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Question: Radius of current carrying coil is ‘R’. If fractional decreases in field value with respect to the c...

Radius of current carrying coil is ‘R’. If fractional decreases in field value with respect to the center of the coil for a nearby axial point is 1% then the final axial position of that point.

Explanation

Solution

In this question let the distance of the axial point with respect to the center of the coil be x. We have to use the formula of magnetic field at the axis and the magnetic field at center of the coil. Then we can evaluate the axial position of the point.
Formula used:
Use the formula of the magnetic field at the axis.
B=μoiR22(X2+R2)32B=\dfrac{{{\mu }_{o}}i{{R}^{2}}}{2{{\left( {{X}^{2}}+{{R}^{2}} \right)}^{\dfrac{3}{2}}}}
And magnetic field at the center of coil is
B=μ0i2RB=\dfrac{{{\mu }_{0}}i}{2R}

Complete answer:
Given data:
Radius of the current carrying coil is R. Let the distance of the axial point w.r.t center of the coil be x. We know, magnetic field at this point w.r.t the center or at the axis is given as
B=μoiR22(X2+R2)32........(1)B=\dfrac{{{\mu }_{o}}i{{R}^{2}}}{2{{\left( {{X}^{2}}+{{R}^{2}} \right)}^{\dfrac{3}{2}}}}........\left( 1 \right)
Where, B = magnetic field at the axis
‘i’ = current in the coil
R = radius of the coil
μo{{\mu }_{o}} = permeability of free space
As we know magnetic field at the center of the coil is given as,
Bcenter=μoi2R.......(2){{B}_{center}}=\dfrac{{{\mu }_{o}}i}{2R}.......\left( 2 \right)
Where, Bcenter{{B}_{center}} = magnetic field at the center
‘i’ = current in the coil
R = radius of the coil
μo{{\mu }_{o}}= permeability of the free space
Now it is given to us in question that the fractional decreases in the field w.r.t. the center of the coil for a nearby axial point is 1%
ΔB=1100Bcenter\Delta B=\dfrac{1}{100}{{B}_{center}}
Where ΔB\Delta B is the difference of equation (2) and (1) i.e. difference of the magnetic fields. Now substitute the values we have,
μoi2RμoiR22(x2+R2)32=1100μoi2R\Rightarrow \dfrac{{{\mu }_{o}}i}{2R}-\dfrac{{{\mu }_{o}}i{{R}^{2}}}{2{{\left( {{x}^{2}}+{{R}^{2}} \right)}^{\dfrac{3}{2}}}}=\dfrac{1}{100}\dfrac{{{\mu }_{o}}i}{2R}
Now simplify this we have,
μoi2R1100μoi2R=μoiR22(x2+R2)32     99100μoi2R=μoiR22(x2+R2)32 \begin{aligned} & \dfrac{{{\mu }_{o}}i}{2R}-\dfrac{1}{100}\dfrac{{{\mu }_{o}}i}{2R}=\dfrac{{{\mu }_{o}}i{{R}^{2}}}{2{{\left( {{x}^{2}}+{{R}^{2}} \right)}^{\dfrac{3}{2}}}} \\\ & \implies \dfrac{99}{100}\dfrac{{{\mu }_{o}}i}{2R}=\dfrac{{{\mu }_{o}}i{{R}^{2}}}{2{{\left( {{x}^{2}}+{{R}^{2}} \right)}^{\dfrac{3}{2}}}} \\\ \end{aligned}
Now cancel out the common terms, we have,
99100=R3(x2+R2)32     (x2+R2)32=10099R3     (x2+R2)=(10099R3)23     (x2+R2)=(10099)23R2     x2+R2=1.0067R2     x2=(1.00671)R2     x2=0.0067R2 \begin{aligned} & \dfrac{99}{100}=\dfrac{{{R}^{3}}}{{{\left( {{x}^{2}}+{{R}^{2}} \right)}^{\dfrac{3}{2}}}} \\\ & \implies {{\left( {{x}^{2}}+{{R}^{2}} \right)}^{\dfrac{3}{2}}}=\dfrac{100}{99}{{R}^{3}} \\\ & \implies \left( {{x}^{2}}+{{R}^{2}} \right)={{\left( \dfrac{100}{99}{{R}^{3}} \right)}^{\dfrac{2}{3}}} \\\ & \implies \left( {{x}^{2}}+{{R}^{2}} \right)={{\left( \dfrac{100}{99} \right)}^{\dfrac{2}{3}}}{{R}^{2}} \\\ & \implies {{x}^{2}}+{{R}^{2}}=1.0067{{R}^{2}} \\\ & \implies {{x}^{2}}=\left( 1.0067-1 \right){{R}^{2}} \\\ & \implies {{x}^{2}}=0.0067{{R}^{2}} \\\ \end{aligned}

Now take square root on both sides we have,
x=0.0067R2=±0.0818Rx=\sqrt{0.0067{{R}^{2}}}=\pm 0.0818R
So at the distance ±0.0818R\pm 0.0818R the fractional decrease in field value w.r.t center of the coil for nearby axial point is 1% hence, this is the required answer.

Note:
It is advised to remember the formula for magnetic field at any point x due to circular current carrying coil of radius R and magnetic field at the center of coil the trick was that magnetic permeability is taken as μo{{\mu }_{o}} because coil is placed in air however suppose if this would have not been the case then it would have taken in accordance to medium’s permeability involved.