A cube of side 'a' has a charge q placed at each of its eight corners. The potential at the centre of the cube due to all the charges is:
A) \[\dfrac{16q}{4\pi {{\varepsilon }_{0}}a\sqrt{3}}\]
B) \[\dfrac{16q}{4\pi {{\varepsilon }_{0}}a}\]
C) \[\dfrac{q}{4\pi {{\varepsilon }_{0}}a}\]
D) \[\dfrac{q}{4\pi {{\varepsilon }_{0}}a\sqrt{3}}\]
Answer
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Hint: Here, we calculate potential at centre due to each charge. The distance between each charge and centre is equal to half of the diagonal. The total potential due to 8 charges at the corner will give potential at the centre.
Complete answer:
A diagram can be illustrated as follows:
Let the cube of side be 'a’
So the length of each diagonal is given by \[D=\sqrt{{{a}^{2}}+{{a}^{2}}+{{a}^{2}}}\]
\[=\sqrt{3{{a}^{2}}}=\sqrt{3}a\]
Distance of each corner from the Centre O is half of its diagonal\[r=\dfrac{\sqrt{3}a}{2}\]
Potential at O due to charge q at each centre is given by
\[V=\dfrac{1}{4\pi {{\varepsilon }_{0}}}.\dfrac{a}{r}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}.\dfrac{q}{\dfrac{\sqrt{3}a}{2}} \]
\[ =\dfrac{2q}{4\pi {{\varepsilon }_{0}}\sqrt{3}a} \]
Therefore, net potential at O due to all the 8 changes at the corners of the cubes \[V=8\times \dfrac{2q}{4\pi {{\varepsilon }_{0}}\sqrt{3}a}\]
\[V=\dfrac{16q}{4\pi {{\varepsilon }_{0}}\sqrt{3}a}\]
The electric field at O due to charge at all the corners of the cube is zero, since the electric field due to charges at opposite 8 corners are equal and opposite.
Note:
As we know that the cube of side a and diagonal is \[D=\sqrt{3}a\]. So, Be careful during the calculation of distance of each corner from the Centre is half of its diagonal i.e. \[r=\dfrac{\sqrt{3}a}{2}\] and the potential \[V=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{2q}{\sqrt{3}a}\] For eight corners we multiplied it by 8 we get the results.
Complete answer:
A diagram can be illustrated as follows:
Let the cube of side be 'a’
So the length of each diagonal is given by \[D=\sqrt{{{a}^{2}}+{{a}^{2}}+{{a}^{2}}}\]
\[=\sqrt{3{{a}^{2}}}=\sqrt{3}a\]
Distance of each corner from the Centre O is half of its diagonal\[r=\dfrac{\sqrt{3}a}{2}\]
Potential at O due to charge q at each centre is given by
\[V=\dfrac{1}{4\pi {{\varepsilon }_{0}}}.\dfrac{a}{r}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}.\dfrac{q}{\dfrac{\sqrt{3}a}{2}} \]
\[ =\dfrac{2q}{4\pi {{\varepsilon }_{0}}\sqrt{3}a} \]
Therefore, net potential at O due to all the 8 changes at the corners of the cubes \[V=8\times \dfrac{2q}{4\pi {{\varepsilon }_{0}}\sqrt{3}a}\]
\[V=\dfrac{16q}{4\pi {{\varepsilon }_{0}}\sqrt{3}a}\]
The electric field at O due to charge at all the corners of the cube is zero, since the electric field due to charges at opposite 8 corners are equal and opposite.
Note:
As we know that the cube of side a and diagonal is \[D=\sqrt{3}a\]. So, Be careful during the calculation of distance of each corner from the Centre is half of its diagonal i.e. \[r=\dfrac{\sqrt{3}a}{2}\] and the potential \[V=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{2q}{\sqrt{3}a}\] For eight corners we multiplied it by 8 we get the results.
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