Differential Equations › First-Order Differential Equations
Solve the following differential equation
So this is a separable differential equation. The first step is to move all of the x terms (including dx) to one side, and all of the y terms (including dy) to the other side.
So the differential equation we are given is:
Which rearranged looks like:
At this point, in order to solve for y, we need to take the anti-derivative of both sides:
Which equals:
And since this an anti-derivative with no bounds, we need to include the general constant C
So, solving for y, we raise e to the power of both sides:
which, simplified gives us our answer:
Find the general solution of the differential equation
None of the other answers
This is a Bernoulli Equation of the form
which requires a substitution
to transform it into a linear equation
Rearranging our equation gives us
Substituting
Solving the linear ODE gives us
Substituting in and solving for
Find the solution for the following differential equation:
where
.
This equation can be put into the form as follows:
. Differential equations in this form can be solved by use of integrating factor. To solve, take
and solve for
Note, when using integrating factors, the +C constant is irrelevant as we only need one solution, not infinitely many. Thus, we have set C to 0.
Next, note that
Or more simply, . Integrating both sides using substitution of variables we find
Finally dividing by , we see
. Plugging in our initial condition,
So
And .
Find the general solution of the given differential equation and determine if there are any transient terms in the general solution.
First, divide by on both sides of the equation.
Identify the factor term.
Integrate the factor.
Substitute this value back in and integrate the equation.
Now divide by to get the general solution.
The transient term means a term that when the values get larger the term itself gets smaller. Therefore the transient term for this function is .
Solve the general solution for the ODE:
where C is an arbitrary constant
where C is an arbitrary constant
where C is an arbitrary constant
where C is an arbitrary constant
First the differential equation can be separated to:
And then integrated simply to:
Find the general solution of the differential equation
None of the other answers
This is a Bernoulli Equation of the form
which requires a substitution
to transform it into a linear equation
Rearranging our equation gives us
Substituting
Solving the linear ODE gives us
Substituting in and solving for
Find the general solution of the given differential equation and determine if there are any transient terms in the general solution.
First, divide by on both sides of the equation.
Identify the factor term.
Integrate the factor.
Substitute this value back in and integrate the equation.
Now divide by to get the general solution.
The transient term means a term that when the values get larger the term itself gets smaller. Therefore the transient term for this function is .
Find the solution for the following differential equation:
where
.
This equation can be put into the form as follows:
. Differential equations in this form can be solved by use of integrating factor. To solve, take
and solve for
Note, when using integrating factors, the +C constant is irrelevant as we only need one solution, not infinitely many. Thus, we have set C to 0.
Next, note that
Or more simply, . Integrating both sides using substitution of variables we find
Finally dividing by , we see
. Plugging in our initial condition,
So
And .
Solve the general solution for the ODE:
where C is an arbitrary constant
where C is an arbitrary constant
where C is an arbitrary constant
where C is an arbitrary constant
First the differential equation can be separated to:
And then integrated simply to:
Solve the following differential equation
So this is a separable differential equation. The first step is to move all of the x terms (including dx) to one side, and all of the y terms (including dy) to the other side.
So the differential equation we are given is:
Which rearranged looks like:
At this point, in order to solve for y, we need to take the anti-derivative of both sides:
Which equals:
And since this an anti-derivative with no bounds, we need to include the general constant C
So, solving for y, we raise e to the power of both sides:
which, simplified gives us our answer: