$(frac{d}{dt} + 2a)int w^2 dx le 0 implies w=0$ where $a>0$












0












$begingroup$


$F(t) := int w^2 dx$ where x is a vector and $a,t>0$



Given that $(frac{d}{dt} - 2a)F(t) le 0$



How do I deduce that $w=0$?



My idea was to do:



$(frac{d}{dt} + 2a)F(t) le 0$



$implies $$frac{d}{dt}F(t) le 2aF(t)$



$implies $$int frac{d}{dt}F(t) le int 2aF(t)$



$implies $$F(t) le int 2aF(t)$



Since $a, F(t) > 0 $ $implies $$int 2aF(t)ge0$



$ implies F(t) le 0$ just realised this line is not true either



Since $F(t) ge 0 implies F(t)=0 implies w=0$



The only line am i not sure about is:



$int frac{d}{dt}F(t) le int 2aF(t)$ $implies $$F(t) le int 2aF(t)$



because there should be a constant of integration introduced somewhere



The soln i was given was that $F(t)$ is bdd above by $G(t)$ where $(frac{d}{dt}-2a)G(t) = 0$ and $G(0)=0$ so $implies G=0$
but since $F(t) le 0 implies F=0 implies w=0$



I cant seem to understand this since answer since G isnt defined explicitly










share|cite|improve this question











$endgroup$












  • $begingroup$
    $G(t)$ is defined expticitly: $G(t) = 0$ for all $t$. What you need to do is to make use of the fact that $G$ is the solution of the differential equation $G' = 2aG$ with $G(0) = 0$ to show that it must also be an upper bound for $F$.
    $endgroup$
    – Paul Sinclair
    Dec 15 '18 at 21:58










  • $begingroup$
    @PaulSinclair but how does G being a soln to that diff eq make it an upper bound for f
    $endgroup$
    – pablo_mathscobar
    Dec 15 '18 at 21:59
















0












$begingroup$


$F(t) := int w^2 dx$ where x is a vector and $a,t>0$



Given that $(frac{d}{dt} - 2a)F(t) le 0$



How do I deduce that $w=0$?



My idea was to do:



$(frac{d}{dt} + 2a)F(t) le 0$



$implies $$frac{d}{dt}F(t) le 2aF(t)$



$implies $$int frac{d}{dt}F(t) le int 2aF(t)$



$implies $$F(t) le int 2aF(t)$



Since $a, F(t) > 0 $ $implies $$int 2aF(t)ge0$



$ implies F(t) le 0$ just realised this line is not true either



Since $F(t) ge 0 implies F(t)=0 implies w=0$



The only line am i not sure about is:



$int frac{d}{dt}F(t) le int 2aF(t)$ $implies $$F(t) le int 2aF(t)$



because there should be a constant of integration introduced somewhere



The soln i was given was that $F(t)$ is bdd above by $G(t)$ where $(frac{d}{dt}-2a)G(t) = 0$ and $G(0)=0$ so $implies G=0$
but since $F(t) le 0 implies F=0 implies w=0$



I cant seem to understand this since answer since G isnt defined explicitly










share|cite|improve this question











$endgroup$












  • $begingroup$
    $G(t)$ is defined expticitly: $G(t) = 0$ for all $t$. What you need to do is to make use of the fact that $G$ is the solution of the differential equation $G' = 2aG$ with $G(0) = 0$ to show that it must also be an upper bound for $F$.
    $endgroup$
    – Paul Sinclair
    Dec 15 '18 at 21:58










  • $begingroup$
    @PaulSinclair but how does G being a soln to that diff eq make it an upper bound for f
    $endgroup$
    – pablo_mathscobar
    Dec 15 '18 at 21:59














0












0








0





$begingroup$


$F(t) := int w^2 dx$ where x is a vector and $a,t>0$



Given that $(frac{d}{dt} - 2a)F(t) le 0$



How do I deduce that $w=0$?



