Three charged particles are at the corners of an equilateral triangle as shown in the figure below. (Let q = 4.00
a) You have to break the E-fields into components.
Let q1 be 4 microcoulombs and q2 be 7 microcoulombs. The variables will be positive. I'll deal with the negative charge on q1 "by hand".
E-field1 = k (q1) / L^2.
Because q1 is negative, the E-field's direction at q is to the
right (positive i-hat), toward q1.
E-field2 = k(q2) / L^2
Because q2 is positive, the field direction at q is left and down,
away from q2.
(-cos(60) i-hat - sin(60) j-hat)
Multiply that out.
You've got the vertical component: - sin (60) k(q2) / L^2
You have to subtract the horizontal component of the second E-field from the first: (q1 - q2 cos(60)) k / L^2
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