What are differential equations and how do you solve ${dy over dx}=y$ and find $y$ in terms $x$?How do you...
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What are differential equations and how do you solve ${dy over dx}=y$ and find $y$ in terms $x$?
How do you solve differential equations in the form of $ay'' + by' +cy = d$?How do you solve second-order linear differential equations without inspection?how to solve second order differential equationFind the maximum area of a right triangle with a constant perimeter P.How do you know when to use the Chain Rule instead of the Power Rule?What method should I apply to solve this differential equation?How to solve differential equations that look like theseSolve System of Differential equations w/o using matrices.How to solve differential equation with one differential termFind the integrating factor and solve
$begingroup$
I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$
ordinary-differential-equations derivatives exponential-function chain-rule
$endgroup$
add a comment |
$begingroup$
I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$
ordinary-differential-equations derivatives exponential-function chain-rule
$endgroup$
1
$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20
2
$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21
$begingroup$
it's variable separable ODE also linear .
$endgroup$
– Faraday Pathak
Mar 10 at 14:26
$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46
$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50
add a comment |
$begingroup$
I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$
ordinary-differential-equations derivatives exponential-function chain-rule
$endgroup$
I had been wondering about how to solve the equation $${dy over dx}=y$$. My progress was to use the chain rule, like setting $$z=2x;{dyover dx}={dyover dz}*{dzover dx}={dyover d(2x)}*2=y.$$ Now I’m officially stuck. What am I supposed to do?
An answer that do work(just for checking): $e^{x+1}$
ordinary-differential-equations derivatives exponential-function chain-rule
ordinary-differential-equations derivatives exponential-function chain-rule
asked Mar 10 at 14:18
Math LoverMath Lover
16010
16010
1
$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20
2
$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21
$begingroup$
it's variable separable ODE also linear .
$endgroup$
– Faraday Pathak
Mar 10 at 14:26
$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46
$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50
add a comment |
1
$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20
2
$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21
$begingroup$
it's variable separable ODE also linear .
$endgroup$
– Faraday Pathak
Mar 10 at 14:26
$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46
$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50
1
1
$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20
$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20
2
2
$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21
$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21
$begingroup$
it's variable separable ODE also linear .
$endgroup$
– Faraday Pathak
Mar 10 at 14:26
$begingroup$
it's variable separable ODE also linear .
$endgroup$
– Faraday Pathak
Mar 10 at 14:26
$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46
$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46
$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50
$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50
add a comment |
4 Answers
4
active
oldest
votes
$begingroup$
This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:
$$
frac{dy}{dx}=y\
frac{1}{y}frac{dy}{dx}=1\
intfrac{1}{y}frac{dy}{dx},dx=int,dx\
intfrac{1}{y},dy=x+C_1\
ln{|y|}+C_2=x+C_1\
ln{|y|}=x+C_1-C_2\
ln{|y|}=x+C_3\
|y|=e^{x+C_3}\
y=pm e^{C_3}e^{x}
$$
$pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:
$$y=Ce^x, Cinmathbb{R}.$$
$endgroup$
add a comment |
$begingroup$
$frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$
$Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$
$C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.
New contributor
$endgroup$
$begingroup$
I corrected $C’e$ to $C’e^x$
$endgroup$
– J. W. Tanner
Mar 10 at 14:45
$begingroup$
My mistake typing it, thank you!
$endgroup$
– Jack Talion
Mar 10 at 14:46
add a comment |
$begingroup$
Here comes a solution without "magical" manipulation of differentials.
Assuming that $y neq 0$ on some interval, divide the equation with $y$:
$$frac{y'(x)}{y(x)} = 1.$$
Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
$$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$
Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
$$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
where $C' = pm e^C$ is a nonzero constant.
We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.
$endgroup$
add a comment |
$begingroup$
The first question in your title is
What are differential equations?
The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
$$
p'(t) = v(t) .
$$
That's just integration. You use any known position to find the "constant of integration".
The differential equation you ask about,
$$
y' = y,
$$
says that the rate of change of $y$ is $y$ itself. In slightly more generality
$$
y' = ky
$$
says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
$$
y = Ce^{kt}.
$$
The second order differential equation
$$
y" = -ky
$$
models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.
