What is Dipole: Definition and 853 Discussions

In electromagnetism, there are two kinds of dipoles:

An electric dipole deals with the separation of the positive and negative charges found in any electromagnetic system. A simple example of this system is a pair of electric charges of equal magnitude but opposite sign separated by some typically small distance. (A permanent electric dipole is called an electret.)
A magnetic dipole is the closed circulation of an electric current system. A simple example is a single loop of wire with constant current through it. A bar magnet is an example of a magnet with a permanent magnetic dipole moment.Dipoles, whether electric or magnetic, can be characterized by their dipole moment, a vector quantity. For the simple electric dipole, the electric dipole moment points from the negative charge towards the positive charge, and has a magnitude equal to the strength of each charge times the separation between the charges. (To be precise: for the definition of the dipole moment, one should always consider the "dipole limit", where, for example, the distance of the generating charges should converge to 0 while simultaneously, the charge strength should diverge to infinity in such a way that the product remains a positive constant.)
For the magnetic (dipole) current loop, the magnetic dipole moment points through the loop (according to the right hand grip rule), with a magnitude equal to the current in the loop times the area of the loop.
Similar to magnetic current loops, the electron particle and some other fundamental particles have magnetic dipole moments, as an electron generates a magnetic field identical to that generated by a very small current loop. However, an electron's magnetic dipole moment is not due to a current loop, but to an intrinsic property of the electron. The electron may also have an electric dipole moment though such has yet to be observed (see electron electric dipole moment).

A permanent magnet, such as a bar magnet, owes its magnetism to the intrinsic magnetic dipole moment of the electron. The two ends of a bar magnet are referred to as poles—not to be confused with monopoles, see Classification below)—and may be labeled "north" and "south". In terms of the Earth's magnetic field, they are respectively "north-seeking" and "south-seeking" poles: if the magnet were freely suspended in the Earth's magnetic field, the north-seeking pole would point towards the north and the south-seeking pole would point towards the south. The dipole moment of the bar magnet points from its magnetic south to its magnetic north pole. In a magnetic compass, the north pole of a bar magnet points north. However, that means that Earth's geomagnetic north pole is the south pole (south-seeking pole) of its dipole moment and vice versa.
The only known mechanisms for the creation of magnetic dipoles are by current loops or quantum-mechanical spin since the existence of magnetic monopoles has never been experimentally demonstrated.
The term comes from the Greek δίς (dis), "twice" and πόλος (polos), "axis".

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  1. S

    How Do You Calculate the Electric Field of a Dipole at a Specific Point?

    Homework Statement A dipole consists of two charges +q and -q, held apart by a rod of length s, as shown in the diagram. If q = 4 nC and s = 2 mm, what is the magnitude of the electric field due to the dipole at location A, a distance d = 5 cm from the dipole? The diagram shows point A...
  2. C

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    There is a two part problem that I'm struggling with. 1) A dipole with a moment of 2.5 nC . m is oriented 33 degrees from a field with strength 3.6 MN/C. What is the magnitude of the torque on the dipole? ____ mN . m I know the equation T = qd x E sin (theta) where qd is the given dipole...
  3. A

    Electric Dipole in Simple Harmonic Motion

    Homework Statement An electric dipole in a uniform horizontal electric field is displaced slightly from its equilibrium position, where theta is small. The separation of the charges is 2a, and each of the two particles has mass m. Assuming the dipole is released from this position, show that...
  4. L

    Dipole Moments Problem HELP

    Homework Statement A molecule of water has a dipole moment of 6.1×10–30 C m. Calculate the difference in potential energy between when its dipole is parallel to an electric field of 2.0×105 V m–1 and when it is anti-parallel to the field. Homework Equations U=kq1q2/r V=U/q V=Ex...
  5. R

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    Homework Statement Can't get to the final equality ( integral = - 4*Pi/3). Homework Equations \int_V \mathbf{E }dV = - \int_F \frac{_{\mathbf{p}.\mathbf{e_{r}}}}{r^2}\mathbf{e_{r}}r^{2}d\Omega = \mathbf{p}\frac{-4\pi }{3} The Attempt at a Solution Can't find how to get -4Pi/3...
  6. Y

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  7. Y

    Potential Energy of an Electric Dipole

    I understand that potential energy of an electric dipole is U(θ)=-pEcosθ where p is the dipole moment, E is the electric field and θ is the angle between vector p vector E. However i have some doubts about its derivation. in my readings, the work done is derived as such: dw=t*d(theta) =...
  8. Z

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  9. D

    Finding Zero Magnetic Field for a Magnetic Dipole

    Homework Statement A magnetic dipole m = -m0^z is situated at the origin, in an otherwise uniform magnetic eld B = B0^z. Show that there exists a spherical surface, centered at the origin, through which no magnetic eld lines pass. Find the radius of this sphere, and sketch the eld lines...
  10. C

