00:01
So we're given the differential equation of d t over t equal to k of m minus t.
00:10
I write, we write this as d t over d t equal to minus k.
00:18
I pull out a minus and i have t minus m.
00:22
This is just the same thing.
00:24
Now i separate these and i have d t over t minus.
00:30
Minus m equal to minus k multiplied by d t now let's take the integral of both sides you will have that the integral of this will just be the natural log of absolute value of t minus m equal to when you integrate these k is a constant so you have minus k t and then let me add plus c one the next thing we do is that we take the exponential of both sides.
01:01
So i have e and i have e.
01:04
So that gives me that this will cancel out.
01:07
I have that t minus m equal to e to the minus kt multiply by e to the c1, which is equal to if i take this e to the c1 is a constant, so i can name that c2.
01:23
So i have c2, e to the minus kt.
01:27
So that implies that absolute value of t minus m equal to c2 e minus k t, which implies that t minus m equal to plus or minus of c2 e minus kt.
01:44
This implies that t equal to m plus c e minus k t, where c equal to plus c e minus k t, where c equal to plus a minus of.
01:57
Of c2.
01:59
So let's name this equation star.
02:01
We're going to use it later on.
02:03
Now the b parts we're given that the constant temperature m equal to 70 degrees.
02:12
We're given t at zero equal to 100 degrees.
02:17
We're given t at 6 equal to 80 degrees and we want to find t at 20.
02:26
That's what we're looking for.
02:28
Now plug this into equation star, plugging into star, the equation star we got.
02:36
So we have that t at zero, that's 100 equal to 70.
02:43
Our m is 70 plus c, e to the, because at t equals to zero, that's e to the zero...