POTENTIAL DUE TO AN ELECTRIC DIPOLE Electric dipole An electric dipole consists of two equal and Cloze (1): JXUwMDM3JXUwMDFmJXUwMDAwJXUwMDFmJXUwMDFjJXUwMDFhJXUwMDFkJXUwMDEx charges separated by a (small) vector distance 2a Its total charge is Cloze (2): JXUwMDIyJXUwMDFmJXUwMDE3JXUwMDFk It is characterised by a dipole moment vector p whose magnitude is q × 2a and which points in the direction from Cloze (3): JXUwMDM2JXUwMDBiJXUwMDAyJXUwMDA2JXUwMDE1JXUwMDFkJXUwMDFmJXUwMDEz charge to Cloze (4): JXUwMDI4JXUwMDFmJXUwMDFjJXUwMDFhJXUwMDFkJXUwMDFkJXUwMDFmJXUwMDEz charge Enable JavaScript Electric field intensity has some Angle dependencies in addition to magnitude Potential due to Electric dipole Read and complete Electric potential is Cloze (1): positivenegativezero JXUwMDI4JXUwMDFmJXUwMDFjJXUwMDFhJXUwMDFkJXUwMDFkJXUwMDFmJXUwMDEz for θ = 0, Cloze (2): positivenegativezero JXUwMDM2JXUwMDBiJXUwMDAyJXUwMDA2JXUwMDE1JXUwMDFkJXUwMDFmJXUwMDEz for θ = π. The potential in the equatorial plane ( θ = π/2) is Cloze (3): positivenegativezero JXUwMDIyJXUwMDFmJXUwMDE3JXUwMDFk Enable JavaScript Single charge versus Dipole Read and complete The Cloze (1): electric dipolesingle chargeSystem of charge JXUwMDNkJXUwMDA5JXUwMDA5JXUwMDA2JXUwMDE3JXUwMDA2JXUwMDFiJXUwMDBhJXUwMDQzJXUwMDQ0JXUwMDBkJXUwMDE5JXUwMDFmJXUwMDAzJXUwMDA5 potential falls off, at large distance, obeying inverse square law , not as the characteristic of the potential due to a Cloze (2): electric dipolesingle chargeSystem of charge JXUwMDJiJXUwMDFhJXUwMDA3JXUwMDA5JXUwMDBiJXUwMDA5JXUwMDQ1JXUwMDQzJXUwMDBiJXUwMDA5JXUwMDEzJXUwMDE1JXUwMDAy which varies inversely with distance Enable JavaScript
Electric dipole An electric dipole consists of two equal and Cloze (1): JXUwMDM3JXUwMDFmJXUwMDAwJXUwMDFmJXUwMDFjJXUwMDFhJXUwMDFkJXUwMDEx charges separated by a (small) vector distance 2a Its total charge is Cloze (2): JXUwMDIyJXUwMDFmJXUwMDE3JXUwMDFk It is characterised by a dipole moment vector p whose magnitude is q × 2a and which points in the direction from Cloze (3): JXUwMDM2JXUwMDBiJXUwMDAyJXUwMDA2JXUwMDE1JXUwMDFkJXUwMDFmJXUwMDEz charge to Cloze (4): JXUwMDI4JXUwMDFmJXUwMDFjJXUwMDFhJXUwMDFkJXUwMDFkJXUwMDFmJXUwMDEz charge Enable JavaScript Electric field intensity has some Angle dependencies in addition to magnitude
Potential due to Electric dipole Read and complete Electric potential is Cloze (1): positivenegativezero JXUwMDI4JXUwMDFmJXUwMDFjJXUwMDFhJXUwMDFkJXUwMDFkJXUwMDFmJXUwMDEz for θ = 0, Cloze (2): positivenegativezero JXUwMDM2JXUwMDBiJXUwMDAyJXUwMDA2JXUwMDE1JXUwMDFkJXUwMDFmJXUwMDEz for θ = π. The potential in the equatorial plane ( θ = π/2) is Cloze (3): positivenegativezero JXUwMDIyJXUwMDFmJXUwMDE3JXUwMDFk Enable JavaScript
Single charge versus Dipole Read and complete The Cloze (1): electric dipolesingle chargeSystem of charge JXUwMDNkJXUwMDA5JXUwMDA5JXUwMDA2JXUwMDE3JXUwMDA2JXUwMDFiJXUwMDBhJXUwMDQzJXUwMDQ0JXUwMDBkJXUwMDE5JXUwMDFmJXUwMDAzJXUwMDA5 potential falls off, at large distance, obeying inverse square law , not as the characteristic of the potential due to a Cloze (2): electric dipolesingle chargeSystem of charge JXUwMDJiJXUwMDFhJXUwMDA3JXUwMDA5JXUwMDBiJXUwMDA5JXUwMDQ1JXUwMDQzJXUwMDBiJXUwMDA5JXUwMDEzJXUwMDE1JXUwMDAy which varies inversely with distance Enable JavaScript