For the given figure the direction of electric field at point A will be (Given that AB=BC=CA)
A.Towards AL
B.Towards AY
C.Towards AX
D.Towards AZ
Answer
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Hint: Study about the electric field at a distance r due to a point charge. Find the direction and the value of the field at point A due to both the charges. Then take the components and cancel the opposite and equal terms. The final value and direction will be given by the vector sum of the remaining components.
Formula used:
$E=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{q}{{{r}^{2}}}$
Complete step by step answer:
The electric field due to a point charge q at a distance r is given by,
$E=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{q}{{{r}^{2}}}$
Where, ${{\varepsilon }_{0}}$ is the permittivity of free space
$\dfrac{1}{4\pi {{\varepsilon }_{0}}}=8.98\times {{10}^{9}}N{{m}^{2}}{{C}^{-2}}\approx 9\times {{10}^{9}}N{{m}^{2}}{{C}^{-2}}$
Electric field at point A due to the point charge Q at point B is
${{E}_{1}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{A{{B}^{2}}}$ , which will be along AX
Electric field at point A due to the point charge -Q at point C is
${{E}_{2}}=-\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{A{{C}^{2}}}$ , which will be along AZ
Now, ${{E}_{1}}$ will make an angle of ${{60}^{0}}$with AY
Taking the components of ${{E}_{1}}$,
Along AY ${{E}_{1}}\cos {{60}^{0}}$
Along AL ${{E}_{1}}\sin {{60}^{o}}$
${{E}_{2}}$ will make an angle of ${{60}^{0}}$with AY
Taking the components of ${{E}_{2}}$,
Along AY ${{E}_{2}}\cos {{60}^{0}}$
Along negative direction of AL ${{E}_{2}}\sin {{60}^{0}}$
Now along AL and opposite to AL we have the same field. So, it will cancel out each other.
So, we have the total field along AY direction.
The correct option is (B)
Note: Superposition of electric charge tells us that if there is more than one charge then each charge will contribute individually to the electric field. The total electric field will be the vector sum of all the fields.
Formula used:
$E=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{q}{{{r}^{2}}}$
Complete step by step answer:
The electric field due to a point charge q at a distance r is given by,
$E=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{q}{{{r}^{2}}}$
Where, ${{\varepsilon }_{0}}$ is the permittivity of free space
$\dfrac{1}{4\pi {{\varepsilon }_{0}}}=8.98\times {{10}^{9}}N{{m}^{2}}{{C}^{-2}}\approx 9\times {{10}^{9}}N{{m}^{2}}{{C}^{-2}}$
Electric field at point A due to the point charge Q at point B is
${{E}_{1}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{A{{B}^{2}}}$ , which will be along AX
Electric field at point A due to the point charge -Q at point C is
${{E}_{2}}=-\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{A{{C}^{2}}}$ , which will be along AZ
Now, ${{E}_{1}}$ will make an angle of ${{60}^{0}}$with AY
Taking the components of ${{E}_{1}}$,
Along AY ${{E}_{1}}\cos {{60}^{0}}$
Along AL ${{E}_{1}}\sin {{60}^{o}}$
${{E}_{2}}$ will make an angle of ${{60}^{0}}$with AY
Taking the components of ${{E}_{2}}$,
Along AY ${{E}_{2}}\cos {{60}^{0}}$
Along negative direction of AL ${{E}_{2}}\sin {{60}^{0}}$
Now along AL and opposite to AL we have the same field. So, it will cancel out each other.
So, we have the total field along AY direction.
The correct option is (B)
Note: Superposition of electric charge tells us that if there is more than one charge then each charge will contribute individually to the electric field. The total electric field will be the vector sum of all the fields.
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