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Mathematics for Quantum Physics
lectures
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b0beddd7
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b0beddd7
authored
4 years ago
by
Scarlett Gauthier
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Add 3 simple practice problems.
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!8
Differential Equations Lecture 1
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...
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@@ -5,12 +5,12 @@ title: Differential Equations
# Differential equations
A differential equation or DE is any equation which involves both a function and some
derivative of that function. In this
co
ur
s
e we will be focusing on
*Ordinary Differential Equations*
, meaning that our equations will involve
derivative of that function. In this
lect
ure we will be focusing on
*Ordinary Differential Equations*
(ODEs)
, meaning that our equations will involve
functions of one independent variable and hence any derivatives will be full
derivatives. Equations which involve a function of several independent variables
and their partial derivatives are
handled in courses on
*Partial Differential Equations*
.
and their partial derivatives are
called
*Partial Differential Equations*
(PDEs). and will
be introduced in the follow up lecture
.
We consider functions $x(t)$ and define $
\d
ot{x}(t)=
\f
rac{dx}{dt}$,
$x^{(n)}(t)=
\f
rac{d^{n}x}{dt^{n}}$. An $n$
*-th*
order differential equation is
...
...
@@ -55,13 +55,13 @@ that unknowns resulting from integration may be determined.
2. If the largest derivative in a differential equation is of first order,
i.e. $n=1$, then the equation is called a first order differential
equation.
3. Often you will see differential equation presented using $y(x)$
3. Often you will see differential equation
s
presented using $y(x)$
instead of $x(t)$. This is just a different nomenclature.
In this course we will be focusing on
*Linear Differential Equations*
, meaning
that we consider differential equations $x^{(n)}(t) = f(x^{(n-1)}(t),
\c
dots, x(t), t)$
where the function $f$ is a linear ploynomial function of the unknown function
$x(t)$. A simple way to spot a non-linear differential euation is to look for
$x(t)$. A simple way to spot a non-linear differential e
q
uation is to look for
non-linear terms, such as $x(t)
*\dot{x}(t)$ or $x^{(n)}(t)*
x^{(2)}(t)$.
Often, we will be dealing with several coupled differential equations. In this
...
...
@@ -772,6 +772,17 @@ $(**A**- \lambda \mathbbm{1})**v**_{i} = **v**_{i-1}$. This completes the proof
since we have demonstrated that $
**\phi**
_{k}(t)$ is a solution of the DE.
# Problems
1.
[:grinning:] Solve the equation $
\d
ot{x}(t)=5x+3$ subject to the initial
condition $x(0)=
\f
rac{2}{5}$.
2.
[:smirk:] Solve the equation $
\d
ot{x}(t)=-tan(x)sin(x)$ subject to the initial
condition $x(0)=1$.
3.
[:smirk:] Solve the equation $
\d
ot{x(t)}=
\f
rac{1}{3} x^2+9$ subject to the
initial condition $x(0)=3$.
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