Solveeit Logo

Question

Question: An inductor of \(5\) Henry inductance carries the current of \(2\,A\). How can a \(50\,volt\) self i...

An inductor of 55 Henry inductance carries the current of 2A2\,A. How can a 50volt50\,volt self inductance be made to appear at the end of the inductor ?

Explanation

Solution

EMF is the electromotive force which is produced by either electrochemical cell or by changing the magnetic field. The emf is induced in a coil due to the change of its own flux linked with it is known as Self-induced emf. Emf is induced without physical motion or flux. It is usually denoted by the letter ε\varepsilon .

Complete step by step answer:
In the above problem, it is given that the inductance of the inductor, L=5HL = 5H and it carries a current which is equal to 2A2A.
Induced emf= 50V50V
By Using Faraday’s law, we know that the expression for inductance is given by
ε=Ndϕdt_{\varepsilon = N\dfrac{{d\phi }}{{dt}}}
From our prior knowledge we know that ϕ=μ0NIAl\phi = \dfrac{{{\mu _0}NIA}}{l} . Now substituting this value in the above equation we get,
ε=ddt(μ0N2IAl) ε=μ0N2AldIdt\varepsilon = \dfrac{d}{{dt}}\left( {\dfrac{{{\mu _0}{N^2}IA}}{l}} \right) \\\ \Rightarrow \varepsilon = \dfrac{{{\mu _0}{N^2}A}}{l}\dfrac{{dI}}{{dt}}
ε=LdIdt\Rightarrow \varepsilon = L\dfrac{{dI}}{{dt}}
Now substitute all the values in the above equation to get the final solution,
Ldidt=50 dt=L×di50L\dfrac{{di}}{{dt}} = 50 \\\ \Rightarrow dt = \dfrac{{L \times di}}{{50}}
Now substitute the values of didi and LL in the above equation we get
dt=5×220\Rightarrow dt = \dfrac{{5 \times 2}}{{20}}
dt=0.2s\therefore dt = 0.2s

Hence, the induced emf can be produced by decreasing the current to zero at 0.2 s.

Note: Inductance is the ability of an inductor to store energy and it does this in the magnetic field that is created by the flow of electrical current . As a result of the magnetic field associated with the current flow, the inductor generates an opposing voltage proportional to the rate of change in the current circuit.