00:01
Hi there, consider a lake with constant volume v containing at the time t an amount of pollutants given by qt which is evenly distributed throughout the lake with a concentration c t which is equal to qt divided by v.
00:19
Assume that water containing concentration k of pollutants enter the lake at the rate r and that the water leaves the lake at the same rate.
00:29
Suppose that the pollutants are also added directly to the lake with a concentrate p.
00:37
If at time t is equal to 0, the concentration of pollutants was c0, then we want to find the expression of concentration c t.
00:46
By the law of conservation, we can say that the rate of mass accumulation is equal to rate of mass in minus rate of mass out.
01:15
From here we know that the rate of mass in is the sum of rk plus p and the rate of mass out is r multiplied by c t so we have d q divided by d t is equal to rk is equal to rk plus p minus r multiplied by c of t which can be written as r k plus p minus r d divided by v q of t this gives us the differential equation d q divided by d t plus r divided by v q is equal to r k plus p this is a first order linear in homogeneous differential equation and we will solve it by multiplying both sides by the integrating factor i which is given by e raised to the power integral r divided by v d t now since d divided by d x of x is equal to 1 this and by that integral 1 d x will be equal to x so we have i is equal to e raised to the power r t divided by v now we multiply the equation by the integrating factor i and we get e raised to the power r t divided by v d q divided by d t plus e e raise to the power r t divided by d t plus e raise to the power r t the power r t divided by v multiplied by r divided by v multiplied by r divided by q is equal to e to the power r d divided by v multiplied by r k plus p now notice that since d divided by d d of e x to the power r t divided by v of q is equal to by the product rule of differentiation we have d divided by d t e raised to the power r t divided by v multiplied by q plus e r t divided r t divided by v d d t of q which is equal to r d divided by v e raised to the power r t divided by v of q plus e to the power r t divided by v d q divided by d t so we can write the differential equation as d divided by d t of e raised to the power r t divided by v multiplied by q is equal to e raised to the power r t divided by v multiplied by r k plus p so this can be written as d of e raised to the power r t divided by v multiplied by q is equal to e raised to the power r t divided by v multiplied by r k plus e raise to the power r t divided by v multiplied by p t t integrating both sides we get e -raged to the power r t divided by v multiplied by cube is equal to integration is linear we can write it as integral e -raise to the bar r t divided by v multiplied by r k d t plus integral e -raise to the power r t divided by v multiplied by d t since d divided by d x of e raise to the power a x where a sum constant is equal to a, e to the power a x, this implies that integral e raised to the bar a x, dx will be equal to e raised to the bar a x divided by a.
05:58
So we have this equal to e raised to the bar rt divided by v divided by r divided by v multiplied by r k plus e -rae -rae -to -the -par -t divided by v multiplied by p divided by r divided by v plus some constant c so we get e -ra -t to the part r t divided by v multiplied by q will be equal to r divided by r is one kb e -rae -raise to the part r t divided by v plus p v divided by r e raised to the power rt divided by v plus some constant c.
06:46
Now we divide both sides by e raise to the power r2 divided by v and we get q is equal to kv plus pv divided by r plus c multiplied by e raised to the power minus rt divided by v.
07:06
Dividing both sides with the volume b we obtained the concentration c t to be equal to k plus p divided by r plus c divided by v e raised to the power minus r t divided by v now since c of zero is equal to c not we get c not is equal to k plus b divided by r plus c divided by v e raised to the path 0.
07:45
This implies that c divided by v will be equal to c0 minus k minus p divided by r.
07:55
Therefore, concentration at any time t will be given by c of t is equal to k plus p divided by r plus c0 minus k minus p divided by r it divided by e raised to the power minus r t divided by v now we want to know the limiting concentration as t tends towards infinity that will be limit t t tending towards infinity c of t will be equal to limit k tense towards infinity k plus p divided by r plus c0 minus k minus p divided by r multiplied by e raised to the power minus r t divided by p.
08:48
Limit of sum is equal to the sum of limits.
08:51
This will be equal to limit t t t tending towards infinity of k plus limit t t t t t t t t t t turning towards infinity p divided by r plus limit t t t tending towards infinity c not minus k minus p divided by r multiplied by one divided by e x to the power r t divided by v which is equal to k plus p divided by r plus c not minus k minus p divided by r multiplied by 1 divided by infinity which is equal to k plus p divided by r and since 1 divided by infinity is 0 this is 2 plus 0 as t tends towards infinity concentration c of t 10ths towards k plus p divided by r now if the addition of the polluted to the lake is terminated, that is if k is equal to 0 and p is equal to 0, we wish to determine the time interval t that must elapse before the concentration of the pollutants is reduced to 50 % of the original value and when it is reduced to 10 % of its original value.
10:25
Now if the pollution stops then the rate of mass in must be 0.
10:30
So we have rate of mass accumulation is equal to rate of mass in minus rate of mass out.
10:58
And since this is zero, we get dq divided by dt is equal to minus r multiplied by c of d.
11:12
R divided by v or deprived by q of t this implies that dq divided by q is equal to minus r divided by v t t now integrating both sides since d divided by d x of ln x is equal to one divided by x this implies that integral one divided by x v x this implies that integral one divided by x v x is equal to lnx.
11:47
So integral dq divided by q will be lnq which is equal to integral minus r divided by v dt that is minus r divided by vt plus some constant c.
12:05
We can write it as q is equal to e raise to the power minus r divided by v multiplied by t plus c plus c.
12:17
This can be written as e raised to the par c multiplied by e raised to the power minus rt divided by v...