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Pulse-Width Modulation Efficiency

Pulse-Width Modulation (PWM) is a technique used to control the power delivered to electrical devices by varying the width of the pulses in a signal. The efficiency of PWM refers to how effectively this method converts input power into usable output power without excessive losses. Key factors influencing PWM efficiency include the frequency of the PWM signal, the load being driven, and the characteristics of the switching components (like transistors) used in the circuit.

In general, PWM is considered efficient because it minimizes heat generation, as the switching devices are either fully on or fully off, leading to lower power losses compared to linear regulation. The efficiency can be quantified using the formula:

Efficiency(η)=PoutPin×100%\text{Efficiency} (\eta) = \frac{P_{\text{out}}}{P_{\text{in}}} \times 100\%Efficiency(η)=Pin​Pout​​×100%

where PoutP_{\text{out}}Pout​ is the output power delivered to the load, and PinP_{\text{in}}Pin​ is the input power from the source. Hence, high PWM efficiency is crucial in applications like motor control and power supply systems, where maintaining energy efficiency is essential for performance and thermal management.

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Bilateral Monopoly Price Setting

Bilateral monopoly price setting occurs in a market structure where there is a single seller (monopoly) and a single buyer (monopsony) negotiating the price of a good or service. In this scenario, both parties have significant power: the seller can influence the price due to the lack of competition, while the buyer can affect the seller's production decisions due to their unique purchasing position. The equilibrium price is determined through negotiation, often resulting in a price that is higher than the competitive market price but lower than the monopolistic price that would occur in a seller-dominated market.

Key factors influencing the outcome include:

  • The costs and willingness to pay of the seller and the buyer.
  • The strategic behavior of both parties during negotiations.

Mathematically, the price PPP can be represented as a function of the seller's marginal cost MCMCMC and the buyer's marginal utility MUMUMU, leading to an equilibrium condition where PPP maximizes the joint surplus of both parties involved.

Power Spectral Density

Power Spectral Density (PSD) is a measure used in signal processing and statistics to describe how the power of a signal is distributed across different frequency components. It provides a frequency-domain representation of a signal, allowing us to understand which frequencies contribute most to its power. The PSD is typically computed using techniques such as the Fourier Transform, which decomposes a time-domain signal into its constituent frequencies.

The PSD is mathematically defined as the Fourier transform of the autocorrelation function of a signal, and it can be represented as:

S(f)=∫−∞∞R(τ)e−j2πfτdτS(f) = \int_{-\infty}^{\infty} R(\tau) e^{-j 2 \pi f \tau} d\tauS(f)=∫−∞∞​R(τ)e−j2πfτdτ

where S(f)S(f)S(f) is the power spectral density at frequency fff and R(τ)R(\tau)R(τ) is the autocorrelation function of the signal. It is important to note that the PSD is often expressed in units of power per frequency (e.g., Watts/Hz) and helps in identifying the dominant frequencies in a signal, making it invaluable in fields like telecommunications, acoustics, and biomedical engineering.

Hamilton-Jacobi-Bellman

The Hamilton-Jacobi-Bellman (HJB) equation is a fundamental result in optimal control theory, providing a necessary condition for optimality in dynamic programming problems. It relates the value of a decision-making process at a certain state to the values at future states by considering the optimal control actions. The HJB equation can be expressed as:

Vt(x)+min⁡u[f(x,u)+Vx(x)⋅g(x,u)]=0V_t(x) + \min_u \left[ f(x, u) + V_x(x) \cdot g(x, u) \right] = 0Vt​(x)+umin​[f(x,u)+Vx​(x)⋅g(x,u)]=0

where V(x)V(x)V(x) is the value function representing the minimum cost-to-go from state xxx, f(x,u)f(x, u)f(x,u) is the immediate cost incurred for taking action uuu, and g(x,u)g(x, u)g(x,u) represents the system dynamics. The equation emphasizes the principle of optimality, stating that an optimal policy is composed of optimal decisions at each stage that depend only on the current state. This makes the HJB equation a powerful tool in solving complex control problems across various fields, including economics, engineering, and robotics.

Dynamic Stochastic General Equilibrium Models

Dynamic Stochastic General Equilibrium (DSGE) models are a class of macroeconomic models that capture the behavior of an economy over time while considering the impact of random shocks. These models are built on the principles of general equilibrium, meaning they account for the interdependencies of various markets and agents within the economy. They incorporate dynamic elements, which reflect how economic variables evolve over time, and stochastic aspects, which introduce uncertainty through random disturbances.

A typical DSGE model features representative agents—such as households and firms—that optimize their decisions regarding consumption, labor supply, and investment. The models are grounded in microeconomic foundations, where agents respond to changes in policy or exogenous shocks (like technology improvements or changes in fiscal policy). The equilibrium is achieved when all markets clear, ensuring that supply equals demand across the economy.

Mathematically, the models are often expressed in terms of a system of equations that describe the relationships between different economic variables, such as:

Yt=Ct+It+Gt+NXtY_t = C_t + I_t + G_t + NX_tYt​=Ct​+It​+Gt​+NXt​

where YtY_tYt​ is output, CtC_tCt​ is consumption, ItI_tIt​ is investment, GtG_tGt​ is government spending, and NXtNX_tNXt​ is net exports at time ttt. DSGE models are widely used for policy analysis and forecasting, as they provide insights into the effects of economic policies and external shocks on

Berry Phase

The Berry phase is a geometric phase acquired over the course of a cycle when a system is subjected to adiabatic (slow) changes in its parameters. When a quantum system is prepared in an eigenstate of a Hamiltonian that changes slowly, the state evolves not only in time but also acquires an additional phase factor, which is purely geometric in nature. This phase shift can be expressed mathematically as:

γ=i∮C⟨ψn(R)∣∇Rψn(R)⟩⋅dR\gamma = i \oint_C \langle \psi_n(\mathbf{R}) | \nabla_{\mathbf{R}} \psi_n(\mathbf{R}) \rangle \cdot d\mathbf{R}γ=i∮C​⟨ψn​(R)∣∇R​ψn​(R)⟩⋅dR

where γ\gammaγ is the Berry phase, ψn\psi_nψn​ is the eigenstate associated with the Hamiltonian parameterized by R\mathbf{R}R, and the integral is taken over a closed path CCC in parameter space. The Berry phase has profound implications in various fields such as quantum mechanics, condensed matter physics, and even in geometric phases in classical systems. Notably, it plays a significant role in phenomena like the quantum Hall effect and topological insulators, showcasing the deep connection between geometry and physical properties.

Pwm Control

PWM (Pulse Width Modulation) is a technique used to control the amount of power delivered to electrical devices, particularly in applications involving motors, lights, and heating elements. It works by varying the duty cycle of a square wave signal, which is defined as the percentage of one period in which a signal is active. For instance, a 50% duty cycle means the signal is on for half the time and off for the other half, effectively providing half the power. This can be mathematically represented as:

Duty Cycle=Time OnTotal Time×100%\text{Duty Cycle} = \frac{\text{Time On}}{\text{Total Time}} \times 100\%Duty Cycle=Total TimeTime On​×100%

By adjusting the duty cycle, PWM can control the speed of a motor or the brightness of a light with great precision and efficiency. Additionally, PWM is beneficial because it minimizes energy loss compared to linear control methods, making it a popular choice in modern electronic applications.