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    Homework Statement Point electric dipole \vec{p}=p_0 \hat{z} is a distance d above an infinite metal plane of surface normal \hat{n}=\hat{z}. What is the force on the dipole. Is the dipole attracted to, or repelled from the surface?Homework Equations V(r) = \frac{\hat{n} \cdot \hat{p}}{4 \pi...
  11. G

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    Homework Statement I have been given the problem of finding the potential of a dipole in cylindrical coordinates. The only way that comes to my mind is to extract the dipole term from the multipole expansion of the potential of an arbitrary charge distribution in cylindrical coordinates. But I...
  12. M

    Exploring Binomial Expansion in Electric Dipole Fields

    I'm learning the subject of electric fields from Resnick and Halliday's book, and they have an equation for the field of the dipole: E = \frac{1}{4\pi\epsilon_0}\frac{p}{x^3} \left[1+\left(\frac{d}{2x}\right)^2\right]^{-3/2} Their next step is to find out what happens when x is larger than...
  13. E

    Point dipole embedded in dielectric sphere

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  14. TrickyDicky

    What is the velocity and direction of the CMB dipole?

    Does anyone know how is the direction of motion from the CMB dipole determined? Do Earth's motion around the sun affect the direction and magnitude of the velocity as seen on observations made over many months?
  15. M

    Potential of Dipole I think I am close to completing it

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  16. D

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    Homework Statement Consider a magnet floating over a large piece of superconductor. Treat the magnet as a perfect dipole m floating a distance h from the surface of the superconductor, which we take to be the x–y plane. The dipole is oriented at an angle of θ to the z-axis, and without loss...
  17. A

    Converting the Electric Field of a Dipole from Cartesian to Spherical Coords

    Homework Statement Show that E_z = \frac{p}{4 \pi \epsilon_0} \left( \frac{3z^2}{r^5} - \frac{1}{r^3} \right) is equivalent to the electric field on the positive z-axis from E_r = \frac{2 p \cos \theta}{4 \pi \epsilon_0 r^3} Homework Equations The unit normal for a sphere, sin0cos%...
  18. L

    How is our speed (~605km/s) derived from the CMB dipole anisotropy?

    Hi. How does the number 605km/s come from the observed CMB wavelength of 1.9mm? (http://en.wikipedia.org/wiki/Cosmic_microwave_background_radiation) Please only reply in 'English' and not a bunch of calculations because Google already provides lots of calculations. I am trying to get a...
  19. C

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  20. G

    Torque of electrical dipole moment

    Homework Statement Calculate each torque of a dipole rotating at 30 degree increments for 180 degrees. Dipole: s=.55 cm q=+/- 3.7nC Distance from point charge to axis of dipole = 14.3 cm point charge = +4.5 nC So there should be 8 phases and 7 torques (number 4 doesn't have a torque...
  21. S

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  22. T

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    Hi,can anyone tell me how to calculute magnitude and direction of the electric dipole moment of a system? If the system is a bit complicated? What kind of formula I suppose to use? \vec{p}=q\vec{d}?
  23. T

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  24. B

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  25. D

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  26. C

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  27. P

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  28. D

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    Homework Statement Show that E = \frac {q}{4\pi\varepsilon(z-\frac{1}{2}d)^2} - \frac{q}{4\pi\varepsilon(z+\frac{1}{2}d)^2} is E = \frac {q}{4\pi\varepsilon z^2} [(1-\frac{d}{2z})^{-2} - (1+\frac{d}{2z})^{-2}] Homework Equations The Attempt at a Solution After...
  29. G

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  30. K

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  31. P

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  32. L

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  33. V

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  34. V

    Electric Dipole Flux at Center of Sphere: Answer & Explanation

    Homework Statement an electrical dipole is placed at the centre of the sphere,the electric flux due to dipole is? i know the answer is zero but i don't find my reasons satisfactory pls post reply (i thought if the flux are normal to the centre the cos90 is zero hence zero) pls pls...
  35. N

    About the electric field of a dipole

    I would like to know that 1) Is there a point where the electric field is zero from a dipole? 2) If the point is very far away from a dipole, how is the electric from the dipole? I mean, for example, if there is a charge...
  36. G

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  37. D

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  38. M

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  39. D

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  40. S

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  41. M

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  42. M

    Electric field halfway between dipole isn't 0?

    I was just wondering... say you have a dipole, and you wanted to find the net electric field right in the middle. The electric field from the electron will be: E = k(-1.60*10^-19)/r^2 The electric field from the proton will be the same magnitude, but opposite direction...
  43. M

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    I know that the potential at any point P is the sum of the two potentials of a dipole. But we make two assumptions to get an equation: 1 - the distance from the dipole to P is very large relative to the dipole distance (d) 2 - we also make the assumption that r2 - r1 = dcosθ r2 and r1 is...
  44. P

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  45. C

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  46. V

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  47. A

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  48. I

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