Dell
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2 infinite plates are placed one next to another in a V formation with an angle β between them, they have charge densities of σ1 and σ2. what is the magitude of the field betweein them.
ϕ=\ointEdA=EA
ϕ=\frac{q}{ϵ}=\frac{σA}{ϵ}
E1=\frac{σ1}{ϵ}
E2=\frac{σ2}{ϵ}
E=E1+E2
lets make our x-axis parallel to plate 1 giving E1 a 0 value on x axis
Ex= 0 + \frac{σ2}{ϵ}*sinβ
Ey= \frac{σ1}{ϵ} + \frac{σ2}{ϵ}*cosβ
|E|2=|Ex|2 + |Ey|2
=(\frac{σ2}{ϵ}*sinβ)2 +(\frac{σ1}{ϵ} + \frac{σ2}{ϵ}*cosβ)2
=\frac{1}{ϵ}*(σ22sin2β + σ12 + σ22cos2β + 2(σ1)(σ2)cosβ )
=\frac{1}{ϵ}*(σ22(sin2β + cos2β ) + σ12 + 2(σ1)(σ2)cosβ)
|E|2=\frac{1}{ϵ}*(σ12 + σ22 + 2(σ1)(σ2)cosβ)
which is almost right except that in my answers there is a second possible solution that
|E|2=\frac{1}{ϵ}*(σ12 + σ22 - 2(σ1)(σ2)cosβ)
where does this minus come from? originally i thought it might be because of a possible negative charge density but surely if that was so the sign would be part of σ and come automatically when i plug in values
ϕ=\ointEdA=EA
ϕ=\frac{q}{ϵ}=\frac{σA}{ϵ}
E1=\frac{σ1}{ϵ}
E2=\frac{σ2}{ϵ}
E=E1+E2
lets make our x-axis parallel to plate 1 giving E1 a 0 value on x axis
Ex= 0 + \frac{σ2}{ϵ}*sinβ
Ey= \frac{σ1}{ϵ} + \frac{σ2}{ϵ}*cosβ
|E|2=|Ex|2 + |Ey|2
=(\frac{σ2}{ϵ}*sinβ)2 +(\frac{σ1}{ϵ} + \frac{σ2}{ϵ}*cosβ)2
=\frac{1}{ϵ}*(σ22sin2β + σ12 + σ22cos2β + 2(σ1)(σ2)cosβ )
=\frac{1}{ϵ}*(σ22(sin2β + cos2β ) + σ12 + 2(σ1)(σ2)cosβ)
|E|2=\frac{1}{ϵ}*(σ12 + σ22 + 2(σ1)(σ2)cosβ)
which is almost right except that in my answers there is a second possible solution that
|E|2=\frac{1}{ϵ}*(σ12 + σ22 - 2(σ1)(σ2)cosβ)
where does this minus come from? originally i thought it might be because of a possible negative charge density but surely if that was so the sign would be part of σ and come automatically when i plug in values