Second order differential - Tanks in series cooling coil

AI Thread Summary
The discussion revolves around solving a second-order differential equation related to cooling coils in tanks. The user is attempting to find steady-state temperatures T1(∞) and T2(∞) and has derived initial conditions for T1* and T2*. They have calculated the homogeneous solution for T2* and are working through the initial conditions to determine constants A and B. The conversation highlights the complexity of substituting variables and solving coupled differential equations, with users sharing their approaches and calculations. The thread emphasizes the iterative nature of solving these equations and the importance of correctly setting initial conditions.
gmaverick2k
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Homework Statement
Second order differential - Tanks in series cooling coil
Relevant Equations
Second order differential eq's
I'm stuck on a problem:
T1 = dT2/dt + xT2 - y
T2 = (Ae^(-4.26t))+(Be^(-1.82t))+39.9

I'm unsure how to proceed
 
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I was able to get XXV by setting T2 = 94.9 @ t = 0 and putting this into XXIV, but I'm stumped with the other boundary condition result in XXVI
 
Can you please provide the original problem statement?
 
Problem statement below. Final two pages in posts #2 & 3

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Note for XXIII, I got 159.6 for the right hand sided term instead of 309 (see post #2) although the coeffcients remained unchanged
 
I would never have solved this problem the way that they solved it. The first thing I would have done would have been to solve Eqns. 19 and 20 for the final steady state temperatures in the two tanks and large ##\theta## (##T_1(\infty)## and ##T_2(\infty)##), when the two time derivatives approach zero. Then I would write $$T_1=T_1^*+T_1(\infty)$$and$$T_2=T_2^*+T_2(\infty)$$What do you get for the final steady state temperatures, and what do you get when you substitute my Eqns. 1 and 2 into their Eqns. 19 and 20?
 
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Chestermiller said:
I would never have solved this problem the way that they solved it. The first thing I would have done would have been to solve Eqns. 19 and 20 for the final steady state temperatures in the two tanks and large ##\theta## (##T_1(\infty)## and ##T_2(\infty)##), when the two time derivatives approach zero. Then I would write $$T_1=T_1^*+T_1(\infty)$$and$$T_2=T_2^*+T_2(\infty)$$What do you get for the final steady state temperatures, and what do you get when you substitute my Eqns. 1 and 2 into their Eqns. 19 and 20?
I'm most likely wrong here, setting the differentials to 0 in both eq.'s [19] and [20], I get for both eq.'s:

4486.2*T2 - 1500*T1 = 59724

as expected because eq.'s [20] is rearranged form of [19]
 
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  • #10
gmaverick2k said:
I'm most likely wrong here, setting the differentials to 0 in both eq.'s [19] and [20], I get for both eq.'s:

4486.2*T2 - 1500*T1 = 59724

as expected because eq.'s [20] is rearranged form of [19]
Sorry, I meant Eqns. 18 and 19.
 
  • #11
Chestermiller said:
Sorry, I meant Eqns. 18 and 19.
I get:
T1 (∞) = 79.3°C
T2 (∞) = 39.8°C
 
  • #12
gmaverick2k said:
I get:
T1 (∞) = 79.3°C
T2 (∞) = 39.8°C
I didn't check them, but these values look like they are probably right. Now, what do you get when you substitute my Eqns. 1 and 2 into their Eqns. 18 and 19 (in terms of the T*'s)?
 
  • #13
Chestermiller said:
I didn't check them, but these values look like they are probably right. Now, what do you get when you substitute my Eqns. 1 and 2 into their Eqns. 18 and 19 (in terms of the T*'s)?
I get:
T1* = 0.01°C
T2* = 0.03°C
Most likely incorrect because of rounding error
 
  • #14
gmaverick2k said:
I get:
T1* = 0.01°C
T2* = 0.03°C
Most likely incorrect because of rounding error. Differentials again set to zero
 
  • #15
I get $$C\frac{dT_1^*}{d\theta}=-\left[C_W(1-\alpha)+C\right]T_1^*+C_W(1-\alpha)(1-\beta)T_2^*$$ and $$C\frac{T_2^*}{d\theta}=CT_1^*-[C_W(1-\beta)+C]T_2^*$$
Note, that, in terms of the asterisk parameters, there are no constant terms in these equations. Initial conditions are $$T_1^*=142.4-79.3=63.1$$and $$T_2^*=94.9-39.8=55.1$$

Does this make sense to you so far?
 