My idea was to do:



$(frac{d}{dt} + 2a)F(t) le 0$



$implies $$frac{d}{dt}F(t) le 2aF(t)$



$implies $$int frac{d}{dt}F(t) le int 2aF(t)$



$implies $$F(t) le int 2aF(t)$



Since $a, F(t) > 0 $ $implies $$int 2aF(t)ge0$



$ implies F(t) le 0$ just realised this line is not true either



Since $F(t) ge 0 implies F(t)=0 implies w=0$



The only line am i not sure about is:



$int frac{d}{dt}F(t) le int 2aF(t)$ $implies $$F(t) le int 2aF(t)$



because there should be a constant of integration introduced somewhere



The soln i was given was that $F(t)$ is bdd above by $G(t)$ where $(frac{d}{dt}-2a)G(t) = 0$ and $G(0)=0$ so $implies G=0$
but since $F(t) le 0 implies F=0 implies w=0$



I cant seem to understand this since answer since G isnt defined explicitly










share|cite|improve this question











$endgroup$




$F(t) := int w^2 dx$ where x is a vector and $a,t>0$



Given that $(frac{d}{dt} - 2a)F(t) le 0$



How do I deduce that $w=0$?



My idea was to do:



$(frac{d}{dt} + 2a)F(t) le 0$



$implies $$frac{d}{dt}F(t) le 2aF(t)$



$implies $$int frac{d}{dt}F(t) le int 2aF(t)$



$implies $$F(t) le int 2aF(t)$



Since $a, F(t) > 0 $ $implies $$int 2aF(t)ge0$



$ implies F(t) le 0$ just realised this line is not true either



Since $F(t) ge 0 implies F(t)=0 implies w=0$



The only line am i not sure about is:



$int frac{d}{dt}F(t) le int 2aF(t)$ $implies $$F(t) le int 2aF(t)$



because there should be a constant of integration introduced somewhere



The soln i was given was that $F(t)$ is bdd above by $G(t)$ where $(frac{d}{dt}-2a)G(t) = 0$ and $G(0)=0$ so $implies G=0$
but since $F(t) le 0 implies F=0 implies w=0$



I cant seem to understand this since answer since G isnt defined explicitly







ordinary-differential-equations multivariable-calculus






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Dec 16 '18 at 11:54







pablo_mathscobar

















asked Dec 15 '18 at 13:45









pablo_mathscobarpablo_mathscobar

996




996












  • $begingroup$
    $G(t)$ is defined expticitly: $G(t) = 0$ for all $t$. What you need to do is to make use of the fact that $G$ is the solution of the differential equation $G' = 2aG$ with $G(0) = 0$ to show that it must also be an upper bound for $F$.
    $endgroup$
    – Paul Sinclair
    Dec 15 '18 at 21:58










  • $begingroup$
    @PaulSinclair but how does G being a soln to that diff eq make it an upper bound for f
    $endgroup$
    – pablo_mathscobar
    Dec 15 '18 at 21:59


















  • $begingroup$
    $G(t)$ is defined expticitly: $G(t) = 0$ for all $t$. What you need to do is to make use of the fact that $G$ is the solution of the differential equation $G' = 2aG$ with $G(0) = 0$ to show that it must also be an upper bound for $F$.
    $endgroup$
    – Paul Sinclair
    Dec 15 '18 at 21:58










  • $begingroup$
    @PaulSinclair but how does G being a soln to that diff eq make it an upper bound for f
    $endgroup$
    – pablo_mathscobar
    Dec 15 '18 at 21:59
















$begingroup$
$G(t)$ is defined expticitly: $G(t) = 0$ for all $t$. What you need to do is to make use of the fact that $G$ is the solution of the differential equation $G' = 2aG$ with $G(0) = 0$ to show that it must also be an upper bound for $F$.
$endgroup$
– Paul Sinclair
Dec 15 '18 at 21:58




$begingroup$
$G(t)$ is defined expticitly: $G(t) = 0$ for all $t$. What you need to do is to make use of the fact that $G$ is the solution of the differential equation $G' = 2aG$ with $G(0) = 0$ to show that it must also be an upper bound for $F$.
$endgroup$
– Paul Sinclair
Dec 15 '18 at 21:58












$begingroup$
@PaulSinclair but how does G being a soln to that diff eq make it an upper bound for f
$endgroup$
– pablo_mathscobar
Dec 15 '18 at 21:59




$begingroup$
@PaulSinclair but how does G being a soln to that diff eq make it an upper bound for f
$endgroup$
– pablo_mathscobar
Dec 15 '18 at 21:59










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