StudySmarter: Study help & AI tools

4.5 • +22k Ratings

More than 22 Million Downloads

Free

System of Differential Equations

Dive into the intricate world of Engineering Mathematics with this comprehensive guide to the System of Differential Equations. Providing in-depth insights and practical understanding, this exposition covers everything from the basic meaning of System of Differential Equations and its importance in the field of engineering, to its numerous practical applications. Learn the techniques to solve it systematically and discover the features of different types such as an autonomous system and coupled system. Moreover, understand the Euler Method's uniqueness for solving System of Differential Equations.

Explore our app and discover over 50 million learning materials for free.

- Design Engineering
- Engineering Fluid Mechanics
- Engineering Mathematics
- Acceptance Sampling
- Addition Rule of Probability
- Algebra Engineering
- Application of Calculus in Engineering
- Area under curve
- Basic Algebra
- Basic Derivatives
- Basic Matrix Operations
- Bayes' Theorem
- Binomial Series
- Bisection Method
- Boolean Algebra
- Boundary Value Problem
- CUSUM
- Cartesian Form
- Causal Function
- Centroids
- Cholesky Decomposition
- Circular Functions
- Complex Form of Fourier Series
- Complex Hyperbolic Functions
- Complex Logarithm
- Complex Trigonometric Functions
- Conservative Vector Field
- Continuous and Discrete Random Variables
- Control Chart
- Convergence Engineering
- Convergence of Fourier Series
- Convolution Theorem
- Correlation and Regression
- Covariance and Correlation
- Cramer's rule
- Cross Correlation Theorem
- Curl of a Vector Field
- Curve Sketching
- D'alembert Wave Equation
- Damping
- Derivative of Polynomial
- Derivative of Rational Function
- Derivative of a Vector
- Directional Derivative
- Discrete Fourier Transform
- Divergence Theorem
- Divergence Vector Calculus
- Double Integrals
- Eigenvalue
- Eigenvector
- Engineering Analysis
- Engineering Graphs
- Engineering Statistics
- Euler's Formula
- Exact Differential Equation
- Exponential and Logarithmic Functions
- Fourier Coefficients
- Fourier Integration
- Fourier Series
- Fourier Series Odd and Even
- Fourier Series Symmetry
- Fourier Transform Properties
- Fourier Transform Table
- Gamma Distribution
- Gaussian Elimination
- Half Range Fourier Series
- Higher Order Integration
- Hypergeometric Distribution
- Hypothesis Test for a Population Mean
- Implicit Function
- Improved Euler Method
- Interpolation
- Inverse Laplace Transform
- Inverse Matrix Method
- Inverse Z Transform
- Jacobian Matrix
- Laplace Shifting Theorem
- Laplace Transforms
- Large Sample Confidence Interval
- Least Squares Fitting
- Logic Gates
- Logical Equivalence
- Maths Identities
- Maxima and Minima of functions of two variables
- Maximum Likelihood Estimation
- Mean Value and Standard Deviation
- Method of Moments
- Modelling waves
- Multiple Regression
- Multiple Regression Analysis
- Newton Raphson Method
- Non Parametric Statistics
- Nonlinear Differential Equation
- Nonlinear Regression
- Numerical Differentiation
- Numerical Root Finding
- One Way ANOVA
- P Value
- Parseval's Theorem
- Partial Derivative
- Partial Derivative of Vector
- Partial Differential Equations
- Particular Solution for Differential Equation
- Phasor
- Piecewise Function
- Polar Form
- Polynomial Regression
- Probability Engineering
- Probability Tree
- Quality Control
- RMS Value
- Radians vs Degrees
- Rank Nullity Theorem
- Rank of a Matrix
- Reliability Engineering
- Runge Kutta Method
- Scalar & Vector Geometry
- Second Order Nonlinear Differential Equation
- Simple Linear Regression Model
- Single Sample T Test
- Standard Deviation of Random Variable
- Superposition
- System of Differential Equations
- System of Linear Equations Matrix
- Taylor's Theorem
- Three Way ANOVA
- Total Derivative
- Transform Variables in Regression
- Transmission Line Equation
- Triple Integrals
- Triple Product
- Two Sample Test
- Two Way ANOVA
- Unit Vector
- Vector Calculus
- Wilcoxon Rank Sum Test
- Z Test
- Z Transform
- Z Transform vs Laplace Transform
- Engineering Thermodynamics
- Materials Engineering
- Professional Engineering
- Solid Mechanics
- What is Engineering

Lerne mit deinen Freunden und bleibe auf dem richtigen Kurs mit deinen persönlichen Lernstatistiken

Jetzt kostenlos anmeldenNie wieder prokastinieren mit unseren Lernerinnerungen.

