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On a printed circuit board, a relatively long straight conductorand a conducting rectangular loop lie in...

On a printed circuit board, a relatively long straight conductorand a conducting rectangular loop lie in the same plane, as shownin Figure P31.9. Taking h = 0.500 mm, w = 1.50 mm, and L = 2.50 mm, find their mutual inductance.
pH

Figure P31.9

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Answer #1
Concepts and reason

The given problem can be solved by using the expression of magnetic field due to straight current carrying conductor, the concept of mutual inductance.

First, use the expression of magnetic field to calculate the magnetic flux. Then, find the mutual inductance.

Fundamentals

The expression for magnetic field due to straight current carrying conductor can be expressed as follows,

B=μ0I2πrB = \frac{{{\mu _0}I}}{{2\pi r}}

Here, μ0{\mu _0} is the absolute permeability, II is the current and rr is the distance.

The expression for magnetic flux can be expressed as follows,

φB=BdA{\varphi _B} = \int {\vec B \cdot d\vec A}

Here, BB is the magnetic field and AA is the area.

The expression for the mutual inductance can be expressed as follows,

M=NφIM = \frac{{N\varphi }}{I}

Consider the given diagram as follows,

I-
h
-L-

The magnetic field due to the current carrying conductor can be expressed as follows,

B=μ0I2πxB = \frac{{{\mu _0}I}}{{2\pi x}}

Here, xx is the distance from the wire.

The small area of the rectangular loop can be calculated as follows,

dA=Ldxd\vec A = Ldx

Calculate the magnetic flux.

φB=BdA{\varphi _B} = \int {\vec B \cdot d\vec A}

Substitute μ0I2πx\frac{{{\mu _0}I}}{{2\pi x}} for B\vec B and LdxLdx for dAd\vec A in the expression of magnetic flux.

φB=hh+w(μ0I2πx)(Ldx)=Lμ0I2πln(h+wh)\begin{array}{c}\\{\varphi _B} = \int\limits_h^{h + w} {\left( {\frac{{{\mu _0}I}}{{2\pi x}}} \right)\left( {Ldx} \right)} \\\\ = \frac{{L{\mu _0}I}}{{2\pi }}\ln \left( {\frac{{h + w}}{h}} \right)\\\end{array}

The expression for the mutual inductance can be expressed as follows,

M=NφBIM = \frac{{N{\varphi _B}}}{I}

Substitute Lμ0I2πln(h+wh)\frac{{L{\mu _0}I}}{{2\pi }}\ln \left( {\frac{{h + w}}{h}} \right) for φB{\varphi _B} and 11 for NN .

M=(1)(Lμ0I2πln(h+wh))I=Lμ02πln(h+wh)\begin{array}{c}\\M = \frac{{\left( 1 \right)\left( {\frac{{L{\mu _0}I}}{{2\pi }}\ln \left( {\frac{{h + w}}{h}} \right)} \right)}}{I}\\\\ = \frac{{L{\mu _0}}}{{2\pi }}\ln \left( {\frac{{h + w}}{h}} \right)\\\end{array}

Substitute 4π×107Hm14\pi \times {10^{ - 7}}{\rm{ H}} \cdot {{\rm{m}}^{ - 1}} for μ0{\mu _0} , 0.500mm0.500{\rm{ mm}} for hh , 1.50mm1.50{\rm{ mm}} for ww and 2.50mm2.50{\rm{ mm}} for LL .

M=(2.50mm)(4π×107Hm1)2πln(0.500mm+1.50mm0.500mm)=693×1012H\begin{array}{c}\\M = \frac{{\left( {2.50{\rm{ mm}}} \right)\left( {4\pi \times {{10}^{ - 7}}{\rm{ H}} \cdot {{\rm{m}}^{ - 1}}} \right)}}{{2\pi }}\ln \left( {\frac{{0.500{\rm{ mm}} + 1.50{\rm{ mm}}}}{{0.500{\rm{ mm}}}}} \right)\\\\ = 693 \times {10^{ - 12}}{\rm{ H}}\\\end{array}

Convert H{\rm{H}} to pH{\rm{pH}} .

M=(693×1012H)(1pH1012H)=693pH\begin{array}{c}\\M = \left( {693 \times {{10}^{ - 12}}{\rm{ H}}} \right)\left( {\frac{{1{\rm{ pH}}}}{{{{10}^{ - 12}}{\rm{ H}}}}} \right)\\\\ = 693{\rm{ pH}}\\\end{array}

Ans:

The value of mutual induction is 693pH693{\rm{ pH}} .

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