Max power in in sinusoidal circuits

In summary: Average_powerIn summary, the load impedance in a sinusoidal circuit must be the conjugate of the Thevenin resistance, consisting of both the resistive and inductive parts, in order to achieve maximum average power. This is because if the impedances are not conjugate matched, part of the power will not enter the network, resulting in lower dissipation in the resistance. Therefore, in order to achieve maximum power, the input voltage must be fixed and the total reactance must be minimized, leading to the requirement of conjugate matching.
  • #1
dexterbla
4
0
in a sinusoidal circuit, only the resistive part gives the average power. so why is the load impedance the conjugate of thevenin resistance, consisting of both the resistive part and inductive part, required for maximum average power?
 
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  • #2
Part of the power never enters the network if the impedances are not conjugate matched, so the dissipation in the resistance is lower than it could be.
 
  • #3
impedance matching

hi dexterbla! :smile:
dexterbla said:
in a sinusoidal circuit, only the resistive part gives the average power.

he he … it depends how you write it! :biggrin:

as a function of current, yes …

Pav = (Ir.m.s.)2Re(Zload). :smile:

but as a function of voltage, it's …

Pav = (Ir.m.s.)2Re(Zload)

= (Vsource,r.m.s./|Ztotal|)2Re(Zload) :frown:

so if the input current is fixed, yes the reactance has no effect on the maximum power o:); unfortunately, however, life isn't that simple :rolleyes:, and it's always the input voltage that's fixed :redface:,

and then the average power in the load is maximised (for a given Re(Zload)) by minimising |Ztotal| (= |Zsource + Zload|), ie by reducing the total reactance to zero. :smile:

(ie by making Im(Zload) = -Im(Zsource), and since you can prove that power in the load in a purely resistive circuit is maximised when load resistance equals source resistance, that means that the impedances must be conjugates … see http://en.wikipedia.org/wiki/Maximum_power_theorem#Proof" for details :wink:)
 
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  • #5


This is because in a sinusoidal circuit, the inductive and capacitive components cause the voltage and current to be out of phase, resulting in a reactive power component. This reactive power does not contribute to the average power dissipated in the circuit. Therefore, in order to achieve maximum average power, the load impedance must be matched to the Thevenin resistance, which takes into account both the resistive and reactive components, in order to minimize the reactive power and maximize the average power. This is known as the maximum power transfer theorem.
 

1. What is max power in sinusoidal circuits?

Max power in sinusoidal circuits refers to the maximum amount of power that can be delivered to a load in a circuit when it is operating at a sinusoidal frequency. It is also known as the peak power or the maximum power transfer.

2. How is max power calculated in sinusoidal circuits?

Max power in sinusoidal circuits can be calculated using the formula Pmax = Vrms^2/R, where Vrms is the root-mean-square voltage and R is the resistance of the load. Alternatively, it can also be calculated using the formula Pmax = I^2R, where I is the root-mean-square current and R is the resistance of the load.

3. What is the significance of max power in sinusoidal circuits?

The significance of max power in sinusoidal circuits lies in the fact that it represents the optimum operating point for the circuit. At this point, the load receives the maximum amount of power and the efficiency of the circuit is at its highest. It is important in designing and optimizing circuits for maximum performance.

4. How does max power vary with frequency in sinusoidal circuits?

In sinusoidal circuits, max power varies with frequency according to the power transfer theorem, which states that the maximum power is transferred when the load impedance is equal to the complex conjugate of the source impedance. This means that as the frequency changes, the load impedance also changes and thus the maximum power transfer point shifts.

5. What are some applications of max power in sinusoidal circuits?

Max power in sinusoidal circuits has several applications, such as in audio amplifiers, where the goal is to deliver the maximum power to the speakers for optimal sound quality. It is also important in power transmission systems, as it allows for efficient transfer of power over long distances. Additionally, it is used in renewable energy systems, where the goal is to maximize the power output of solar panels or wind turbines.

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