Example 21.12 Field of two oppositely charged infinite sheets wo infinite plane sheets with uniform surface charge densities 21.26 Finding the electric field due to two oppositely charged o and -o are placed parallel to each other with separation d infinite sheets. The sheets are seen edge-on; only a portion of the Fig. 21.26). Find the electriç field between the sheets, above the infinite sheets can be shown! pper sheet, and below the lower sheet. SOLUTION E = E, + E, = 0 Sheet 2 の ENTIFY and SET UP: Equation (21.12) gives the electric field ue to a single infinite plane sheet of charge. To find the field due two such sheets, we combine the fields using the principle of perposition (Fig. 21.26). E4 AE, Sheet I E = E, + E, = 0

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How is the value between the two sheets like this? If possible i'd like a step by step explanation for it
Example 21.12
Field of two oppositely charged infinite sheets
Two infinite plane sheets with uniform surface charge densities 21.26 Finding the electric field due to two oppositely charged
to and -o are placed parallel to each other with separation d infinite sheets. The sheets are seen edge-on; only a portion of the
(Fig. 21.26). Find the electric field between the sheets, above the infinite sheets can be shown!
upper sheet, and below the lower sheet.
SOLUTION
E-
E = E,+E, = 0
Sheet 2
IDENTIFY and SET UP: Equation (21.12) gives the electric field
due to a single infinite plane sheet of charge. To find the field due
to two such sheets, we combine the fields using the principle of
superposition (Fig. 21.26).
Sheet 1
E = E, + E, = 0
Transcribed Image Text:Example 21.12 Field of two oppositely charged infinite sheets Two infinite plane sheets with uniform surface charge densities 21.26 Finding the electric field due to two oppositely charged to and -o are placed parallel to each other with separation d infinite sheets. The sheets are seen edge-on; only a portion of the (Fig. 21.26). Find the electric field between the sheets, above the infinite sheets can be shown! upper sheet, and below the lower sheet. SOLUTION E- E = E,+E, = 0 Sheet 2 IDENTIFY and SET UP: Equation (21.12) gives the electric field due to a single infinite plane sheet of charge. To find the field due to two such sheets, we combine the fields using the principle of superposition (Fig. 21.26). Sheet 1 E = E, + E, = 0
some
above the upper sheet
È = Ë ¡ + Ë; = {-j
charg
fields
between the sheets
%D
tions
below the lower sheet
tor su
Transcribed Image Text:some above the upper sheet È = Ë ¡ + Ë; = {-j charg fields between the sheets %D tions below the lower sheet tor su
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