velocities $+v\hat{i}$ and $-v\hat{i}$ respectively relative to the lab. If $R_2$ has a length of 1 m in the rest frame of $R_1$, $\frac{v}{c}$ is ................... (Specify answer up to two digits after decimal.)
Step 1: Use Lorentz contraction.
Length in $R_1$ frame: $L = L_0\sqrt{1 - u^2/c^2}$ where $u$ is relative velocity between the rods.
Given: $L = 1$ m, $L_0 = 2$ m.
Step 2: Solve for relative velocity $u$.
$1 = 2\sqrt{1 - u^2/c^2}$
$\sqrt{1 - u^2/c^2} = 1/2$
$1 - u^2/c^2 = 1/4$
$u^2/c^2 = 3/4$
$u/c = \sqrt{3}/2 = 0.866$.
Step 3: Relate $u$ to $v$.
Using relativistic velocity addition:
$u = \frac{v + v}{1 + v^2/c^2} = \frac{2v}{1 + v^2/c^2}$.
Step 4: Solve for $v/c$.
$\frac{2(v/c)}{1 + (v/c)^2} = 0.866$.
Solving gives $v/c = 0.75$.

At a particular temperature T, Planck's energy density of black body radiation in terms of frequency is \(\rho_T(\nu) = 8 \times 10^{-18} \text{ J/m}^3 \text{ Hz}^{-1}\) at \(\nu = 3 \times 10^{14}\) Hz. Then Planck's energy density \(\rho_T(\lambda)\) at the corresponding wavelength (\(\lambda\)) has the value \rule{1cm}{0.15mm} \(\times 10^2 \text{ J/m}^4\). (in integer)
[Speed of light \(c = 3 \times 10^8\) m/s]
(Note: The unit for \(\rho_T(\nu)\) in the original problem was given as J/m³, which is dimensionally incorrect for a spectral density. The correct unit J/(m³·Hz) or J·s/m³ is used here for the solution.)
