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Question: A wire having mass \(m\) and length \(l\) can freely slide on a pair of parallel smooth horizontal r...

A wire having mass mm and length ll can freely slide on a pair of parallel smooth horizontal rails placed in a vertical magnetic field BB. The rails are connected by a capacitor of capacitance CC. The electric resistance of the rails and the wire is zero. If a constant force FF acts on the wire as shown in the figure. Then, the acceleration of the wire can be given as?

A. a=C2B2lFma = \dfrac{{{C^2}{B^2}l - F}}{m}
B. a=Fm+CBla = \dfrac{F}{{m + CBl}}
C. a=FC2B2lma = \dfrac{{F{C^2}{B^2}l}}{m}
D. a=Fm+CB2l2a = \dfrac{F}{{m + C{B^2}{l^2}}}

Explanation

Solution

Find a relation between charge and magnetic field using the relation of potential and charge. Then differentiate the charge to find current. Then use the formula of force in terms of acceleration as well as in terms of magnetic field. Compare them to solve this question.

Complete step by step answer:
Let the velocity of the wire be vv
And the charge on the capacitor be qq
It is given that the length of the wire is ll
Mass of the wire is mm
The wire is placed in the magnetic field BB
Then emf induced in the wire can be given by
e=Blve = Blv
The potential difference across the terminals of a capacitor and the emf induced in the wire must be equal as they are connected in parallel.
V=e\Rightarrow V = e
We know that,
q=CVq = CV
V=qC\Rightarrow V = \dfrac{q}{C}
Therefore, we get
qC=Blv\dfrac{q}{C} = Blv
q=BClv\Rightarrow q = BClv
Differentiating it with respect to tt we get
i=dqdti = \dfrac{{dq}}{{dt}}
i=ddt(CBlv)\Rightarrow i = \dfrac{d}{{dt}}\left( {CBlv} \right)
Since, CBlCBl is constant, we get
i=CBlddt(v)\Rightarrow i = CBl\dfrac{d}{{dt}}\left( v \right)
Since, dvdt=a\dfrac{{dv}}{{dt}} = a
We get
i=CBlai = CBla
Where,
aa is acceleration of the wire
Now, the net force on the rod will be the force due to gravity and the force due to the magnetic field.
Fnet=FgFm{F_{net}} = {F_g} - {F_m} . . . (1)
Where,
Fg=mg{F_g} = mg is the force due to gravity
Fm=ilB{F_m} = ilB is the force due to the magnetic field.
And Fnet=ma{F_{net}} = ma is the resultant force
ma=mgilB\Rightarrow ma = mg - ilB
Substituting the value of ii in the above equation, we get
ma=mgCBlaBlma = mg - CBlaBl
By rearranging it we get
(m+CB2l2)a=mg(m + C{B^2}{l^2})a = mg
a=Fm+CB2l2\Rightarrow a = \dfrac{F}{{m + C{B^2}{l^2}}}
Therefore, from the above explanation, the correct answer is, option (D) a=Fm+CB2l2a = \dfrac{F}{{m + C{B^2}{l^2}}}

Note: Net resultant force is actually the sum of all the forcing acting on the body. And still we have done subtraction in equation (1) because, force is a vector quantity and the net resultant force is the vector sum of all the forces. And since, the force due to gravity and the force due to magnetic field will be acting in the opposite direction, we will subtract them.