Jetzt kostenlos anmeldenDive into the intricate world of Engineering Mathematics with this comprehensive guide to the System of Differential Equations. Providing in-depth insights and practical understanding, this exposition covers everything from the basic meaning of System of Differential Equations and its importance in the field of engineering, to its numerous practical applications. Learn the techniques to solve it systematically and discover the features of different types such as an autonomous system and coupled system. Moreover, understand the Euler Method's uniqueness for solving System of Differential Equations.

In a journey through the complex yet intriguing world of Engineering Mathematics, you come across different concepts. One of these concepts is the System of Differential Equations. Let's dive into this exciting topic.

A system of differential equations is a collection of two or more correlated differential equations. A solution to this system is a function or a set of functions that satisfies each equation in the set simultaneously.

Formally, given a system of \( n \) differential equations, if \( x_1(t),x_2(t),...,x_n(t) \) are functions of a variable \( t \) such that these functions and their derivatives satisfy all the equations, it is considered as a solution of the System of Differential Equations.

Here's a simple example to illustrate this:

Consider the system of differential equations:

dy/dt = y + z dz/dt = z - yIn this case, a possible solution might be:

y = e^t z = e^tAs each of these functions and their derivatives would satisfy all the equations of the system.

A single differential equation is defined by the relation involving a function and its derivatives. On the other hand, a system of differential equations is a set of two or more related differential equations containing the same variables and derivatives.

For instance, \( dx/dt = x+y \) is a single differential equation while \( dx/dt = x+y \) and \( dy/dt = x-y \) comprise a System of Differential Equations.

The understanding of System of Differential Equations holds significant importance in the engineering field. They are used to model multi-variable systems. Such systems can include mechanical systems like transportation models, electrical circuits, or ecological systems, to name just a few. The solutions to the system of equations provide insight into the system's general behaviour and allow engineers to control and optimize these systems.

For instance, in electrical engineering, solving a system of differential equations can yield the currents and voltages in an electrical circuit, providing crucial insights for the design, operation, and maintenance of these circuits.

Often in engineering mathematics, you'll encounter the necessity to solve a system of differential equations. The process can seem challenging, but don't worry - we will break it down for you, step by step. It's worth mentioning that methods may vary based on the type of the system, such as whether it's linear or non-linear, homogeneous or non-homogeneous.

The method of solving a system of differential equations greatly depends on its properties, but we'll outline a general approach that you may follow.

- Identify the Type of System: First, discern if the system is linear or non-linear, and whether it's homogeneous or non-homogeneous. This will determine the method used for solving it.
- Create a Matrix: If the system of equations is linear, write it in matrix form. This will allow the use of matrix methods to solve the system.
- Solve for Eigenvalues: If solving a linear system, next, find the eigenvalues of the matrix.
- Solve for Eigenvectors: Once you've found the eigenvalues, use them to solve for eigenvectors.
- Create the General Solution: Combining the eigenvalues and eigenvectors, construct the general solution to the system.
- Initial Conditions: If initial conditions are given, substitute them into the general solution to find the particular solution.

Remember that when the system is not linear, or the linear system has no eigenvalues, different methods - often involving numerical approximations - will be required.

Linear systems of differential equations are simplified when written in matrix form. This approach permits the use of eigenvalues and eigenvectors to construct the general solution.

For example, consider the system of equations:

\[\frac{dx}{dt} = 5x - 3y \]

\[\frac{dy}{dt} = 3x + 2y\]

This is a linear system, and the matrix form is \( A = \begin{bmatrix} 5 & -3 \\ 3 & 2\end{bmatrix} \). Solving for the eigenvalues and eigenvectors will provide the elements necessary to construct the general solution.

In contrast, non-linear systems present a higher level of complexity and require alternate approaches such as numerical approximation methods like Euler's method.

Let's consider a non-linear system like:

\[ \frac{dx}{dt} = x^2 - y \]

\[ \frac{dy}{dt} = x + y^2 \]This system cannot be directly written in matrix form or solved using the eigenvalue-eigenvector method. Instead, numerical methods are employed to obtain an approximate solution.

Homogeneous and non-homogeneous systems distinguish themselves by whether or not the system has constant terms. In a homogeneous system, there are no constant terms.

