Curly Electric Fields: Difference between revisions

Latest revision as of 11:41, 2 December 2015

Written by Miranda Fyfe

The Curly Electric Field is the non-Coulombic result of a changing current and time-varying magnetic field.

Definition

In the case where current in a solenoid is constant and magnetic force is likewise constant in time, it can be observed that the magnetic and electric forces experienced by some moving charge outside the solenoid are essentially zero.

However, in the situation where current in the solenoid is changing and magnetic force is thereby time-varying, a Curly Electric Field can be observed.

*The **curly electric field** curls around the axis of the solenoid*

*Outside of the solenoid, magnetic field is still virtually zero, but the curly electric field can be observed both inside and outside of the solenoid*

Proportionality

This electric field is proportional to the rate of change of the magnetic field [math]\displaystyle{ ( \frac{\delta B}{\delta t} ) }[/math].

Inside the solenoid

Curly electric field is proportional to distance from the solenoid axis, r.

Outside the solenoid

Curly electric field is proportional to 1/r, with the field decreasing as distance from the axis increases.

The Non-Coulomb Curly Electric Field

Read more about the Non-Coulomb Electric Field

Coulomb Electric Field

Any electric field in accordance with Coulomb's law is said to be a Coulomb electric field.

Coulomb's Law: [math]\displaystyle{ \vec{E} = \frac{1}{4{\pi}{{\epsilon}_0}} \frac{q}{r^2} \hat{r} }[/math]

Non-Coulomb Electric Field

An electric field associated with a time-varying magnetic field, i.e. the curly electric field.

Effect on charges

The curly electric field has a standard effect on charges [math]\displaystyle{ ( \vec{F} = q\vec{E} ) }[/math]

Because the curly electric field deals with non-stationary charges and the magnetic field and current are time-variant, the curly electric field is a Non-Coloumb Electric Field.

Direction of Curly Electric Field

Faraday's Experiment

In 1831, Michael Faraday conducted an experiment which proved magnetic fields could be produced by electric currents. The experiment involved connecting a battery to a large coiled wire, and measuring the effects with a voltmeter. Faraday recorded effects both upon first connecting the battery and when initially disconnecting it the later of which was found surprising.

Because an effect could only be gauged when the magnetic field was changing, it was concluded that this effect was proportional to [math]\displaystyle{ ( \frac{\delta B}{\delta t} ) }[/math]

Finding the Direction

Implementing this proportion takes the process a step further; a Right Hand Rule can be utilized to pinpoint the direction of the curly electric field as follows:

Point the thumb of the right hand in the direction of [math]\displaystyle{ ( - \frac{\delta B}{\delta t} ) }[/math] , and curl the fingers in the direction of the curly electric field.

*The right hand rule for finding the direction of curly electric field*

For each of the following four situations, the right hand rule can be used to determine direction of curly electric field.

Magnetic field out of the page and increasing [math]\displaystyle{ \rightarrow }[/math] Clockwise curly electric field
Magnetic field into the page and increasing [math]\displaystyle{ \rightarrow }[/math] Counterclockwise curly electric field
Magnetic field out of the page and decreasing [math]\displaystyle{ \rightarrow }[/math] Counterclockwise curly electric field
Magnetic field into the page and decreasing [math]\displaystyle{ \rightarrow }[/math] Clockwise curly electric field

Driving Current with Curly Electric Field

*The non-Coulombic curly electric field drives the current in the metal ring*

The non-Coulombic curly electric field has the potential to create an effect akin to that of a battery; if a circular metal ring is placed around a solenoid with increasing magnetic field over time (see image), the curly electric field in the solenoid will drive the current in the metal ring clockwise. Further, as in an ordinary circuit, the current in the ring will be proportional to the electric field.

emf in Non-Coulomb Field

The emf in a non-Coulomb field such as the curly electric field can be computed as the energy input per unit charge. Therefore the equation for emf in a non-Coulombic field is calculated thus:

[math]\displaystyle{ emf = \oint \vec{E}_{NC} \bullet {d}{\vec{l}} }[/math]

Outside Path

For any round-trip path that lies outside the solenoid--that is, it does not encircle the solenoid-- the emf is equal to zero. In the picture below, the path on the left does encircle the solenoid, and therefore has a nonzero emf. However, the rightmost path does not encircle the solenoid, and therefore that path has a zero emf value.

*When the solenoid is not encircled by the path, emf = 0*

External Links

References

Matter and Interactions, Vol. 2 by Chabay and Sherwood
http://physwiki.ucdavis.edu/Fundamentals/11._Electromagnetism/11.5_Induced_Electric_Fields
http://www.phy.uct.ac.za/courses/opencontent/phy1004w/1004W%20EM%2022.pdf

