F
Fred Bloggs
Guest
sert wrote:
.
.
.
.
. i
. ->
. .----------. v= i x R
. | ^ |
. | | | d 3
. +| | | and i= - -- (3 x v )
. --- / dt
. C --- v \ R
. | / 2 dv
. | | \ so v = -9 x R x v x --
. | | | dt
. | | |
. '----------.
.
.
. 2 dv dv
. this becomes v + 9 x R x v x -- = v x ( 1 + 9 x R x v x -- )=0
. dt dt
.
. at each instant of time because although C is nonlinear the basic
.
.
. laws of physics still apply to the circuit.
.
.
. The above equation has only two possible solutions:
.
.
. 1) v(t)=0 for all t, which is ruled out because we need v(0)=1
.
. --------------
. | 2
. 2) v(t)= | 1 - ----- x t
. \| 9 x R
.
.
.
. 9 x R dv
. at time t= ----- v=0, the v x ( 1 + 9 x R x v x -- )=0
. 2 dt
.
. 9 x R
. equation still applies where t is now measured from -----
. 2
.
. and since v(0)=0 the v(t)=0 solution does
.
. dv
. apply, and the 1 + 9 x R x v x -- = 0 solution leads to an
. dt
.
. an imaginary and extraneous result.
.
.
. All of this can be condensed into:
.
.
.
. ----------------------
. | 2
. v(t)= | MAX(0,1 - ----- x t) t>=0
. \| 9 x R
.
.
View in a fixed-width font such as Courier.Fred Bloggs <nospam@nospam.com> wrote in
news:484C6008.5070809@nospam.com:
View in a fixed-width font such as Courier.
.
--------------
. 9 2 | 2
. or t = - - x R x (v - 1) from which v = | 1 -
----- x t . 2
\| 9 x R .
.
Thanks. But there's something unusual going on; the capacitor is
discharging completely. A linear capacitor, as we know, never
discharges completely.
Also, for values of t over a certain threshold the formula is
undefined.
Let's assume that the capacitor will discharge completely as the
formula suggests. Surely the time t will continue (time will not
stop!) but the formula doesn't actually give v=0 for any t after
the discharging, it's simply undefined.
Why? Is there some other non-obvious solution to the DE?
.
.
.
.
. i
. ->
. .----------. v= i x R
. | ^ |
. | | | d 3
. +| | | and i= - -- (3 x v )
. --- / dt
. C --- v \ R
. | / 2 dv
. | | \ so v = -9 x R x v x --
. | | | dt
. | | |
. '----------.
.
.
. 2 dv dv
. this becomes v + 9 x R x v x -- = v x ( 1 + 9 x R x v x -- )=0
. dt dt
.
. at each instant of time because although C is nonlinear the basic
.
.
. laws of physics still apply to the circuit.
.
.
. The above equation has only two possible solutions:
.
.
. 1) v(t)=0 for all t, which is ruled out because we need v(0)=1
.
. --------------
. | 2
. 2) v(t)= | 1 - ----- x t
. \| 9 x R
.
.
.
. 9 x R dv
. at time t= ----- v=0, the v x ( 1 + 9 x R x v x -- )=0
. 2 dt
.
. 9 x R
. equation still applies where t is now measured from -----
. 2
.
. and since v(0)=0 the v(t)=0 solution does
.
. dv
. apply, and the 1 + 9 x R x v x -- = 0 solution leads to an
. dt
.
. an imaginary and extraneous result.
.
.
. All of this can be condensed into:
.
.
.
. ----------------------
. | 2
. v(t)= | MAX(0,1 - ----- x t) t>=0
. \| 9 x R
.
.