A homogeneous system may be written as \( \frac{d(x)}{dt} = A*x \), where A is a matrix, and x is a vector of functions. The homogeneous system's general solution will be a combination of terms \( e^{\lambda t}v \), where \( \lambda \) is an eigenvalue, and \( v \) is the corresponding eigenvector.

A non-homogeneous system, on the other hand, will include constant terms,such as \( \frac{d(x)}{dt} = A*x + B \), where B is a vector of constants. For such systems, you will seek the particular solution and the homogeneous solution, then combine these two for the general solution.

Given the system:

\[\frac{dx}{dt} = 5x - 3y + 2\]

\[\frac{dy}{dt} = 3x + 2y + 1\]The system is non-homogeneous. The particular solution will often be a constant vector, and it may be found by setting the system in equilibrium (setting the derivatives equal to zero and solving the resulting system of algebraic equations). If the particular solution is \( x_p \), and the solution to the corresponding homogeneous system is \( x_h \), the general solution of the system will be \( x = x_h + x_p \).

By understanding these distinctions, you'll become more proficient in solving systems of differential equations, and primarily in how these solutions are applied in engineering mathematics.

Now that you have a strong understanding of the concept, types, and solutions of System of Differential Equations, let's delve into various examples that will deepen your comprehension and learning about their application in real-world contexts, specifically within the field of engineering.

In the field of engineering, the use of the system of differential equations is ubiquitous. We shall explain, through detailed examples and calculations, how these equations serve as the fundamental element driving numerous applications such as mechanical systems, electrical circuits, and even chemical reactions.

Starting with a classic mechanical application, let's consider a **mass-spring-damper system** represented by a system of differential equations. Such a system could represent a vehicle suspension, where the damper is the shock absorber, the spring is the car's body, and the mass is the vehicle itself. The motion of the system can be commonly described as:

\[ m\frac{d^2x}{dt^2} + b\frac{dx}{dt} + kx = 0 \]where:

- \( m \) is the mass of the vehicle.
- \( b \) is the damping coefficient, related to the shock absorber.
- \( k \) is the spring constant, related to the stiffness of the car body.
- \( x \) is the displacement from the equilibrium position.

**In electrical engineering**, the analysis of **RLC circuits**(Resistor, Inductor, Capacitor) often involves solving a system of differential equations. For instance, for a series RLC circuit governed by Kirchhoff’s voltage law (KVL), the differential equation can be written as:

\[ L\frac{d^2q}{dt^2} + R\frac{dq}{dt} + \frac{q}{C} = V \]where:

- \( L \) is the inductance,
- \( R \) is the resistance,
- \( C \) is the capacitance,
- \( q \) is the charge on the capacitor,
- \( V \) is the applied voltage.

To illustrate further, let's take a closer look at how we can solve these system of differential equations with some practical examples.

Let’s consider a **predator-prey model** that describes the interaction of two species in an ecosystem, for example, foxes (predators) and rabbits (prey). We denote the population of rabbits by \( x \) and foxes by \( y \).The system can be represented as:

\[ \frac{dx}{dt} = ax - bxy \]

\[ \frac{dy}{dt} = -cy + dxy \]where:

- \( a, b, c, \) and \( d \) are constants that represent the reproduction rate of rabbits, the rate of predation on rabbits, the natural death rate of foxes, and the increase in fox population due to abundant food, respectively.

A more advanced engineering example would be a drone following a certain path in space. A **quadrotor drone** has four propellers, and the control of these can get quite complex. The motion along one axis can be represented by a system of differential equations.Let's denote the displacement by \( x \), velocity by \( v \), and acceleration by \( a \). The state-space representation of the system could be:

\[ \frac{dx}{dt} = v \]

\[ \frac{dv}{dt} = a \]

\[ \frac{da}{dt} = u \]where:

- \( u \) is the control input, which would be a combination of the thrusts of the different propellers.

These examples offer a glimpse into the diverse applications of System of Differential Equations in the realm of engineering - composing the basic framework for understanding and solving real-world engineering problems. Indeed, the practical value of mastering this mathematical tool couldn't be overstated.

Autonomous systems of differential equations find extensive application in many varied scientific disciplines such as physics, chemistry, biology, economics, and engineering. These systems are defined by equations that depend solely on the state variable and not explicitly on an independent variable like time.

A system of differential equations is termed **autonomous** when the equations composing the system are independent of the independent variable, often time, in the problem under consideration. In simpler terms, the behaviour of the dynamical system described by autonomous equations doesn't change over time, which dramatically simplifies the analysis and understanding of the system's dynamics.