$endgroup$
add a comment |
Your Answer
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4 Answers
4
active
oldest
votes
4 Answers
4
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:
$$
frac{dy}{dx}=y\
frac{1}{y}frac{dy}{dx}=1\
intfrac{1}{y}frac{dy}{dx},dx=int,dx\
intfrac{1}{y},dy=x+C_1\
ln{|y|}+C_2=x+C_1\
ln{|y|}=x+C_1-C_2\
ln{|y|}=x+C_3\
|y|=e^{x+C_3}\
y=pm e^{C_3}e^{x}
$$
$pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:
$$y=Ce^x, Cinmathbb{R}.$$
$endgroup$
add a comment |
$begingroup$
This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:
$$
frac{dy}{dx}=y\
frac{1}{y}frac{dy}{dx}=1\
intfrac{1}{y}frac{dy}{dx},dx=int,dx\
intfrac{1}{y},dy=x+C_1\
ln{|y|}+C_2=x+C_1\
ln{|y|}=x+C_1-C_2\
ln{|y|}=x+C_3\
|y|=e^{x+C_3}\
y=pm e^{C_3}e^{x}
$$
$pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:
$$y=Ce^x, Cinmathbb{R}.$$
$endgroup$
add a comment |
$begingroup$
This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:
$$
frac{dy}{dx}=y\
frac{1}{y}frac{dy}{dx}=1\
intfrac{1}{y}frac{dy}{dx},dx=int,dx\
intfrac{1}{y},dy=x+C_1\
ln{|y|}+C_2=x+C_1\
ln{|y|}=x+C_1-C_2\
ln{|y|}=x+C_3\
|y|=e^{x+C_3}\
y=pm e^{C_3}e^{x}
$$
$pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:
$$y=Ce^x, Cinmathbb{R}.$$
$endgroup$
This is a separable differential equation. Assuming $yne0$ which is a condition we will check separately, divide both sides of the equation by $y$:
$$
frac{dy}{dx}=y\
frac{1}{y}frac{dy}{dx}=1\
intfrac{1}{y}frac{dy}{dx},dx=int,dx\
intfrac{1}{y},dy=x+C_1\
ln{|y|}+C_2=x+C_1\
ln{|y|}=x+C_1-C_2\
ln{|y|}=x+C_3\
|y|=e^{x+C_3}\
y=pm e^{C_3}e^{x}
$$
$pm e^{C_3}$ covers all real numbers except $0$. But $y=0$ is also a solution because $0'=0$. Therefore, we can write the following as the general solution to this equation:
$$y=Ce^x, Cinmathbb{R}.$$
edited Mar 11 at 1:08
J. W. Tanner
3,2401320
3,2401320
answered Mar 10 at 16:40
Michael RybkinMichael Rybkin
3,884420
3,884420
add a comment |
add a comment |
$begingroup$
$frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$
$Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$
$C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.
New contributor
$endgroup$
$begingroup$
I corrected $C’e$ to $C’e^x$
$endgroup$
– J. W. Tanner
Mar 10 at 14:45
$begingroup$
My mistake typing it, thank you!
$endgroup$
– Jack Talion
Mar 10 at 14:46
add a comment |
$begingroup$
$frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$
$Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$
$C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.
New contributor
$endgroup$
$begingroup$
I corrected $C’e$ to $C’e^x$
$endgroup$
– J. W. Tanner
Mar 10 at 14:45
$begingroup$
My mistake typing it, thank you!
$endgroup$
– Jack Talion
Mar 10 at 14:46
add a comment |
$begingroup$
$frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$
$Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$
$C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.
New contributor
$endgroup$
$frac{dy}{dx}=yRightarrowfrac{dy}{y}=dxRightarrowintfrac{dy}{y}=int dx$
$Rightarrow lnleft(yright)=x+CRightarrow y=e^{x+C}=C'e^x$
$C$ and $C'=e^{C}$ are constants; in order to put integrals, you should quote the theorem of separation of variables for differential equations.
New contributor
edited Mar 10 at 16:24
J. W. Tanner
3,2401320
3,2401320
New contributor
answered Mar 10 at 14:26
Jack TalionJack Talion
886
886
New contributor
New contributor
$begingroup$
I corrected $C’e$ to $C’e^x$
$endgroup$
– J. W. Tanner
Mar 10 at 14:45
$begingroup$
My mistake typing it, thank you!
$endgroup$
– Jack Talion
Mar 10 at 14:46
add a comment |
$begingroup$
I corrected $C’e$ to $C’e^x$
$endgroup$
– J. W. Tanner
Mar 10 at 14:45
$begingroup$
My mistake typing it, thank you!
$endgroup$
– Jack Talion
Mar 10 at 14:46
$begingroup$
I corrected $C’e$ to $C’e^x$
$endgroup$
– J. W. Tanner
Mar 10 at 14:45
$begingroup$
I corrected $C’e$ to $C’e^x$
$endgroup$
– J. W. Tanner
Mar 10 at 14:45
$begingroup$
My mistake typing it, thank you!
$endgroup$
– Jack Talion
Mar 10 at 14:46
$begingroup$
My mistake typing it, thank you!
$endgroup$
– Jack Talion
Mar 10 at 14:46
add a comment |
$begingroup$
Here comes a solution without "magical" manipulation of differentials.
Assuming that $y neq 0$ on some interval, divide the equation with $y$:
$$frac{y'(x)}{y(x)} = 1.$$
Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
$$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$
Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
$$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
where $C' = pm e^C$ is a nonzero constant.
