Solutions of certain differential equations in two variablesProve theorem of Existence and Uniqueness of solutions of a $n$-th order differential equation using Picard-Lindelöf theoremDisplacement of differential equationfinding a solution of an autonomous differential equation with two variablesnecessary and sufficient conditions for the existence of solutions.Is it the Picard-Lindelöf Theorem?Is there a harder way to prove that if an integral curve's derivative vanishes then the curve is constant?Boundedness of solutions to a certain system of “weakly-coupled” linear differential equationsEquivalence of two definitions for submanifoldsProperty of solutions of differential equationSmooth map with null differential at each point are constant on the connected component of the domain
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Solutions of certain differential equations in two variables
Prove theorem of Existence and Uniqueness of solutions of a $n$-th order differential equation using Picard-Lindelöf theoremDisplacement of differential equationfinding a solution of an autonomous differential equation with two variablesnecessary and sufficient conditions for the existence of solutions.Is it the Picard-Lindelöf Theorem?Is there a harder way to prove that if an integral curve's derivative vanishes then the curve is constant?Boundedness of solutions to a certain system of “weakly-coupled” linear differential equationsEquivalence of two definitions for submanifoldsProperty of solutions of differential equationSmooth map with null differential at each point are constant on the connected component of the domain
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Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.
How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
$$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$
I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.
ordinary-differential-equations differential-geometry
$endgroup$
add a comment |
$begingroup$
Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.
How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
$$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$
I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.
ordinary-differential-equations differential-geometry
$endgroup$
add a comment |
$begingroup$
Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.
How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
$$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$
I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.
ordinary-differential-equations differential-geometry
$endgroup$
Let $phi:[a,b] to mathbbR^n$ be a smooth function such that $phi(a)=phi(b)=0,$ and let $x,y in mathbbR^n$ be arbitrary points. Suppose we have another fixed smooth path $f: [a,b] to mathbbR^n$.
How do I prove that there always exists a smooth $psi:mathbbR times [a,b] to mathbbR^n$ such that:
$$psi(0,t)= f(t), psi(s,a)=x, psi(s,b)=y$$ and $$fracpartialpartial s psi(0,t)= phi(t)?$$
I would assume to use some version of Picard-Lindelöf, but I do not see how to apply it here.
ordinary-differential-equations differential-geometry
ordinary-differential-equations differential-geometry
asked Mar 17 at 13:04
inequalitynoob2inequalitynoob2
1447
1447
add a comment |
add a comment |
1 Answer
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$begingroup$
This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.
In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.
With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
$$
psi(s,t) = f(t) + sphi(t).
$$
$endgroup$
add a comment |
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1 Answer
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1 Answer
1
active
oldest
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active
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active
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votes
$begingroup$
This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.
In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.
With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
$$
psi(s,t) = f(t) + sphi(t).
$$
$endgroup$
add a comment |
$begingroup$
This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.
In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.
With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
$$
psi(s,t) = f(t) + sphi(t).
$$
$endgroup$
add a comment |
$begingroup$
This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.
In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.
With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
$$
psi(s,t) = f(t) + sphi(t).
$$
$endgroup$
This is not a differential equation. A differential equation would relate the derivative(s) of $psi(s,t)$ to $s$, $t$, and $psi(s,t)$ throughout the domain. Your equations are essentially just boundary conditions and initial conditions for $psi$.
In order to find such a function, you have to stipulate first that $f(a)=x$ and $f(b)=y$; otherwise the conditions are self-contradictory.
With this assumption, there are many such functions, but here's a simple one that you can write down explicitly:
$$
psi(s,t) = f(t) + sphi(t).
$$
answered Mar 17 at 17:44
Jack LeeJack Lee
27.7k54868
27.7k54868
add a comment |
add a comment |
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