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To simplify things, we would prefer to have a field that depends only on Q size 12{Q} {} and not on the test charge q size 12{q} {} . The electric field is defined in such a manner that it represents only the charge creating it and is unique at every point in space. Specifically, the electric field E size 12{E} {} is defined to be the ratio of the Coulomb force to the test charge:

E = F q , size 12{E= { {F} over {q,} } } {}

where F size 12{F} {} is the electrostatic force (or Coulomb force) exerted on a positive test charge q size 12{q} {} . It is understood that E size 12{E} {} is in the same direction as F size 12{F} {} . It is also assumed that q size 12{q} {} is so small that it does not alter the charge distribution creating the electric field. The units of electric field are newtons per coulomb (N/C). If the electric field is known, then the electrostatic force on any charge q size 12{q} {} is simply obtained by multiplying charge times electric field, or F = q E size 12{F=qE} {} . Consider the electric field due to a point charge Q size 12{Q} {} . According to Coulomb's law, the force it exerts on a test charge q size 12{q} {} is F = k | qQ | / r 2 size 12{F= { ital "kqQ"} slash {r rSup { size 8{2} } } } {} . Thus the magnitude of the electric field, E size 12{E} {} , for a point charge is

E = | F q | = k | qQ qr 2 | = k | Q | r 2 . size 12{E= { {F} over {q} } =k { { ital "qQ"} over { ital "qr" rSup { size 8{2} } } } =k { {Q} over {r rSup { size 8{2} } } } } {}

Since the test charge cancels, we see that

E = k | Q | r 2 . size 12{E=k { {Q} over {r rSup { size 8{2} } } } } {}

The electric field is thus seen to depend only on the charge Q size 12{Q} {} and the distance r size 12{r} {} ; it is completely independent of the test charge q size 12{q} {} .

Calculating the electric field of a point charge

Calculate the strength and direction of the electric field E size 12{E} {} due to a point charge of 2.00 nC (nano-Coulombs) at a distance of 5.00 mm from the charge.

Strategy

We can find the electric field created by a point charge by using the equation E = kQ / r 2 size 12{E= { ital "kQ"} slash {r rSup { size 8{2} } } } {} .

Solution

Here Q = 2 . 00 × 10 9 size 12{Q=2 "." "00" times "10" rSup { size 8{ - 9} } } {} C and r = 5 . 00 × 10 3 size 12{r=5 "." "00" times "10" rSup { size 8{ - 3} } } {} m. Entering those values into the above equation gives

E = k Q r 2 = ( 8.99 × 10 9 N m 2 /C 2 ) × ( 2.00 × 10 9 C ) ( 5.00 × 10 3 m ) 2 = 7.19 × 10 5 N/C. alignl { stack { size 12{E=k { {Q} over {r rSup { size 8{2} } } } } {} #= \( 9 "." "00" times "10" rSup { size 8{9} } N cdot m rSup { size 8{2} } "/C" rSup { size 8{2} } \) times { { \( 2 "." "00" times "10" rSup { size 8{ - 9} } C \) } over { \( 5 "." "00" times "10" rSup { size 8{ - 3} } m \) rSup { size 8{2} } } } {} # =7 "." "20" times "10" rSup { size 8{5} } "N/C" {}} } {}

Discussion

This electric field strength is the same at any point 5.00 mm away from the charge Q size 12{Q} {} that creates the field. It is positive, meaning that it has a direction pointing away from the charge Q size 12{Q} {} .

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Calculating the force exerted on a point charge by an electric field

What force does the electric field found in the previous example exert on a point charge of –0.250 μ C ?

Strategy

Since we know the electric field strength and the charge in the field, the force on that charge can be calculated using the definition of electric field E = F / q size 12{E= {F} slash {q} } {} rearranged to F = q E size 12{F= ital "qE"} {} .

Solution

The magnitude of the force on a charge q = 0 . 250 μC size 12{q= - 0 "." "250"μC"} {} exerted by a field of strength E = 7 . 20 × 10 5 size 12{E=7 "." "20" times "10" rSup { size 8{5} } } {} N/C is thus,

F = qE = ( 0.250 × 10 –6 C ) ( 7.20 × 10 5 N/C ) = 0.180 N. alignl { stack { size 12{F= ital "qE"} {} #size 12{ {}= \( "-0" "." "250" times "10" rSup { size 8{"-6"} } `C \) \( 7 "." "20" times "10" rSup { size 8{5} } `"N/C" \) } {} # ="-0" "." "180"`N {}} } {}

Because q is negative, the force is directed opposite to the direction of the field.

Discussion

The force is attractive, as expected for unlike charges. (The field was created by a positive charge and here acts on a negative charge.) The charges in this example are typical of common static electricity, and the modest attractive force obtained is similar to forces experienced in static cling and similar situations.

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Phet explorations: electric field of dreams

Play ball! Add charges to the Field of Dreams and see how they react to the electric field. Turn on a background electric field and adjust the direction and magnitude.

Electric Field of Dreams
Practice Key Terms 3

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Source:  OpenStax, College physics for ap® courses. OpenStax CNX. Nov 04, 2016 Download for free at https://legacy.cnx.org/content/col11844/1.14
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