The de-Broglie wavelength \( \lambda \) is given by: \[ \lambda = \frac{h}{p} = \frac{h}{mv} \] Where: - \( h \) is Planck's constant, - \( p \) is the momentum, - \( m \) is the mass, - \( v \) is the velocity. For an electron and a proton moving with the same velocity \( v \): \[ \lambda_e = \frac{h}{m_e v} \] \[ \lambda_p = \frac{h}{m_p v} \] The ratio of the wavelengths is: \[ \frac{\lambda_e}{\lambda_p} = \frac{m_p}{m_e} \] Thus, the ratio of de-Broglie wavelengths for the electron and proton is \( m_p: m_e \).
Final Answer: \( m_p: m_e \)
In the given circuit, the electric currents through $15\, \Omega$ and $6 \, \Omega$ respectively are

Two bar magnets A and B are identical and arranged as shown. Their lengths are negligible compared to the separation between them. A magnetic needle placed between the magnets at point P gets deflected through an angle \( \theta \) under their influence. The ratio of distances \( d_1 \) and \( d_2 \) is:
