Answer
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Hint: We will use the idea of the electric field as a gradient of potential to answer this problem. We are going to solve this problem using the relationship \[E = - \dfrac{{dv}}{{dr}}\].
Complete step by step answer:
We know that in an electrical field the electrical potential between two points A and B is defined as the amount of work performed per unit of positive test charge in moving it against the electrostatic force due to the electrical field from point A to point B.
If $dW$ is the work done in moving a small positive test charge ${q_0}$ from point P to Q, then
$ \Rightarrow (V + dV) - V = \dfrac{{dW}}{{{q_0}}}$.
$ \Rightarrow dV = \dfrac{{dW}}{{{q_0}}}$ ………..(i)
And, if $\overrightarrow E $ is the electric field at point P due to charge +a place at point O, then the test charge experiences a force equal to ,
$ \Rightarrow \overrightarrow F = {q_0}\overrightarrow E $.
Therefore, work done to move the test charge through an infinitely small displacement $PQ = dl$is given by
$dW = \overrightarrow F .\overrightarrow {dl} $
and we have $\overrightarrow F = {q_0}\overrightarrow E $, then
$dW = {q_0}\overrightarrow E .\overrightarrow {dl} = ({q_0}\overrightarrow E ).\overrightarrow {dl} \cos {180^0}$ [ ]
$dW = - {q_0}E.dl$ ……..(ii)
As the distance r decreases in the direction of $\overrightarrow {dl} $, the distance dl is taken as dr.
So now, form equation (ii), we get
$
dW = - {q_0}E.dr \\
\dfrac{{dW}}{{{q_0}}} = - E.dr \\
$
From equation (i), we have $dV = \dfrac{{dW}}{{{q_0}}}$, then
$
dV = - Edr \\
E = - \dfrac{{dV}}{{dr}} \\
$.
Therefore the electric field at a point is equal to the negative gradient of the electric potential at that point.
The negative sign indicates that the direction of E is always in the direction of decreased potential.
Hence, we can say that, In the direction of electric field, the electric potential decreases.
Therefore the correct answer is option (A).
Note: In this type of questions, first we have to identify what relationship of the given terms is required to solve the question. Then we will assume some conditions and prove the statement step by step. While solving the question, we have to remember the significance of the signs. After that we will get the required answer.
Complete step by step answer:
We know that in an electrical field the electrical potential between two points A and B is defined as the amount of work performed per unit of positive test charge in moving it against the electrostatic force due to the electrical field from point A to point B.
If $dW$ is the work done in moving a small positive test charge ${q_0}$ from point P to Q, then
$ \Rightarrow (V + dV) - V = \dfrac{{dW}}{{{q_0}}}$.
$ \Rightarrow dV = \dfrac{{dW}}{{{q_0}}}$ ………..(i)
And, if $\overrightarrow E $ is the electric field at point P due to charge +a place at point O, then the test charge experiences a force equal to ,
$ \Rightarrow \overrightarrow F = {q_0}\overrightarrow E $.
Therefore, work done to move the test charge through an infinitely small displacement $PQ = dl$is given by
$dW = \overrightarrow F .\overrightarrow {dl} $
and we have $\overrightarrow F = {q_0}\overrightarrow E $, then
$dW = {q_0}\overrightarrow E .\overrightarrow {dl} = ({q_0}\overrightarrow E ).\overrightarrow {dl} \cos {180^0}$ [ ]
$dW = - {q_0}E.dl$ ……..(ii)
As the distance r decreases in the direction of $\overrightarrow {dl} $, the distance dl is taken as dr.
So now, form equation (ii), we get
$
dW = - {q_0}E.dr \\
\dfrac{{dW}}{{{q_0}}} = - E.dr \\
$
From equation (i), we have $dV = \dfrac{{dW}}{{{q_0}}}$, then
$
dV = - Edr \\
E = - \dfrac{{dV}}{{dr}} \\
$.
Therefore the electric field at a point is equal to the negative gradient of the electric potential at that point.
The negative sign indicates that the direction of E is always in the direction of decreased potential.
Hence, we can say that, In the direction of electric field, the electric potential decreases.
Therefore the correct answer is option (A).
Note: In this type of questions, first we have to identify what relationship of the given terms is required to solve the question. Then we will assume some conditions and prove the statement step by step. While solving the question, we have to remember the significance of the signs. After that we will get the required answer.
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