Let's
consider one of the simplest differential equations:
xdx + ydy = 0
One could be understandably tempted to write this in terms of the 1st derivative to obtain:
dy/dx = -x/y
but this serves no useful purpose. It's more productive to directly integrate the equation: xdx = -ydy, viz.
xdx + ydy = 0
One could be understandably tempted to write this in terms of the 1st derivative to obtain:
dy/dx = -x/y
but this serves no useful purpose. It's more productive to directly integrate the equation: xdx = -ydy, viz.
ò x dx = ò-y dy
(since
variables are already separated) to obtain:
x/2 = - y2 / 2 , so
x2 + y2 = c
where c is the constant of integration.
Now, say the particular conditions are such that y = Ö2 when x = Ö2 then:
(Ö2)2 + (Ö2)2 = 2 + 2 = 4
so the particular solution is: x2 + y2 = 4
x/2 = - y2 / 2 , so
x2 + y2 = c
where c is the constant of integration.
Now, say the particular conditions are such that y = Ö2 when x = Ö2 then:
(Ö2)2 + (Ö2)2 = 2 + 2 = 4
so the particular solution is: x2 + y2 = 4
Which is the equation for the circle, e.g.
Now
let's examine a more complex 1st order equation :
Find the general solution and the particular curve passing through the point (0,0) of the differential equation:
exp(x) cos(y) + (1 + exp(x)) sin(y) dy = 0
This looks a bit fearsome, but again, the first rule is simplify, which means separating variables (this is also usually where one's acumen with basic algebra comes in!)
we obtain:
exp(x)/ (1 + exp(x)) + [sin(y)/ cos(y)] dy
=
exp(x)/ (1 + exp(x)) + tan(y)dy = 0
We then integrate: ò (ex)/ (1 + ex) dx = ò tan (y) dy
We then integrate: ò (ex)/ (1 + ex) dx = ò tan (y) dy
To
obtain:
ln(1 + ex) - ln cos(y) = ln c
Or: ln(1 + ex) = ln c + ln cos(y)
where again, c is the constant of integration. We can easily simplify the above (using well known principles of natural logs) to get:
1 + ex = c cos (y)
Which is the general solution.
To get the particular solution we need to substitute the ordered pair values for (0,0) into the general solution, whence:
1 + e0 = c(cos (0))
so that: 1 + 1 = c
and c = 2 , then we get: 1 + ex = 2 cos (y)
ln(1 + ex) - ln cos(y) = ln c
Or: ln(1 + ex) = ln c + ln cos(y)
where again, c is the constant of integration. We can easily simplify the above (using well known principles of natural logs) to get:
1 + ex = c cos (y)
Which is the general solution.
To get the particular solution we need to substitute the ordered pair values for (0,0) into the general solution, whence:
1 + e0 = c(cos (0))
so that: 1 + 1 = c
and c = 2 , then we get: 1 + ex = 2 cos (y)
Problems:
1)Show that y = cx2
- x is a solution of the DE:
xy'
= 2y + x
2)
Show that y = (2x + c) exp(-x) is a solution of the DE: dy/dx + y = 2 exp(-x)
3) For the differential equation: dy/dx = -x/4y , sketch the curve which passes through the point (1,1)
4) Find the general solution of: sin (t) dp + p cos(t) dt = 0
5) Find the particular solution for the equation:
3) For the differential equation: dy/dx = -x/4y , sketch the curve which passes through the point (1,1)
4) Find the general solution of: sin (t) dp + p cos(t) dt = 0
5) Find the particular solution for the equation:
exp(x)
sec(y)dx + (1 + ex) sec (y) tan(y) dy = 0
with y = 60 deg when x = 3
with y = 60 deg when x = 3
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