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Question: An electromagnetic wave of frequency \(\upsilon =3MHz\) passes from vacuum into a dielectric medium ...

An electromagnetic wave of frequency υ=3MHz\upsilon =3MHz passes from vacuum into a dielectric medium with relative permittivity εr=4{{\varepsilon }_{r}}=4 . Then:
(a) Wavelength is halved and frequency remains unchanged
(b) Wavelength is doubled and frequency remains becomes half
(c) Wavelength is doubled and frequency remains unchanged
(d) Wavelength and frequency both remain unchanged

Explanation

Solution

As the electromagnetic wave passes from one vacuum to a dielectric, it changes its medium. So, in order to comment on the parameters like wavelength and frequency, we will first calculate the speed of the electromagnetic wave in the new medium and then use it to calculate the refractive index of the new medium.

Complete answer:
Since the electromagnetic wave is moving from one medium to another without any loss in its energy, then it is simply a case of refraction and we also know that.
So, by using the property of refraction we can say that the frequency of the EM wave will remain constant throughout.
Hence, the frequency of the EM wave will not change.
Now, let the wavelength of the wave before entering the dielectric be λ1{{\lambda }_{1}} and the wavelength after entering the dielectric be λ2{{\lambda }_{2}}.
Now, we know the relation between λ1{{\lambda }_{1}} and λ2{{\lambda }_{2}} can be given as:
λ2μair=λ1μdielectric\Rightarrow \dfrac{{{\lambda }_{2}}}{{{\mu }_{air}}}=\dfrac{{{\lambda }_{1}}}{{{\mu }_{dielectric}}}
Here, μair{{\mu }_{air}} is equal to 1.
And, μdielectric{{\mu }_{dielectric}} can be found out using the relation:
μdielectric=μrεr\Rightarrow {{\mu }_{dielectric}}=\sqrt{{{\mu }_{r}}{{\varepsilon }_{r}}}
Here,
μr=1\Rightarrow {{\mu }_{r}}=1 [as it is not mentioned in the problem, we will take the standard value]
εr=4\Rightarrow {{\varepsilon }_{r}}=4
Putting these values in the above equation, we get:
μdielectric=1×4 μdielectric=2 \begin{aligned} & \Rightarrow {{\mu }_{dielectric}}=\sqrt{1\times 4} \\\ & \Rightarrow {{\mu }_{dielectric}}=2 \\\ \end{aligned}
Therefore, the wavelength after reflection can be calculated as follows:
λ21=λ12 λ2=λ12 \begin{aligned} & \Rightarrow \dfrac{{{\lambda }_{2}}}{1}=\dfrac{{{\lambda }_{1}}}{2} \\\ & \Rightarrow {{\lambda }_{2}}=\dfrac{{{\lambda }_{1}}}{2} \\\ \end{aligned}
Hence, the wavelength is halved after refraction.
Thus, the final conclusion is, the wavelength is halved and frequency remains unchanged.

Hence, option (a) is the correct option.

Note:
We should know the change in parameters of an electromagnetic wave upon entering a dielectric medium, like the frequency remains unchanged wavelength and speed of the EM wave changes. Upon entering a dielectric, the phase constant of an EM wave can also change.