Lecture 12 Review Source transformations Maximum power transfer
- Slides: 19
Lecture 12 • Review: • Source transformations • Maximum power transfer • Derivation of maximum power transfer • Thévenin theorem examples • Operational Amplifiers • Related educational modules: –Sections 1. 7. 5, 1. 8. 0, 1. 8. 1
Using Source Transformations in Circuit Analysis • Any voltage source in series with a resistance can be modeled as a current source in parallel with the same resistance and vice-versa
Maximum Power Transfer • The load receives the maximum amount of power if RL = RTH • Why?
Maximum Power Transfer – Derivation • Load voltage: • Delivered power:
Maximizing power • Set derivative of power to zero: • Chain rule: • Set numerator to zero:
Maximum Power Delivered • Delivered power: • Letting RL = RTH:
Example 1: Maximum power transfer (a) Determine the load resistance, R, which absorbs the maximum power from the circuit. (b) What is the maximum power delivered to the load?
Example 1(a): Load Design
Example 1(b): Power delivered
Example 2 • Determine the Norton equivalent of the circuit of example 1
Operational Amplifiers • So far, with the exception of our ideal power sources, all the circuit elements we have examined have been passive – Total energy delivered by the circuit to the element is non -negative • We now introduce another class of active devices – Operational Amplifiers (op-amps) – Note: These require an external power supply!
Operational Amplifiers – overview • We will analyze op-amps as a “device” or “black box”, without worrying about their internal circuitry – This may make it appear as if KVL, KCL do not apply to the operational amplifier – Our analysis is based on “rules” for the overall op-amp operation, and not performing a detailed analysis of the internal circuitry • We want to use op-amps to perform operations, not design and build the op-amps themselves
u. A 741 op-amp schematic • Source: RFIC Technologies web site
Ideal Operational Amplifiers • Typical circuit schematic symbol: • Three-terminal device (2 inputs, 1 output) • Operation characterized by: – Voltage difference between input terminals ( vin) – Currents into the input terminals (ip and in)
Ideal Operational Amplifier “Rules” • More complete circuit symbol • (Power supplies shown) • Assumptions: • ip = 0, in = 0 • vin = 0 • V - < vout < V +
Notes on op-amp operation 1. Output current is generally not known (it is provided by external power supplies) 2. KCL at input nodes is generally a good starting point in op-amp circuit analysis 3. vin is multiplied by a large number to get vout 4. vout is limited by the external power supplies
Op-amp circuit – example 1 • Find Vout
Op-amp circuit – example 2 • Find Vout
- Maximum power transfer theorem
- Maximum power transfer ac
- Maximum power transfer formula
- Maximum power transfer theorem
- Source transformation
- Maximum power transfer theorem
- L matching network
- Absolute max
- Maximum parsimony vs maximum likelihood
- Maximum likelihood vs maximum parsimony
- 01:640:244 lecture notes - lecture 15: plat, idah, farad
- Real power formula
- Ac source transformation
- Transformations review game
- Intensity transformation in digital image processing
- Quantile plot in data mining
- Calculate the maximum monochromatic emissive power at 288k
- Photovoltaic array maximum power point tracking array
- Is a disturbance that transfers energy from place to place
- Power system dynamics and stability lecture notes