In a compound microscope, the objective lens forms a real, inverted, and diminished image at the focal plane of the eyepiece. The eyepiece acts as a magnifier to form a virtual, erect, and magnified image at the least distance of distinct vision. The magnifying power \( M \) of the compound microscope is given by the product of the magnifying powers of the objective lens \( M_o \) and the eyepiece lens \( M_e \): \[ M = M_o \times M_e. \] The magnifying power of the objective lens is given by: \[ M_o = \frac{v_o}{u_o}, \] where \( v_o \) is the image distance and \( u_o \) is the object distance for the objective lens. Since the image is formed at the focal length of the objective lens \( f_o \), we have: \[ v_o = f_o. \] For the eyepiece, the magnifying power is given by: \[ M_e = \frac{D}{f_e}, \] where \( D \) is the least distance of distinct vision and \( f_e \) is the focal length of the eyepiece. Thus, the total magnifying power is: \[ M = \frac{f_o}{u_o} \times \frac{D}{f_e}. \]
A current element X is connected across an AC source of emf \(V = V_0\ sin\ 2πνt\). It is found that the voltage leads the current in phase by \(\frac{π}{ 2}\) radian. If element X was replaced by element Y, the voltage lags behind the current in phase by \(\frac{π}{ 2}\) radian.
(I) Identify elements X and Y by drawing phasor diagrams.
(II) Obtain the condition of resonance when both elements X and Y are connected in series to the source and obtain expression for resonant frequency. What is the impedance value in this case?
In the given reaction sequence, the structure of Y would be: