# Maximum power transfer theorem

In electrical engineering, the maximum power transfer theorem states that, to obtain maximum external power from a power source with internal resistance, the resistance of the load must equal the resistance of the source as viewed from its output terminals. Moritz von Jacobi published the maximum power (transfer) theorem around 1840; it is also referred to as "Jacobi's law".[1]

The theorem results in maximum power transfer from the power source to the load, and not maximum efficiency of useful power out of total power consumed. If the load resistance is made larger than the source resistance, then efficiency increases (since a higher percentage of the source power is transferred to the load), but the magnitude of the load power decreases (since the total circuit resistance increases).[2] If the load resistance is made smaller than the source resistance, then efficiency decreases (since most of the power ends up being dissipated in the source). Although the total power dissipated increases (due to a lower total resistance), the amount dissipated in the load decreases.

The theorem states how to choose (so as to maximize power transfer) the load resistance, once the source resistance is given. It is a common misconception to apply the theorem in the opposite scenario. It does not say how to choose the source resistance for a given load resistance. In fact, the source resistance that maximizes power transfer from a voltage source is always zero (the hypothetical ideal voltage source), regardless of the value of the load resistance.

The theorem can be extended to alternating current circuits that include reactance, and states that maximum power transfer occurs when the load impedance is equal to the complex conjugate of the source impedance.

The mathematics of the theorem also applies to other physical interactions, such as:[2][3]

• mechanical collisions between two objects,
• the sharing of charge between two capacitors,
• liquid flow between two cylinders,
• the transmission and reflection of light at the boundary between two media.

## Maximizing power transfer versus power efficiency

Simplified model for powering a load with resistance RL by a source with voltage VS and resistance RS.

The theorem was originally misunderstood (notably by Joule[4]) to imply that a system consisting of an electric motor driven by a battery could not be more than 50% efficient, since the power dissipated as heat in the battery would always be equal to the power delivered to the motor when the impedances were matched.

In 1880 this assumption was shown to be false by either Edison or his colleague Francis Robbins Upton, who realized that maximum efficiency was not the same as maximum power transfer.

To achieve maximum efficiency, the resistance of the source (whether a battery or a dynamo) could be (or should be) made as close to zero as possible. Using this new understanding, they obtained an efficiency of about 90%, and proved that the electric motor was a practical alternative to the heat engine.

The red curve shows the power in the load, normalized relative to its maximum possible. The black curve shows the efficiency η.

The efficiency η is the ratio of power dissipated by the load resistance RL to total power dissipated by circuit (which includes the voltage source's resistance of RS as well as RL):

${\displaystyle \eta ={\frac {P_{\mathrm {L} }}{P_{\mathrm {Total} }}}={\frac {I^{2}\cdot R_{\mathrm {L} }}{I^{2}\cdot (R_{\mathrm {L} }+R_{\mathrm {S} })}}={\frac {R_{\mathrm {L} }}{R_{\mathrm {L} }+R_{\mathrm {S} }}}={\frac {1}{1+R_{\mathrm {S} }/R_{\mathrm {L} }}}\,.}$

Consider three particular cases:

• If ${\displaystyle R_{\mathrm {L} }/R_{\mathrm {S} }\to 0}$, then ${\displaystyle \eta \to 0.}$ Efficiency approaches 0% if the load resistance approaches zero (a short circuit), since all power is consumed in the source and no power is consumed in the short. Note, voltage sources must have some resistance.
• If ${\displaystyle R_{\mathrm {L} }/R_{\mathrm {S} }=1}$, then ${\displaystyle \eta ={\tfrac {1}{2}}.}$ Efficiency is only 50% if the load resistance equals the source resistance (which is the condition of maximum power transfer).
• If ${\displaystyle R_{\mathrm {L} }/R_{\mathrm {S} }\to \infty }$, then ${\displaystyle \eta \to 1.}$ Efficiency approaches 100% if the load resistance approaches infinity (though the total power level tends towards zero) or if the source resistance approaches zero. Using a large ratio is called impedance bridging.

## Impedance matching

A related concept is reflectionless impedance matching.

In radio frequency transmission lines, and other electronics, there is often a requirement to match the source impedance (at the transmitter) to the load impedance (such as an antenna) to avoid reflections in the transmission line that could overload or damage the transmitter.

## Calculus-based proof for purely resistive circuits

In the simplified model of powering a load with resistance RL by a source with voltage VS and source resistance RS, then by Ohm's law the resulting current I is simply the source voltage divided by the total circuit resistance:

${\displaystyle I={\frac {V_{S}}{R_{\mathrm {S} }+R_{\mathrm {L} }}}.}$

The power PL dissipated in the load is the square of the current multiplied by the resistance:

${\displaystyle P_{\mathrm {L} }=I^{2}R_{\mathrm {L} }=\left({\frac {V_{S}}{R_{\mathrm {S} }+R_{\mathrm {L} }}}\right)^{2}R_{\mathrm {L} }={\frac {V_{S}^{2}}{R_{\mathrm {S} }^{2}/R_{\mathrm {L} }+2R_{\mathrm {S} }+R_{\mathrm {L} }}}.}$

The value of RL for which this expression is a maximum could be calculated by differentiating it, but it is easier to calculate the value of RL for which the denominator

${\displaystyle R_{\mathrm {S} }^{2}/R_{\mathrm {L} }+2R_{\mathrm {S} }+R_{\mathrm {L} }}$
is a minimum. The result will be the same in either case. Differentiating the denominator with respect to RL:
${\displaystyle {\frac {d}{dR_{\mathrm {L} }}}\left(R_{\mathrm {S} }^{2}/R_{\mathrm {L} }+2R_{\mathrm {S} }+R_{\mathrm {L} }\right)=-R_{\mathrm {S} }^{2}/R_{\mathrm {L} }^{2}+1.}$

For a maximum or minimum, the first derivative is zero, so

${\displaystyle R_{\mathrm {S} }^{2}/R_{\mathrm {L} }^{2}=1}$
or
${\displaystyle R_{\mathrm {L} }=\pm R_{\mathrm {S} }.}$

In practical resistive circuits, RS and RL are both positive, so the positive sign in the above is the correct solution.

To find out whether this solution is a minimum or a maximum, the denominator expression is differentiated again:

${\displaystyle {\frac {d^{2}}{dR_{\mathrm {L} }^{2}}}\left({R_{\mathrm {S} }^{2}/R_{\mathrm {L} }+2R_{\mathrm {S} }+R_{\mathrm {L} }}\right)={2R_{\mathrm {S} }^{2}}/{R_{\mathrm {L} }^{3}}.}$

This is always positive for positive values of ${\displaystyle R_{\mathrm {S} }}$ and ${\displaystyle R_{\mathrm {L} }}$, showing that the denominator is a minimum, and the power is therefore a maximum, when

${\displaystyle R_{\mathrm {S} }=R_{\mathrm {L} }.}$

The above proof assumes fixed source resistance ${\displaystyle R_{\mathrm {S} }}$. When the source resistance can be varied, power transferred to the load can be increased by reducing ${\displaystyle R_{\textrm {S}}}$. For example, a 100 Volt source with an ${\displaystyle R_{\textrm {S}}}$ of ${\displaystyle 10\,\Omega }$ will deliver 250 watts of power to a ${\displaystyle 10\,\Omega }$ load; reducing ${\displaystyle R_{\textrm {S}}}$ to ${\displaystyle 0\,\Omega }$ increases the power delivered to 1000 watts.

Note that this shows that maximum power transfer can also be interpreted as the load voltage being equal to one-half of the Thevenin voltage equivalent of the source.[5]

## In reactive circuits

The power transfer theorem also applies when the source and/or load are not purely resistive.

A refinement of the maximum power theorem says that any reactive components of source and load should be of equal magnitude but opposite sign. (See below for a derivation.)

• This means that the source and load impedances should be complex conjugates of each other.
• In the case of purely resistive circuits, the two concepts are identical.

Physically realizable sources and loads are not usually purely resistive, having some inductive or capacitive components, and so practical applications of this theorem, under the name of complex conjugate impedance matching, do, in fact, exist.

If the source is totally inductive (capacitive), then a totally capacitive (inductive) load, in the absence of resistive losses, would receive 100% of the energy from the source but send it back after a quarter cycle.

The resultant circuit is nothing other than a resonant LC circuit in which the energy continues to oscillate to and fro. This oscillation is called reactive power.

Power factor correction (where an inductive reactance is used to "balance out" a capacitive one), is essentially the same idea as complex conjugate impedance matching although it is done for entirely different reasons.

For a fixed reactive source, the maximum power theorem maximizes the real power (P) delivered to the load by complex conjugate matching the load to the source.

For a fixed reactive load, power factor correction minimizes the apparent power (S) (and unnecessary current) conducted by the transmission lines, while maintaining the same amount of real power transfer.