We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.
$endgroup$
add a comment |
$begingroup$
Here comes a solution without "magical" manipulation of differentials.
Assuming that $y neq 0$ on some interval, divide the equation with $y$:
$$frac{y'(x)}{y(x)} = 1.$$
Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
$$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$
Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
$$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
where $C' = pm e^C$ is a nonzero constant.
We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.
$endgroup$
add a comment |
$begingroup$
Here comes a solution without "magical" manipulation of differentials.
Assuming that $y neq 0$ on some interval, divide the equation with $y$:
$$frac{y'(x)}{y(x)} = 1.$$
Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
$$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$
Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
$$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
where $C' = pm e^C$ is a nonzero constant.
We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.
$endgroup$
Here comes a solution without "magical" manipulation of differentials.
Assuming that $y neq 0$ on some interval, divide the equation with $y$:
$$frac{y'(x)}{y(x)} = 1.$$
Now the left hand side can be written as the derivative of $ln |y(x)|$ and the right hand side as the derivative of $x$:
$$frac{d}{dx} ln |y(x)| = frac{d}{dx} x.$$
Therefore, $ln |y(x)| = x + C,$ where $C$ is some constant, and on the interval we thus have
$$y(x) = pm e^{x+C} = pm e^C e^x = C' e^x,$$
where $C' = pm e^C$ is a nonzero constant.
We can see though that also when $C' = 0,$ we get a solution: $y(x) equiv 0.$ We therefore have a general solution $y(x) = C' e^x,$ where $C'$ is a constant.
answered Mar 10 at 16:50
md2perpemd2perpe
8,19611028
8,19611028
add a comment |
add a comment |
$begingroup$
The first question in your title is
What are differential equations?
The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
$$
p'(t) = v(t) .
$$
That's just integration. You use any known position to find the "constant of integration".
The differential equation you ask about,
$$
y' = y,
$$
says that the rate of change of $y$ is $y$ itself. In slightly more generality
$$
y' = ky
$$
says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
$$
y = Ce^{kt}.
$$
The second order differential equation
$$
y" = -ky
$$
models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.
$endgroup$
add a comment |
$begingroup$
The first question in your title is
What are differential equations?
The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
$$
p'(t) = v(t) .
$$
That's just integration. You use any known position to find the "constant of integration".
The differential equation you ask about,
$$
y' = y,
$$
says that the rate of change of $y$ is $y$ itself. In slightly more generality
$$
y' = ky
$$
says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
$$
y = Ce^{kt}.
$$
The second order differential equation
$$
y" = -ky
$$
models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.
$endgroup$
add a comment |
$begingroup$
The first question in your title is
What are differential equations?
The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
$$
p'(t) = v(t) .
$$
That's just integration. You use any known position to find the "constant of integration".
The differential equation you ask about,
$$
y' = y,
$$
says that the rate of change of $y$ is $y$ itself. In slightly more generality
$$
y' = ky
$$
says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
$$
y = Ce^{kt}.
$$
The second order differential equation
$$
y" = -ky
$$
models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.
$endgroup$
The first question in your title is
What are differential equations?
The informal answer is that often what we know about a quantity we are interested in is its rate of change. For example, if you know the velocity as a function $v(t)$ of time you can find the position $p$ by solving the differential equation
$$
p'(t) = v(t) .
$$
That's just integration. You use any known position to find the "constant of integration".
The differential equation you ask about,
$$
y' = y,
$$
says that the rate of change of $y$ is $y$ itself. In slightly more generality
$$
y' = ky
$$
says that the rate of change of $y$ is proportional to $y$. That classic equation models population growth over time or compound interest: the more stuff there is the faster it's growing. The solution is exponential growth:
$$
y = Ce^{kt}.
$$
The second order differential equation
$$
y" = -ky
$$
models a spring: the second derivative of position is (essentially) a force (that's Newton's law $F=ma$). The equation says that the farther $y$ is from $0$ the greater the force returning it to $0$. The solutions are the oscillating functions $y = sin(t+ phi)$.
answered Mar 11 at 1:28
Ethan BolkerEthan Bolker
45k553120
45k553120
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1
$begingroup$
e$^x$ also works
$endgroup$
– J. W. Tanner
Mar 10 at 14:20
2
$begingroup$
$int {dy over y} = int dx$
$endgroup$
– J. W. Tanner
Mar 10 at 14:21
$begingroup$
it's variable separable ODE also linear .
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– Faraday Pathak
Mar 10 at 14:26
$begingroup$
@J.W.Tanner I know that.
$endgroup$
– Math Lover
Mar 10 at 23:46
$begingroup$
THANKS A LOT FOR YOUR ANSWERS!
$endgroup$
– Math Lover
Mar 10 at 23:50