
An inductor of $5$ Henry inductance carries the current of $2\,A$. How can a $50\,volt$ self inductance be made to appear at the end of the inductor ?
Answer
500.7k+ views
Hint: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 $\varepsilon $.
Complete step by step answer:
In the above problem, it is given that the inductance of the inductor, $L = 5H$ and it carries a current which is equal to $2A$.
Induced emf= $50V$
By Using Faraday’s law, we know that the expression for inductance is given by
$_{\varepsilon = N\dfrac{{d\phi }}{{dt}}}$
From our prior knowledge we know that $\phi = \dfrac{{{\mu _0}NIA}}{l}$ . Now substituting this value in the above equation we get,
$\varepsilon = \dfrac{d}{{dt}}\left( {\dfrac{{{\mu _0}{N^2}IA}}{l}} \right) \\
\Rightarrow \varepsilon = \dfrac{{{\mu _0}{N^2}A}}{l}\dfrac{{dI}}{{dt}}$
$\Rightarrow \varepsilon = L\dfrac{{dI}}{{dt}}$
Now substitute all the values in the above equation to get the final solution,
$L\dfrac{{di}}{{dt}} = 50 \\
\Rightarrow dt = \dfrac{{L \times di}}{{50}} $
Now substitute the values of $di$ and $L$ in the above equation we get
$ \Rightarrow dt = \dfrac{{5 \times 2}}{{20}}$
$ \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.
Complete step by step answer:
In the above problem, it is given that the inductance of the inductor, $L = 5H$ and it carries a current which is equal to $2A$.
Induced emf= $50V$
By Using Faraday’s law, we know that the expression for inductance is given by
$_{\varepsilon = N\dfrac{{d\phi }}{{dt}}}$
From our prior knowledge we know that $\phi = \dfrac{{{\mu _0}NIA}}{l}$ . Now substituting this value in the above equation we get,
$\varepsilon = \dfrac{d}{{dt}}\left( {\dfrac{{{\mu _0}{N^2}IA}}{l}} \right) \\
\Rightarrow \varepsilon = \dfrac{{{\mu _0}{N^2}A}}{l}\dfrac{{dI}}{{dt}}$
$\Rightarrow \varepsilon = L\dfrac{{dI}}{{dt}}$
Now substitute all the values in the above equation to get the final solution,
$L\dfrac{{di}}{{dt}} = 50 \\
\Rightarrow dt = \dfrac{{L \times di}}{{50}} $
Now substitute the values of $di$ and $L$ in the above equation we get
$ \Rightarrow dt = \dfrac{{5 \times 2}}{{20}}$
$ \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.
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