### Proof

In this diagram, AC power is being transferred from the source, with phasor magnitude of voltage ${\displaystyle |V_{\text{S}}|}$ (positive peak voltage) and fixed source impedance ${\displaystyle Z_{\text{S}}}$ (S for source), to a load with impedance ${\displaystyle Z_{\text{L}}}$ (L for load), resulting in a (positive) magnitude ${\displaystyle |I|}$ of the current phasor ${\displaystyle I}$. This magnitude ${\displaystyle |I|}$ results from dividing the magnitude of the source voltage by the magnitude of the total circuit impedance:

${\displaystyle |I|={|V_{\text{S}}| \over |Z_{\text{S}}+Z_{\text{L}}|}.}$

The average power ${\displaystyle P_{\text{L}}}$ dissipated in the load is the square of the current multiplied by the resistive portion (the real part) ${\displaystyle R_{\text{L}}}$ of the load impedance ${\displaystyle Z_{\text{L}}}$:

{\displaystyle {\begin{aligned}P_{\text{L}}&=I_{\text{rms}}^{2}R_{\text{L}}={1 \over 2}|I|^{2}R_{\text{L}}\\&={1 \over 2}\left({|V_{\text{S}}| \over |Z_{\text{S}}+Z_{\text{L}}|}\right)^{2}R_{\text{L}}={1 \over 2}{|V_{\text{S}}|^{2}R_{\text{L}} \over (R_{\text{S}}+R_{\text{L}})^{2}+(X_{\text{S}}+X_{\text{L}})^{2}},\end{aligned}}}
where ${\displaystyle R_{\text{S}}}$ and ${\displaystyle R_{\text{L}}}$ denote the resistances, that is the real parts, and ${\displaystyle X_{\text{S}}}$ and ${\displaystyle X_{\text{L}}}$ denote the reactances, that is the imaginary parts, of respectively the source and load impedances ${\displaystyle Z_{\text{S}}}$ and ${\displaystyle Z_{\text{L}}}$.

To determine, for a given source voltage ${\displaystyle V_{\text{S}}}$ and impedance ${\displaystyle Z_{\text{S}},}$ the value of the load impedance ${\displaystyle Z_{\text{L}},}$ for which this expression for the power yields a maximum, one first finds, for each fixed positive value of ${\displaystyle R_{\text{L}}}$, the value of the reactive term ${\displaystyle X_{\text{L}}}$ for which the denominator

${\displaystyle (R_{\text{S}}+R_{\text{L}})^{2}+(X_{\text{S}}+X_{\text{L}})^{2}}$
is a minimum. Since reactances can be negative, this is achieved by adapting the load reactance to
${\displaystyle X_{\text{L}}=-X_{\text{S}}.}$

This reduces the above equation to:

${\displaystyle P_{\text{L}}={\frac {1}{2}}{\frac {|V_{\text{S}}|^{2}R_{\text{L}}}{(R_{\text{S}}+R_{\text{L}})^{2}}}}$
and it remains to find the value of ${\displaystyle R_{\text{L}}}$ which maximizes this expression. This problem has the same form as in the purely resistive case, and the maximizing condition therefore is ${\displaystyle R_{\text{L}}=R_{\text{S}}.}$

The two maximizing conditions

• ${\displaystyle R_{\text{L}}=R_{\text{S}}}$
• ${\displaystyle X_{\text{L}}=-X_{\text{S}}}$

describe the complex conjugate of the source impedance, denoted by ${\displaystyle ^{*},}$ and thus can be concisely combined to:

${\displaystyle Z_{\text{L}}=Z_{\text{S}}^{*}.}$

## Notes

1. ^ Thompson Phillips (2009-05-30), Dynamo-Electric Machinery; A Manual for Students of Electrotechnics, BiblioBazaar, LLC, ISBN 978-1-110-35104-6
2. ^ a b Harrison, Mark (2013-02-22). "Physical collisions and the maximum power theorem: an analogy between mechanical and electrical situations". Physics Education. 48 (2): 207–211. doi:10.1088/0031-9120/48/2/207. ISSN 0031-9120.
3. ^ Atkin, Keith (2013-08-22). "Energy transfer and a recurring mathematical function". Physics Education. 48 (5): 616–620. doi:10.1088/0031-9120/48/5/616. ISSN 0031-9120.
4. ^ Magnetics, Triad. "Understanding the Maximum Power Theorem". info.triadmagnetics.com. Retrieved 2022-06-08.
5. ^

## References

• H.W. Jackson (1959) Introduction to Electronic Circuits, Prentice-Hall.