The Anatomy of an Electromagnetic Wave
Imagine you are standing in a completely empty void, and suddenly, a beam of light pierces through the darkness. What exactly is that light made of?
James Clerk Maxwell beautifully demonstrated that light is an electromagnetic wave. It is a synchronized dance of electric and magnetic fields, oscillating through space and time.
But these fields don't just flail around randomly. They follow a very strict set of geometric rules. The most fundamental rule is that an electromagnetic wave is transverse in nature.
This means that the electric field vector E, the magnetic field vector B, and the velocity vector v (the direction the wave is traveling) are all mutually perpendicular to each other.
Decoding the Direction of Propagation
In our specific problem, we are told that the plane electromagnetic wave is propagating along the y-direction.
Let's visualize our 3D coordinate system. We have the x-axis, the y-axis, and the z-axis. The wave is marching steadily along the y-axis.
Because of the transverse nature of the wave, the electric and magnetic fields must oscillate in a plane that is completely perpendicular to the y-axis.
What plane is perpendicular to the y-axis? It is the xz-plane.
Eliminating the Impossible
This geometric constraint is incredibly powerful. If the fields are entirely confined to the xz-plane, they cannot have any component pointing in the y-direction.
Mathematically, this means that the y-component of the electric field, Ey, must be exactly zero. Similarly, the y-component of the magnetic field, By, must also be exactly zero.
Let's look at the options provided in the question. Any option that suggests the presence of Ey or By is physically impossible for a wave traveling along the y-axis.
Option (a) suggests Ey,By. This is incorrect.
Option (b) suggests Ey,Bx. This is incorrect.
Option (d) suggests Ex,By. This is also incorrect.
The Final Verdict
By simple elimination, we are left with only one physically viable option.
The fields must be composed of x and z components. If the electric field is oscillating along the x-axis (Ex), then the magnetic field must oscillate along the z-axis (Bz) to remain perpendicular to both the electric field and the direction of propagation.
Conversely, if the electric field is along the z-axis (Ez), the magnetic field must be along the x-axis (Bx).
Therefore, the possible pairs of components are Ex,Bz or Ez,Bx.
This perfectly matches option (c). The elegance of this problem lies in how a deep physical principle—the transverse nature of light—allows us to solve it without writing down a single complex equation!