# 3.5: Loss Tangent

- Page ID
- 19556

In Section 3.3, we found that the effect of loss due to non-zero conductivity \(\sigma\) could be concisely quantified using the ratio

\[\frac{\epsilon''}{\epsilon'} = \frac{\sigma}{\omega\epsilon} \label{m0132_eratio}\]

where \(\epsilon'\) and \(\epsilon''\) are the real and imaginary components of the complex permittivity \(\epsilon_c\), and \(\epsilon'\triangleq\epsilon\). In this section, we explore this relationship in greater detail.

Recall Ampere’s law in differential (but otherwise general) form:

\[\nabla \times {\bf H} = {\bf J} + \frac{\partial}{\partial t}{\bf D} \label{m0132_ACL2}\]

The first term on the right is conduction current, whereas the second term on the right is displacement current. In the phasor domain, differentiation with respect to time (\(\partial/\partial t\)) becomes multiplication by \(j\omega\). Therefore, the phasor form of Equation \ref{m0132_ACL2} is

\[\nabla \times \widetilde{\bf H} = \widetilde{\bf J} + j\omega\widetilde{\bf D}\]

Also recall that \(\widetilde{\bf J}=\sigma\widetilde{\bf E}\) and that \(\widetilde{\bf D}=\epsilon\widetilde{\bf E}\). Thus,

\[\nabla \times \widetilde{\bf H} = \sigma\widetilde{\bf E} + j\omega\epsilon\widetilde{\bf E}\]

Interestingly, the total current is the sum of a real-valued conduction current and an imaginary-valued displacement current. This is shown graphically in Figure \(\PageIndex{1}\).

Note that the angle \(\delta\) indicated in Figure \(\PageIndex{1}\) is given by

\[\boxed{ \tan\delta \triangleq \frac{\sigma}{\omega\epsilon} } \label{m0132_lt}\]

The quantity \(\tan\delta\) is referred to as the *loss tangent*. Note that loss tangent is zero for a lossless (\(\sigma\equiv 0\)) material, and increases with increasing loss. Thus, loss tangent provides an alternative way to quantify the effect of loss on the electromagnetic field within a material.

Loss tangent presuming only ohmic (conduction) loss is given by Equation \ref{m0132_lt}.

Comparing Equation \ref{m0132_lt} to Equation \ref{m0132_eratio}, we see loss tangent can equivalently be calculated as

\[\tan\delta = \frac{\epsilon''}{\epsilon} \label{m0132_lt2}\]

and subsequently interpreted as shown in Figure \(\PageIndex{2}\).

The discussion in this section has assumed that \(\epsilon_c\) is complex-valued solely due to ohmic loss. However, it is explained in Section 3.4 that permittivity may also be complex-valued as a way to model delay in the response of \({\bf D}\) to changing \({\bf E}\). Does the concept of loss tangent apply also in this case? Since the math does not distinguish between permittivity which is complex due to loss and permittivity which is complex due to delay, subsequent mathematically-derived results apply in either case. On the other hand, there may be potentially significant differences in the physical manifestation of these effects. For example, a material having large loss tangent due to ohmic loss might become hot when a large electric field is applied, whereas a material having large loss tangent due to delayed response might not. Summarizing:

The expression for loss tangent given by Equation \ref{m0132_lt2} and Figure \(\PageIndex{2}\) does not distinguish between ohmic loss and delayed response.

**Additional Reading:**

- “Dielectric loss” on Wikipedia.