By the superposition property, the resulting field in E ⃗ \vec{E} E is the sum E ⃗ 1 + E ⃗ 2 \vec{E}_1+\vec{E}_2 E 1 + E 2 of fields generated by each of charges. Let us calculate each of fields :
E ⃗ 1 = 1 4 π ε 0 q 1 ∣ r 1 − r ∣ 3 ( r ⃗ − r ⃗ 1 ) = 1 4 π ⋅ 8.85 ⋅ 1 0 − 12 2 ⋅ 1 0 − 6 0.0 8 2 + 0.0 6 2 3 ⋅ ( 0.08 , 0.06 ) \vec{E}_1=\frac{1}{4\pi \varepsilon_0}\frac{q_1}{|r_1-r|^3}(\vec{r}-\vec{r}_1)=\frac{1}{4\pi \cdot 8.85\cdot 10^{-12}}\frac{2\cdot 10^{-6}}{\sqrt{0.08^2+0.06^2}^3}\cdot(0.08,0.06) E 1 = 4 π ε 0 1 ∣ r 1 − r ∣ 3 q 1 ( r − r 1 ) = 4 π ⋅ 8.85 ⋅ 1 0 − 12 1 0.0 8 2 + 0.0 6 2 3 2 ⋅ 1 0 − 6 ⋅ ( 0.08 , 0.06 ) E ⃗ 1 = 9 ⋅ 1 0 9 ⋅ 2 ⋅ 1 0 − 6 ⋅ 1 0 − 2 1 0 − 3 ⋅ ( 8 , 6 ) = ( 144 , 108 ) V / m \vec{E}_1=\frac{9\cdot 10^9 \cdot 2\cdot 10^{-6}\cdot 10^{-2}}{10^{-3}}\cdot (8,6)=(144, 108) \: V/m E 1 = 1 0 − 3 9 ⋅ 1 0 9 ⋅ 2 ⋅ 1 0 − 6 ⋅ 1 0 − 2 ⋅ ( 8 , 6 ) = ( 144 , 108 ) V / m
E ⃗ 2 = 1 4 π ε 0 q 2 ∣ r 2 − r ∣ 3 ( r ⃗ − r ⃗ 2 ) = 1 4 π ⋅ 8.85 ⋅ 1 0 − 12 3 ⋅ 1 0 − 6 0.0 8 2 + 0.0 6 2 3 ⋅ ( − 0.08 , 0.06 ) \vec{E}_2=\frac{1}{4\pi \varepsilon_0}\frac{q_2}{|r_2-r|^3}(\vec{r}-\vec{r}_2)=\frac{1}{4\pi \cdot 8.85\cdot 10^{-12}}\frac{3\cdot 10^{-6}}{\sqrt{0.08^2+0.06^2}^3}\cdot(-0.08,0.06) E 2 = 4 π ε 0 1 ∣ r 2 − r ∣ 3 q 2 ( r − r 2 ) = 4 π ⋅ 8.85 ⋅ 1 0 − 12 1 0.0 8 2 + 0.0 6 2 3 3 ⋅ 1 0 − 6 ⋅ ( − 0.08 , 0.06 ) E ⃗ 2 = 9 ⋅ 1 0 9 ⋅ 3 ⋅ 1 0 − 6 ⋅ 1 0 − 2 1 0 − 3 ⋅ ( − 8 , 6 ) = ( − 216 , 162 ) V / m \vec{E}_2=\frac{9\cdot 10^9 \cdot 3\cdot 10^{-6}\cdot 10^{-2}}{10^{-3}}\cdot (-8,6)=(-216, 162) \: V/m E 2 = 1 0 − 3 9 ⋅ 1 0 9 ⋅ 3 ⋅ 1 0 − 6 ⋅ 1 0 − 2 ⋅ ( − 8 , 6 ) = ( − 216 , 162 ) V / m
Therefore, the total field is E ⃗ = ( − 72 , 270 ) V / m \vec{E}=(-72,270)\: V/m E = ( − 72 , 270 ) V / m
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