**Ferranti Effect in Transmission Line:**

The effect of the line capacitance is to cause the no-load receiving-end voltage to be more than the sending-end voltage. The effect becomes more pronounced as the line length increases. This phenomenon is known as the Ferranti Effect in Transmission Line. A general explanation of this effect is advanced below:

Substituting x = *l* and I_{R}** = **0 (no-load) in Eq. (5.21), we have

The above equation shows that at *l *= 0, the incident (E_{i0}) and reflected (E_{r0}) voltage waves are both equal to V_{R}/2. With reference to Fig. 5.13, as *l* increases, the incident voltage wave increases exponentially in magnitude (V_{R}/2 e^{Î±l}) and turns through a positive angle Î²*l* (represented by phasor OB); while the reflected voltage wave decreases in magnitude exponentially (V_{R}/2 e^{â€“Î±l})Â __and turns through a negative angle Î²__*l*Â (represented by phasor OC).

It is apparent from the geometry of this figure that the resultant phasor voltage V_{S} (OF) is such that |V_{R}| > |V_{S}|.

A simple explanation of the Ferranti Effect in Transmission Line on an approximate basis can be advanced by lumping the inductance and capacitance parameters of the line. As shown in Fig. 5.14 the capacitance is lumped at the receiving-end of the line.

Here

Since C is small compared to L, Ï‰L*l* can be neglected in comparison to 1/Ï‰C*l*.

Thus

Now

Magnitude of voltage rise = |V_{S}|Ï‰^{2}Â CL*l*^{2}

where Î½ = 1/âˆšLC is the velocity of propagation of the electromagnetic wave along the line, which is nearly equal to the velocity of light.