Said differently, for a first-order ordinary differential equation (ODE), the standard form is:

\[ \frac{dx}{dt} = f(t, x) \]However, in an autonomous ODE, the function \( f \) doesn't rely on \( t \) and only depends on \( x \). Thus, an autonomous first-order ODE can be written as:

\[ \frac{dx}{dt} = f(x) \]Consider an autonomous system of two first-order ODEs. Such a system would have the following form:

\[ \frac{dx}{dt} = f(x, y) \]

\[ \frac{dy}{dt} = g(x, y) \]Here \( f(x, y) \) and \( g(x, y) \) are functions of \( x \) and \( y \), but not of \( t \).

The advantage of studying autonomous systems arises from the fact they often possess invariant properties over time, allowing for more straightforward analysis of their long-term behaviour through the concept of equilibrium points and phase portrait analysis.

The behaviour of an autonomous system of differential equations is typically studied by examining its **equilibrium points** and sketching its **phase portrait**. The analysis is usually aimed at determining the system's stability, which is crucial in numerous fields like control systems in engineering, ecological modelling, economics, among others.

Equilibrium points, also known as critical or stationary points, are solutions to the system of equations \( f(x, y) = 0 \) and \( g(x, y) = 0 \). These points represent states of the system where it ceases to change, thus the name equilibrium.

To effectively study the behaviour of the autonomous system, it's often plotted on a phase plane, a two-dimensional space with axes representing the state variables of the system. Each point in this phase plane then corresponds to a unique state of the system.

Consider the autonomous system represented by these equations:

\[ \frac{dx}{dt} = x(3 - y) \]

\[ \frac{dy}{dt} = y(2 - x) \]To find the equilibrium points, we solve for \( x \) and \( y \) when the above expressions are equal to 0. The solutions will be \( (x, y) = (0, 0), (3, 2) \).

The phase portrait is then sketched by drawing numerous solution curves (trajectories), each representing the solution starting from a different initial condition. Analysing these trajectories near the equilibrium points reveals the local behaviour of the system, namely whether the system is stable, unstable or neutral at these points.

For example, trajectories converging to an equilibrium point indicate a stable system at that point. On the contrary, trajectories diverging from an equilibrium point point towards an unstable system.

In summary, the autonomous system of differential equations is a powerful mathematical framework used to describe various dynamical systems. Its strength lies in its independence from the time variable, leading to exploration of the intrinsic behaviour of the system and allowing comprehensive understanding of natural and human-made systems.

A coupled system of differential equations, often central in engineering and physics, is inherently different than isolated differential equations. Let's delve into the concept, definition, and evaluation methods for a better understanding.

A system of differential equations is said to be **coupled** when one or more dependent variables and their derivatives occur in more than one equation. In other words, the equations are interconnected, with their solutions being dependent on each other.

Consider two differential equations, given by \( \frac{dx}{dt} = f(t, x, y) \) and \( \frac{dy}{dt} = g(t, x, y) \). These constitute a system of differential equations. This system is said to be coupled if the right-hand-side function \( f \) of the first equation involves the variable \( y \), or if the function \( g \) of the second equation involves the variable \( x \). If this is not the case, the system is said to be decoupled.

In a coupled system of differential equations, the differential equation that governs the behaviour of one component also depends on the other components. This interdependence calls for more complex methods of solution compared to decoupled systems, where each equation can be solved independently.

Coupled differential equations are frequently encountered in practical scenarios, such as mechanics where position, velocity, and acceleration are usually coupled, electronic circuits with multiple connected elements, and in social and life sciences to model interacting populations or economic systems, to name just a few.

Solving coupled systems of differential equations requires some careful steps and powerful mathematical techniques, often involving the transformation of the system into an equivalent but simpler system.

**For linear systems**, the primary techniques are:

**Elimination method**: This involves expressing one dependent variable in one equation in terms of other variables and their derivatives and substituting into the other equation to create a single equation with one dependent variable.**Matrix method**: It particularly becomes useful when dealing with systems of three or more linear differential equations. The system is written in matrix form, and then eigenvalues and eigenvectors of the system matrix are computed to derive the solutions.

However, coupled **non-linear differential equations** pose bigger challenges. Exact solutions are often difficult if not impossible to obtain. Analytical approaches such as the method of substituted variables or perturbation methods could be used. When these are infeasible, numerical methods such as Euler's method, Runge-Kutta methods, or specialized software like MATLAB or Mathematica® come into play.

