


Here is the equation of motion and time period for the given
system.
2R V Y r the (a) The angle axis the angular bo i polan its centre between the dipole and is (0+2) dipole about (6+2) of the velocity is of mass is of the dipole > 2 d. kinetic energy T = in the 1 (2m). (82 + 2 8 2) + 12. 2m R 2 m R² Corås mie + m (m2+ R²) 6 ² + m R² à ² + 2 mkoa placed electric field charge Q,, so potential dipole is ~ Since the dipole is of of the energy O, Q2 V ། 47 to LA Vita & cosa Vr²+R N r+R+ 28 R cosa + 22 + 2. 2 R cosa Nr 1 1. 2 ? cosa 2 r r = r I R cosa. 31- r. r+ R cosa r- Rcosa
하 SH 2 R cosa 2 – R² costa + 2 R cos of 72 and the potential energy is VE 2 2 R cosa 40 ton re -> is Lagrangian L = T - V m² + m (r² + R²) 0 ² + m R² 22 + 2 m Roa Q, Q2 2Rcosa 40€ 22 + 72 Lagrange's equation gives (8) - 2 = 0 d at 2 C (emr) - 2 mro + 28, Q2 2Rcosa = 0. 4Xto 73 mi 2 R cosa + 2 mno2+Q, & 40€ (;) r3 Other one gives y #) - = 0; = 0 2m (22+R²) + 2m R² i +2mrros (می) - 2L IL and = 0 & CO gives dt aa Q,Q, sind mR (ätö ) + = 0 – (on) 40 to 82
are the equations of motion Equations (i), (i), (2) dipole. of the is a constant * * * 0. As 15$ (6) Also, = 0 <<1 (ie. sində a) from (ui) MR ä + Q, Q, 30, Anto 82 in a is motion the that This shows angular with a frequency simple harmonic Q,Q2 47€ MR82 is The period of such oscillation 2T 2T Anto mRr2 Q, Q2