To find the wavelength of the waves transmitted by the broadcasting station, we use the fundamental wave equation that relates speed, frequency, and wavelength.
The relationship between the speed of a wave ($v$), its frequency ($f$), and its wavelength ($\lambda$) is given by the formula:
$ v = f \lambda $
We need to rearrange the formula to solve for the wavelength ($\lambda$):
$ \lambda = \frac{v}{f} $
$ \lambda = \frac{3 \times 10^8\ m/s}{71 \times 10^4\ Hz} $
$ \lambda = \frac{3}{71} \times \frac{10^8}{10^4}\ m $
$ \lambda = \frac{3}{71} \times 10^{(8-4)}\ m $
$ \lambda = \frac{3}{71} \times 10^4\ m $
$ \lambda \approx 0.0422535 \times 10^4\ m $
$ \lambda \approx 422.535\ m $
$ \lambda \approx 422.5\ m $
The calculated wavelength of the wave is approximately $422.5\ m$. This corresponds to Option C.
Which of the following is related to Doppler effect?
The position of a particle in one dimension changes in discrete steps. With each step it moves to the right, however, the length of the step is drawn from a uniform distribution from the interval \(\left[ {{\rm{λ }}\,{\rm{ - }}\,\frac{{\rm{1}}}{{\rm{2}}}{\rm{w,}}\,{\rm{λ }}\,{\rm{ + }}\,\frac{{\rm{1}}}{{\rm{2}}}{\rm{w}}} \right] \) , where λ and w are positive constants. If X denotes the distance from the starting point after N steps, the standard deviation \(\sqrt {\left\langle {{X^2}} \right\rangle \, - {{\left\langle X \right\rangle }^2}} \) for large values of N is
A particle of mass m in one dimension is in the ground state of a simple harmonic oscillator described by a Hamiltonian \(\frac{{{{\rm{P}}^{\rm{2}}}}}{{{\rm{2m}}}}{\rm{ + }}\frac{{\rm{1}}}{{\rm{2}}}{\rm{m}}{{\rm{\omega }}^{\rm{2}}}{{\rm{x}}^{\rm{2}}} \) in the standard notation. An impulsive force at time t = 0 suddenly imparts a momentum P0 = \(\sqrt {{\rm{hm\omega }}} \) to it. The probability that the particle remains in the original ground state is
In an elastic scattering process at an energy E, the phase shifts satisfy δ 0 ≈ 30°, δ 1≈ 10°, while the other phase shifts are zero. The polar angle at which the differential cross-section peaks is closest to