Physics for Scientists and Engineers
Physics for Scientists and Engineers
6th Edition
ISBN: 9781429281843
Author: Tipler
Publisher: MAC HIGHER
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Chapter 27, Problem 23P
To determine

The proof that dBzdz=0,d2Bzdz2=0andd3Bzdz3=0 .

Expert Solution & Answer
Check Mark

Answer to Problem 23P

It is proved that dBzdz=0,d2Bzdz2=0andd3Bzdz3=0 .

Explanation of Solution

Formula used:

The expression for total magnetic fieldis given by,

  Bz=μ0nR2I2(z11+z21)

Calculation:

The total magnetic fieldis calculated as,

  dBzdz=ddz( μ 0 n R 2 I2( z 1 1 + z 2 1 ))=( μ 0 n R 2 I2)(3z1 4 d z 1 dz3z2 4 d z 2 dz) ....... (1)

Differentiate z1=( z+ 1 2 R)2+R2 with respect to z .

  dz1dz=ddz( ( z+ 1 2 R ) 2 + R 2 )=12( ( ( z+ 1 2 R ) 2 + R 2 ) 1 2 )(2( z+ 1 2 R))=( z+ 1 2 R)z1

Differentiate z2=( z 1 2 R)2+R2 with respect to z .

  dz2dz=ddz( ( z 1 2 R ) 2 + R 2 )=12( ( ( z 1 2 R ) 2 + R 2 ) 1 2 )(2( z 1 2 R))=( z 1 2 R)z2

Substitute (z+12R)z1 for dz1dz and (z12R)z2 for dz2dz in equation (1).

  dBzdz=( μ 0 n R 2 I2)(3z1 4( ( z+ 1 2 R ) z 1 )3z2 4( ( z 1 2 R ) z 2 ))=( μ 0 n R 2 I2)( 3( z+ 1 2 R ) z 1 5 + 3( z 1 2 R ) z 2 5 ) ....... (2)

Substitute 0 for z 54R2 for z1 and 54R2 for z2 in equation (2).

  dBzdz=( μ 0 n R 2 I2)( 3( 0+ 1 2 R ) 5 4 R 2 + 3( 0 1 2 R ) 5 4 R 2 )=0

Differentiate equation (2) with respect to z .

  d2Bzdz2=ddz[( μ 0 n R 2 I 2)( 3( z+ 1 2 R ) z 1 5 + 3( z 1 2 R ) z 2 5 )]=( μ 0 n R 2 I2)(3)( ( 1 z 1 5 5( z+ 1 2 R ) z 1 6 ( d z 1 dz ) ) +( 1 z 2 5 5( z+ 1 2 R ) z 2 6 ( d z 2 dz ) )) ....... (3)

Substitute (z+12R)z1 for dz1dz and (z12R)z2 for dz2dz in equation (3).

  d2Bzdz2=( μ 0 n R 2 I2)(3)( ( 1 z 1 5 5( z+ 1 2 R ) z 1 6 ( ( z+ 1 2 R ) z 1 ) ) +( 1 z 2 5 5( z+ 1 2 R ) z 2 6 ( ( z 1 2 R ) z 2 ) ))=( μ 0 n R 2 I2)(3)(( 1 z 1 5 5 ( z+ 1 2 R ) 2 z 1 7 )+( 1 z 2 5 5 ( z 1 2 R ) 2 z 2 7 )) ....... (4)

Substitute 0 for z 54R2 for z1 and 54R2 for z2 in equation (4).

  d2Bzdz2=( μ 0 n R 2 I2)(3)(( 1 ( 5 4 R 2 ) 5 2 5 ( 0+ 1 2 R ) 2 ( 5 4 R 2 ) 7 2 )+( 1 ( 5 4 R 2 ) 5 2 5 ( 0 1 2 R ) 2 ( 5 4 R 2 ) 7 2 ))=( μ 0 n R 2 I2)(3)(1 ( 5 4 R 2 ) 5 2 1 ( 5 4 R 2 ) 5 2 +1 ( 5 4 R 2 ) 5 2 +1 ( 5 4 R 2 ) 5 2 )=0

Differentiate equation (4) with respect to z .

  d3Bzdz3=ddz[( μ 0 n R 2 I 2)(3)(( 1 z 1 5 5 ( z+ 1 2 R ) 2 z 1 7 )+( 1 z 2 5 5 ( z 1 2 R ) 2 z 2 7 ))]=( μ 0 n R 2 I2)(3)[( 5 z 1 6 ( d z 1 dz ) 10( z+ 1 2 R ) z 1 7 35 ( z+ 1 2 R ) 2 z 1 8 ( d z 1 dz ) )+( 5 z 1 6 ( d z 2 dz ) 10( z 1 2 R ) z 1 7 35 ( z 1 2 R ) 2 z 1 8 ( d z 2 dz ) )] ....... (5)

Substitute (z+12R)z1 for dz1dz and (z12R)z2 for dz2dz in equation (5)

   d 3 B z d z 3 =( μ 0 n R 2 I 2 )( 3 )[ ( 5 z 1 6 ( ( z+ 1 2 R ) z 1 ) 10( z+ 1 2 R ) z 1 7 35 ( z+ 1 2 R ) 2 z 1 8 ( ( z+ 1 2 R ) z 1 ) )+ ( 5 z 1 6 ( ( z 1 2 R ) z 1 ) 10( z 1 2 R ) z 1 7 35 ( z 1 2 R ) 2 z 1 8 ( ( z 1 2 R ) z 1 ) ) ]

   =( μ 0 n R 2 I 2 )( 3 )( 15( z+ 1 2 R ) z 1 7 + 35 ( z+ 1 2 R ) 3 z 1 9 15( z 1 2 R ) z 2 7 + 35 ( z 1 2 R ) 2 z 2 9 )........ (6)

Substitute 0 for z 54R2 for z1 and 54R2 for z2 in equation (6).

  d3Bzdz3=( μ 0 n R 2 I2)(3)( 15( 0+ 1 2 R ) ( 5 4 R 2 ) 7 2 + 35 ( 0+ 1 2 R ) 3 ( 5 4 R 2 ) 9 2 15( z 1 2 R ) ( 5 4 R 2 ) 7 2 + 35 ( z 1 2 R ) 2 ( 5 4 R 2 ) 9 2 )=0

Conclusion:

Therefore, it is proved that dBzdz=0,d2Bzdz2=0andd3Bzdz3=0 .

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Chapter 27 Solutions

Physics for Scientists and Engineers

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