For instance, consider the simple coupled system:

\[ \begin{align*} \frac{dx}{dt} &= y - x, \\ \frac{dy}{dt} &= x - y. \end{align*} \]Subtracting both equations gives \( \frac{dy}{dt} - \frac{dx}{dt} = 0 \), which can be integrated directly to yield \( y - x = C \) for some constant \( C \). Replacing \( y \) in the first differential equation, we get \( \frac{dx}{dt} = C \). Integrating this results in \( x = Ct + D \) for some constant \( D \). Finally, replace \( x \) in \( y - x = C \) to get \( y = Ct + D + C \). Hence, the system is solved.

The process of solving coupled systems of differential equations, therefore, requires a deep understanding of mathematical methods and sometimes computational tools. These systems, despite their complexity, are competent to describe numerous real-world phenomena with interconnected variables, thus incredibly critical to the disciplines of science and engineering.

While exploring the fascinating realm of differential equations, you'll encounter one of the earliest and simplest numerical methods for approximating solutions: the Euler method. Named after the Swiss mathematician Leonhard Euler, this method is a first-order numerical procedure for solving ordinary differential equations (ODEs) with a given initial value.

The general idea of the Euler method is to use the derivative at a particular point to approximate the value of the function at the next point. This method relies on the concept of local linearity, under which a function at a particular point is taken to be roughly linear, thus making the slope of the tangent at that point a reasonable approximation of the function's value at a point nearby.

The Euler method is fairly straightforward to implement. For a first-order differential equation \( \frac{dx}{dt} = f(t, x) \) with an initial condition \( x(t_0) = x_0 \), the method generates a sequence of approximations to the actual solution via the following iterative formula:

\[ x(t + h) = x(t) + h \cdot f(t, x(t)) \]

where \( h \) is a small, chosen step size. The new function value \( x(t + h) \) is thus a mini-step \( h \) away from \( x(t) \), with the mini-step in the direction of the slope \( f(t, x(t)) \) at the current point \( x(t) \).

This process is reiterated for each next time step, making Euler's method an example of a step-by-step (or single-step) method. An important detail to note is that the approximation accuracy of the Euler method is directly correlated to the size of the step \( h \) used. The smaller the step size, the closer the approximation to the actual solution, but the more computations are needed.

for(int i=0; i<n; i++) { x[i+1] = x[i] + h*f(t[i], x[i]); }

The above pseudo-code shows the standard Euler method as applied in a computer algorithm, where \( h \) (the step size), \( f \) (the right-hand-side function of the ODE), \( n \) (the total number of steps), and \( x[0] = x_0 \) (the initial condition) have been previously defined.

Take this for example: let's solve the first-order ODE \( \frac{dx}{dt} = 3x - 2t \) with the initial condition \( x(0) = 1 \), using an Euler method with a step size \( h = 0.2 \). Starting at \( t_0 = 0, x_0 = 1 \), we find \( x_1 = x_0 + h \cdot f(t_0, x_0) = 1 + 0.2 \cdot (3 \cdot 1 - 2 \cdot 0) = 1.6 \), which is the Euler method approximation at \( t_1 = 0.2 \). This process is then repeated for each subsequent time \( t \).

There are, of course, multiple numerical strategies for approximating solutions to differential equations. Each approach offers distinct advantages and certain drawbacks in comparison with the Euler method.

The following techniques, for instance, are notable:

**Improved (or Modified) Euler's Method**: More sophisticated than the original Euler's method, it calculates a more accurate slope at each step by taking the average of the initial slope and the slope at the estimated next point.**Midpoint Method**: It approximates the value of the solution at a mid-point between two time steps to better estimate the slope at the current point, often yielding more accuracy than the basic Euler method for a similar computational effort.**Runge-Kutta Methods**: These include a variety of techniques that estimate the slope at several points within a time step. The fourth-order Runge-Kutta method, often simply referred to as RK4, is the most widely used due to its excellent balance between computational effort and accuracy.

Table comparing Euler and other methods:

Method | Accuracy | Computational Effort |

Euler Method | Low | Low |

Improved Euler's Method | Moderate | Moderate |

Midpoint Method | Moderate | Moderate |

Runge-Kutta (RK4) Method | High | High |

While the Euler Method may lag behind more advanced techniques in accuracy and stability, especially for larger step sizes or more complex differential equations, its simplicity, ease of understanding and implementation make it a good starting point for any numerical analysis of differential equations. It ensures a decent enough approximation for mildly complex equations, particularly when smaller step sizes are utilised. It also serves as a solid foundation for learning more advanced numerical methods.

