Let's write the forces that act on charge q 3 q_3 q 3 due to charges q 1 q_1 q 1 and q 2 q_2 q 2 :
F 1 = k q 1 q 3 r 2 , F_1=\dfrac{kq_1q_3}{r^2}, F 1 = r 2 k q 1 q 3 , F 2 = k q 2 q 3 r 2 . F_2=\dfrac{kq_2q_3}{r^2}. F 2 = r 2 k q 2 q 3 .
We can find the distance from the charges q 1 q_1 q 1 and q 3 q_3 q 3 as well as q 2 q_2 q 2 and q 3 q_3 q 3 from the Pythagorean theorem:
r = ( 0.3 m ) 2 + ( 0.4 m ) 2 = 0.5 m . r=\sqrt{(0.3\ m)^2+(0.4\ m)^2}=0.5\ m. r = ( 0.3 m ) 2 + ( 0.4 m ) 2 = 0.5 m . Since, q 1 = q 2 q_1=q_2 q 1 = q 2 and r 1 = r 2 = r r_1=r_2=r r 1 = r 2 = r the magnitudes of two forces are equal. Let's write the components of forces F 1 F_1 F 1 and F 2 F_2 F 2 in projections on x x x and y y y axis:
F 1 c o s θ + F 2 c o s θ = 2 F 1 c o s θ , F_1cos\theta+F_2cos\theta=2F_1cos\theta, F 1 cos θ + F 2 cos θ = 2 F 1 cos θ , − F 1 s i n θ + F 2 s i n θ = 0. -F_1sin\theta+F_2sin\theta=0. − F 1 s in θ + F 2 s in θ = 0. As we can see, y y y -components cancel out, so we can write the net force on q 3 q_3 q 3 :
F n e t = 2 k q 1 q 3 r 2 c o s θ . F_{net}=2\dfrac{kq_1q_3}{r^2}cos\theta. F n e t = 2 r 2 k q 1 q 3 cos θ . We can find angle θ \theta θ from the geometry:
θ = c o s − 1 ( 0.4 m 0.5 m ) = 36.8 6 ∘ . \theta=cos^{-1}(\dfrac{0.4\ m}{0.5\ m})=36.86^{\circ}. θ = co s − 1 ( 0.5 m 0.4 m ) = 36.8 6 ∘ . Finally, we can find the net force on q 3 q_3 q 3 :
F n e t = 2 ⋅ 9 ⋅ 1 0 9 N m 2 C 2 ⋅ ( 2 ⋅ 1 0 − 6 C ) 2 ( 0.5 m ) 2 c o s 36.8 6 ∘ = 0.23 N . F_{net}=2\cdot\dfrac{9\cdot10^9\ \dfrac{Nm^2}{C^2}\cdot(2\cdot10^{-6}\ C)^2}{(0.5\ m)^2}cos36.86^{\circ}=0.23\ N. F n e t = 2 ⋅ ( 0.5 m ) 2 9 ⋅ 1 0 9 C 2 N m 2 ⋅ ( 2 ⋅ 1 0 − 6 C ) 2 cos 36.8 6 ∘ = 0.23 N . Answer:
F n e t = 0.23 N , F_{net}=0.23\ N, F n e t = 0.23 N , in + x +x + x -direction.
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