Physics, asked by nirman95, 3 months ago

Derive the expression for net Electrostatic Field Intensity at a distance "x" on the geometrical axis of a circular ring of radius R. The ring has been given a uniform charge Q.

#Revision Q8

Answers

Answered by kanishkagupta1234
24

Answer:

force is any interaction that, when unopposed, will change the motion of an object. A force can cause an object with mass to change its velocity, i.e., to accelerate. Force can also be described intuitively as a push or a pull. A force has both magnitude and direction, making it a vector quantity.


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Answered by RockingStarPratheek
131

\underline{\underline{\sf{\maltese\:\:Question}}}

  • Derive the expression for net Electrostatic Field Intensity at a distance \sf{x} on the geometrical axis of a circular ring of radius \sf{R}. The ring has been given a uniform charge \sf{Q}

\underline{\underline{\sf{\maltese\:\:Given}}}

  • The circular ring is having the uniform charge \sf{Q}
  • The distance on the geometrical axis of a circular ring is \sf{x}
  • The circular ring is having radius \sf{R}

\underline{\underline{\sf{\maltese\:\:Answer}}}

  • The expression for net Electrostatic Field Intensity at a distance \sf{x} on the geometrical axis of a circular ring of radius \sf{R} is

\boxed{\boxed{\sf{\displaystyle\frac{Qx}{4\pi\varepsilon_0\left(x^2+R^2\right)^{\left(3/2\right)}}}}}

\underline{\underline{\sf{\maltese\:\:Explanation}}}

The diagram of the circular ring having element charge can be drawn as, (Kindly Refer to Attachment - 1)

\textsc{Points Regarding The Diagram,}

  • The circular ring carrying total charge \sf{Q} with a radius of \sf{R}.
  • The electric field can be represented as \overrightarrow{\sf{dE}} at point A on the central \sf{x\:-\:axis}
  • The elemental strip is taken having the small charge \overrightarrow{\sf{dQ}}
  • The component of the electric field along the x-axis direction can be represented by \overrightarrow{\sf{dE_x}}
  • The perpendicular component of the electric field can be shown as \overrightarrow{\sf{dE_\perp}}

Now, considering an element of the charge \sf{dQ_1}. So there must be an element of equal charge \sf{dQ_2} in the direction opposite to that charge.

  • The diagram of the circular ring having equal and opposite charge can drawn as, (Kindly Refer to Attachment - 2)

\textsc{Points Regarding The Diagram,}

  • The perpendicular components of the electric field 1 and 2 will cancel out with each other.
  • So, this figure represents the symmetric representation of the distribution of the charges.
  • Therefore the net electric field of the full circular ring must be in the same line of \sf{x} - axis.
  • The distance from point A to \sf{dQ_1} is represented as \sf{a}
  • The net summation of the charges perpendicular to the \sf{x} - axis direction is zero as they are in opposite direction to each other.
  • Here, \sf{dE_1} and \sf{dE_2} are the electric fields for the charges \sf{dQ_1} and \sf{dQ_2}                                                              
  • Here, \sf{dE_{1x}} and \sf{dE_{2x}} are the components of electric fields of 1 and 2 along \sf{x} - axis and \sf{d E_{1 \perp}} and \sf{d E_{2 \perp}} are the components of electric field in perpendicular direction.

So, the component of the electric field is along the x-axis because to the small element can be calculated as,

\sf{\displaystyle d E_{x}=\frac{k \times d Q}{a^{2}} \cos \phi \quad \ldots \ldots(1)}

  • Here, k is the constant whose value is \sf{1 /\left(4 \pi \varepsilon_{0}\right)}

  • The radius of the circular ring can be expressed from the figure as \sf{a^{2}=x^{2}+R^{2}}

The angle can be calculated as,

\to\sf{\displaystyle\cos \phi=\frac{x}{a}}

\to\sf{\displaystyle\cos \phi=\frac{x}{\sqrt{a}^2}}

\to\sf{\displaystyle\cos \phi=\frac{x}{\sqrt{x^{2}+R^{2}}}}

  • Substituting the values of radius and angle in the above equation (1)

\sf{\displaystyle d E_{x}=\frac{k \times d Q}{a^{2}}\left(\frac{x}{a}\right)}

\to\sf{\displaystyle d E_{x}=\frac{k \times d Q \times x}{\left(\left(x^{2}+R^{2}\right)^{3 / 2}\right)}}

The net electric field because of the total charge in the x direction can be calculated as,

\sf{\displaystyle E_{x}=\int \frac{k x \times d Q}{\left(x^{2}+R^{2}\right)^{(3 / 2)}}}

Substituting the value as \sf{1 /\left(4 \pi \varepsilon_{0}\right)} for k in the above equation and rearranging the equation.

\to\sf{\displaystyle E_{x}=\frac{x}{4 \pi \varepsilon_{0}\left(x^{2}+R^{2}\right)^{(3 / 2)}} \int d Q}

  • Here, \sf{\varepsilon_{0}} is the permittivity of free space.

After integration the equation expressed as,

\to\sf{\displaystyle E_{x}=\frac{Q x}{4 \pi \varepsilon_{0}\left(x^{2}+R^{2}\right)^{(3 / 2)}}}

  • Here, \sf{Q} is the total charge on the circular ring.

Therefore, the expression for net Electrostatic Field Intensity at a distance \sf{x} on the geometrical axis of a circular ring of radius \sf{R} is

\boxed{\boxed{\sf{\displaystyle\frac{Qx}{4\pi\varepsilon_0\left(x^2+R^2\right)^{\left(3/2\right)}}}}}

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