- System of Differential Equations: A system of equations where the unknowns are functions, rather than simple variables.
- Solving Homogeneous/Non-Homogeneous Systems: In a homogeneous system, there are no constant terms. In a non-homogeneous system, constant terms are included. The solutions comprise both particular and homogeneous solutions.
- Engineering Applications of System of Differential Equations: These systems are used to model various physical phenomena such as mechanical systems, electrical circuits, etc.
- Autonomous System of Differential Equations: These systems don't depend explicitly on an independent variable like time, simplifying the analysis and understanding of the system's dynamics.
- Coupled System of Differential Equations: In these systems, one or more dependent variables and their derivatives occur in more than one equation, meaning the equations are interconnected, with their solutions being dependent on each other.

To solve a System of Differential Equations, one can use several methods such as elimination, substitution, or matrix algebra. For linear systems, methods like Eigenvalue-Eigenvector technique or Laplace Transforms can be used. Numerical methods might be essential for complex or non-linear systems.

To solve a system of linear differential equations, you first write the system in matrix form. Then, find the system's eigenvalues and eigenvectors. Use these to form the general solution. The specific solution can be found by applying any initial conditions.

Systems of Differential Equations are a set of multiple related differential equations that contain more than one unknown function. They model situations where the rate of change of variables depends on the current state of the variables themselves.

To solve a system of coupled differential equations, you can use methods such as substitution, elimination, or matrix methods. These involve expressing the system of equations in matrix form and then applying numerical methods such as Euler's or Runge-Kutta methods. Software like MATLAB or Python's SciPy library can also be used.

Solving a system of partial differential equations (PDEs) usually involves the use of separation of variables, Fourier series, Laplace transforms, or numerical methods. It often requires classifying the PDE into hyperbolic, elliptic or parabolic and then applying the appropriate method.

What is a system of differential equations?

A system of differential equations is a collection of two or more correlated differential equations. A solution to this system is a function or a set of functions that satisfies each equation in the set simultaneously.

What is the significance of system of differential equations in engineering mathematics?

System of differential equations are used to model multi-variable systems in engineering like transportation models, electrical circuits, or ecological systems. The solutions provide insight into the system's general behaviour and allow engineers to control and optimize these systems.

What is the step-by-step guide to solve system of differential equations?

Step one, identify if the system is linear or non-linear, and whether it's homogeneous or non-homogeneous. Step two, if the system is linear, write it in matrix form. Step three, if it's a linear system, find the eigenvalues of the matrix, then solve for eigenvectors. Step five, create the general solution by combining eigenvalues and eigenvectors. Lastly, substitute initial conditions into the general solution to find the particular solution.

How do homogeneous and non-homogeneous system of differential equations differ?

Homogeneous systems do not have constant terms and can be written as \( \frac{d(x)}{dt} = A*x \), where A is a matrix. Non-homogeneous systems include constant terms and can be written as \( \frac{d(x)}{dt} = A*x + B \), where B is a vector of constants. For non-homogeneous systems, you seek the particular solution and the homogeneous solution, then combine these.

What is a practical application of a system of differential equations in mechanical engineering?

A system of differential equations can be used to represent a mass-spring-damper system in mechanical engineering, such as a vehicle suspension. The equation is \( m\frac{d^2x}{dt^2} + b\frac{dx}{dt} + kx = 0 \), where 'm' is the mass of the vehicle, 'b' is the damping coefficient, 'k' is the spring constant, and 'x' is the displacement from equilibrium. The solution can predict the system's behaviour.

How are systems of differential equations used in electrical engineering?

Systems of differential equations are used to analyze Resistor, Inductor, Capacitor (RLC) circuits in electrical engineering. The equation \( L\frac{d^2q}{dt^2} + R\frac{dq}{dt} + \frac{q}{C} = V \), where 'L' is the inductance, 'R' is the resistance, 'C' is the capacitance, 'q' is the charge on the capacitor, and 'V' is the applied voltage, helps define how the charge, current and voltages in the circuit change with time.

Already have an account? Log in

Open in App
More about System of Differential Equations

The first learning app that truly has everything you need to ace your exams in one place

- Flashcards & Quizzes
- AI Study Assistant
- Study Planner
- Mock-Exams
- Smart Note-Taking

Sign up to highlight and take notes. It’s 100% free.

Save explanations to your personalised space and access them anytime, anywhere!

Sign up with Email Sign up with AppleBy signing up, you agree to the Terms and Conditions and the Privacy Policy of StudySmarter.

Already have an account? Log in