@@ Line 1: / Line 1: @@
-This topic is claimed by Miranda Fyfe.
+''Written by Miranda Fyfe''
-==Curly Electric Fields==
+The '''Curly Electric Field''' is the non-Coulombic result of a changing current and time-varying magnetic field.
+==Definition==
 In the case where current in a solenoid is constant and magnetic force is likewise constant in time, it can be observed that the magnetic and electric forces experienced by some moving charge outside the solenoid are essentially zero.
-However, in the situation where current in the solenoid is changing and magnetic force is thereby time-varying, a '''curly electric field''' can be observed.
+However, in the situation where current in the solenoid is changing and magnetic force is thereby time-varying, a '''Curly Electric Field''' can be observed.
 [[File:curlyefield2.png|275px|thumb|center|''The '''curly electric field''' curls around the axis of the solenoid'']]
@@ Line 15: / Line 17: @@
 ==Proportionality==
-This electric field is proportional to the rate of change of the magnetic field (''d''B/''d''t).
+This electric field is proportional to the rate of change of the magnetic field <math> ( \frac{\delta B}{\delta t} ) </math>.
-====Inside the solenoid====
+===Inside the solenoid===
 Curly electric field is proportional to distance from the solenoid axis, ''r''.
-====Outside the solenoid====
+===Outside the solenoid===
 Curly electric field is proportional to 1/''r'', with the field decreasing as distance from the axis increases.
@@ Line 26: / Line 28: @@
 ''Read more about the [[Non-Coulomb Electric Field]]''
-====Coulomb Electric Field====
+===Coulomb Electric Field===
+Any electric field in accordance with Coulomb's law is said to be a ''Coulomb electric field''.
+Coulomb's Law: <math> \vec{E} = \frac{1}{4{\pi}{{\epsilon}_0}} \frac{q}{r^2} \hat{r} </math>
+===Non-Coulomb Electric Field===
+An electric field associated with a time-varying magnetic field, i.e. the curly electric field.
+===Effect on charges===
+The curly electric field has a standard effect on charges <math> ( \vec{F} = q\vec{E} ) </math>
+Because the curly electric field deals with non-stationary charges and the magnetic field and current are time-variant, the curly electric field is a '''Non-Coloumb Electric Field'''.
+==Direction of Curly Electric Field==
+===Faraday's Experiment===
+[[File:faraday.png|300px|thumb|right|''The setup and observations from Faraday's experiment'']]
+In 1831, [[Michael Faraday]] conducted an experiment which proved magnetic fields could be produced by electric currents. The experiment involved connecting a battery to a large coiled wire, and measuring the effects with a voltmeter. Faraday recorded effects both upon first connecting the battery and when initially disconnecting it the later of which was found surprising.
+Because an effect could only be gauged when the magnetic field was changing, it was concluded that this effect was proportional to <math> ( \frac{\delta B}{\delta t} ) </math>
+===Finding the Direction===
+Implementing this proportion takes the process a step further; a [[Right Hand Rule]] can be utilized to pinpoint the direction of the curly electric field as follows:
+:Point the thumb of the right hand in the direction of <math> ( - \frac{\delta B}{\delta t} ) </math> , and curl the fingers in the direction of the curly electric field.
+[[File:rhr.png|250px|thumb|center|''The right hand rule for finding the direction of curly electric field'']]
+For each of the following four situations, the right hand rule can be used to determine direction of curly electric field.
+*Magnetic field out of the page and increasing <math> \rightarrow </math> Clockwise curly electric field
+*Magnetic field into the page and increasing <math> \rightarrow </math> Counterclockwise curly electric field
+*Magnetic field out of the page and decreasing <math> \rightarrow </math> Counterclockwise curly electric field
+*Magnetic field into the page and decreasing <math> \rightarrow </math> Clockwise curly electric field
+==Driving Current with Curly Electric Field==
+[[File:Currentinefield.png|250px|thumb|left|''The non-Coulombic curly electric field drives the current in the metal ring'']]
+The non-Coulombic curly electric field has the potential to create an effect akin to that of a battery; if a circular metal ring is placed around a solenoid with increasing magnetic field over time (see image), the curly electric field in the solenoid will drive the current in the metal ring clockwise. Further, as in an ordinary circuit, the current in the ring will be proportional to the electric field.
+===emf in Non-Coulomb Field===
+The emf in a non-Coulomb field such as the curly electric field can be computed as the energy input per unit charge. Therefore the equation for emf in a non-Coulombic field is calculated thus:
+: <math> emf = \oint \vec{E}_{NC} \bullet {d}{\vec{l}} </math>
+====Outside Path====
-====Non-Coulomb Electric Field====
+For any round-trip path that lies outside the solenoid--that is, it does not encircle the solenoid-- the emf is equal to zero. In the picture below, the path on the left ''does'' encircle the solenoid, and therefore has a nonzero emf. However, the rightmost path ''does not'' encircle the solenoid, and therefore that path has a zero emf value.
+[[File:encricleemf.png|400px|thumb|center|''When the solenoid is not encircled by the path, emf = 0'']]
-====Effect on charges====
+==External Links==
+*http://physwiki.ucdavis.edu/Fundamentals/11._Electromagnetism/11.5_Induced_Electric_Fields
+*http://www.phy.uct.ac.za/courses/opencontent/phy1004w/1004W%20EM%2022.pdf
-The curly electric field has
+==References==
+#''Matter and Interactions'', Vol. 2 by Chabay and Sherwood
+#http://physwiki.ucdavis.edu/Fundamentals/11._Electromagnetism/11.5_Induced_Electric_Fields
+#http://www.phy.uct.ac.za/courses/opencontent/phy1004w/1004W%20EM%2022.pdf