Courses
Courses for Kids
Free study material
Offline Centres
More
Store Icon
Store

Three long, straight and parallel wires are arranged as shown in figure. The force
experienced by 10 cm length of wire $Q$ is

seo images


A. $1.4 \times {10^{ - 4}}\;{\rm{N}}$ toward the right
B. $1.4 \times {10^{ - 4}}\;{\rm{N}}$ towards the left
C. $2.6 \times {10^{ - 4}}\;{\rm{N}}$ toward the right
D. $2.6 \times {10^{ - 4}}\;{\rm{N}}$ toward the left

seo-qna
SearchIcon
Answer
VerifiedVerified
439.2k+ views
Hint: Find the magnetic field due to $R$ on Q and due to $P$on $Q$ and use this expression to find the force and when the current are in opposite direction in the straight conductor, then the force is repulsive in nature.

Formula used: The magnetic field due to infinitely long straight conductor: $B = \dfrac{{{\mu
_0}I}}{{2\pi a}}$

Complete step by step answer:
From the given question, we know that the current in wire $P.\;Q$ and $R$ are ${I_P} =
30\;{\rm{A}}$, ${I_Q} = 10{\rm{A}}$ and ${I_R} = 20\;{\rm{A}}$, the distance between the wire
$R\;$ and $Q$ is ${a_{RQ}} = 0.02\;{\rm{m}}$, the distance between the wire $P$ and $Q$ is
${a_{PQ}} = 0.1\;{\rm{m}}$ and the length of the wire $Q$ is $L = 0.1\;{\rm{m}}$
The magnetic field produced by wire $R$ at $Q$ is expressed as,
${B_{RQ}} = \dfrac{{{\mu _0}{I_R}}}{{2\pi {a_{RQ}}}}$
Since the force experienced by wire $Q$ is in left direction (repulsion) as the directions of the
current are anti parallel and it is calculated as,
$
{F_{RQ}} = {I_Q}L{B_{RQ}}\\
{F_{RQ}} = {I_Q}L\dfrac{{{\mu _0}{I_R}}}{{2\pi {a_{RQ}}}}
$

Similarly, the magnetic field produced by wire $P$ at $Q$ is expressed as,
${B_{PQ}} = \dfrac{{{\mu _0}{I_P}}}{{2\pi {a_{PQ}}}}$
Since the force experienced by wire $Q$ is in right direction (repulsion) as the directions of the
current are anti parallel and it is calculated as,
$
{F_{PQ}} = {I_Q}L{B_{PQ}}\\
{F_{PQ}} = {I_Q}L\dfrac{{{\mu _0}{I_P}}}{{2\pi {a_{PQ}}}}
$
The net force experienced by the wire $Q$ is calculated as,
$
F = {F_{RQ}} - {F_{PQ}}\\
= {I_Q}L\dfrac{{{\mu _0}{I_R}}}{{2\pi {a_{RQ}}}} - {I_Q}L\dfrac{{{\mu _0}{I_P}}}{{2\pi {a_{PQ}}}}\\
= \dfrac{{{I_Q}L{\mu _0}}}{{2\pi }}\left[ {\dfrac{{{I_R}}}{{{a_{RQ}}}} - \dfrac{{{I_P}}}{{{a_{PQ}}}}}
\right]\\
= \dfrac{{10 \times 0.1 \times 4\pi \times {{10}^{ - 7}}}}{{2\pi }}\left[ {\dfrac{{20}}{{0.02}} -
\dfrac{{30}}{{0.1}}} \right]\\
= 1.4 \times {10^{ - 4}}\;{\rm{N}}\;\;{\rm{towards}}\;{\rm{right}}
$

Thus, the force experienced by the wire $Q$ is $1.4 \times {10^{ - 4}}\;{\rm{N}}$ toward right
direction and option (A) is correct.

Note: Be careful while answering, because the formula for finite straight wire and infinite
straight are completely different.
When wire has finite length: \[B = \dfrac{{{\mu _0}I}}{{4\pi a}}\left( {\sin {\phi _2} + \sin {\phi
_1}} \right)\]
When wire has infinite length, ${\phi _1} = {\phi _2} = 90^\circ $: \[B = \dfrac{{{\mu _0}I}}{{2\pi
a}}\]
When wire has infinite length and point $P$ lies at near wire’s end, ${\phi _1} = 90^\circ
\;{\rm{and}}\;{\phi _2} = 0$:
\[B = \dfrac{{{\mu _0}I}}{{4\pi a}}\]