  • #16
Chestermiller said:
I get $$C\frac{dT_1^*}{d\theta}=-\left[C_W(1-\alpha)+C\right]T_1^*+C_W(1-\alpha)(1-\beta)T_2^*$$ and $$C\frac{T_2^*}{d\theta}=CT_1^*-[C_W(1-\beta)+C]T_2^*$$
Note, that, in terms of the asterisk parameters, there are no constant terms in these equations. Initial conditions are $$T_1^*=142.4-79.3=63.1$$and $$T_2^*=94.9-39.8=55.1$$

Does this make sense to you so far?
So T1 is T1,i (after cooling water is put back on) and T1 (∞) was T1 at inifinite time by setting differential to zero
T1* is T1,i+1
Subbed T1* into the differential term in place of T1 as it will vary with time and T (∞) is constant differential is now dT1*/dt
 
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  • #17
gmaverick2k said:
So T1 is T1,i (after cooling water is put back on) and T1 (∞) was T1 at inifinite time by setting differential to zero
T1* is T1,i+1
Subbed T1* into the differential term in place of T1 as it will vary with time and T (∞) is constant differential is now dT1*/dt
If I understand you correctly, yes. Can you figure out how to solve the T* differential equations?
 
  • #18
Chestermiller said:
If I understand you correctly, yes. Can you figure out how to solve the T* differential equations?
so when T1* is subbed into the differential the terms such as Cw(1-alpha)beta*t3 and CT0 disappear as they are not a function of time
 
  • #19
dT1*/dt = 1.489T2* - 3.094T1*
dT2*/dt = T1* - 2.991T2*
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I think this is where eq's. [3] to [7] kick in for simultaneous 1st ODE.
 
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  • #20
Chestermiller said:
If I understand you correctly, yes. Can you figure out how to solve the T* differential equations?
I may be wrong. Changed the initial temps
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  • #21
I can't read what you did. From the initial values of the T*'s and the two differential equations, what are the initial values of the T*'s?

If you solve the first differential equation for T2* (in terms of T1* and its time derivative) and substitute that into the second differential equation, what do you get?
 
  • #22
I initially used @ t = 0, T2* = 55.1°C as per post #15, which gave T1* = 39.97°C. I thought thats pretty low as the outlet temperature of tank 1 when the water is switched back on shouldn't be that low. So I changed the initial conditions as follows:
@ t = 0; T1* = 94.9°C ; T2* = 81.3°C calculated from the 1st ODE as the input into the dT2*/dt
 
  • #23
gmaverick2k said:
I initially used @ t = 0, T2* = 55.1°C as per post #15, which gave T1* = 39.97°C. I thought thats pretty low as the outlet temperature of tank 1 when the water is switched back on shouldn't be that low. So I changed the initial conditions as follows:
@ t = 0; T1* = 94.9°C ; T2* = 81.3°C calculated from the 1st ODE as the input into the dT2*/dt
This is not correct.
 
  • #24
Chestermiller said:
This is not correct.
I'm stumped. Tried the T* method but I'm hitting a wall..
where t > 0
T1*(t) = T1(0) - T1(t) = 142.4 - T1(t)
T1*(∞) = T1(0) - T1(∞) = 142.4 - 79.3 = 63.1°C
T1*(1) = T1(0) - T1(1) = 142.4 - 23.3 = 119.1°C

T2*(t) = T2(0) - T2(t) = 94.9 - T2(t)
T2*(∞) = T2(0) - T2(∞) = 94.9 - 39.8 = 55.1°C
T2*(1) = T2(0) - T2(1) = 94.9 - 20.3 = 74.6°C

I calculate:
T1(1) = 119.1°C
T2(1) = 74.6°C

Apologies, post #'s 19 & 20 are incorrect and should be ignored
 
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  • #25
gmaverick2k said:
I'm stumped. Tried the T* method but I'm hitting a wall..
where t > 0
T1*(t) = T1(0) - T1(t) = 142.4 - T1(t)
T1*(∞) = T1(0) - T1(∞) = 142.4 - 79.3 = 63.1°C
T1*(1) = T1(0) - T1(1) = 142.4 - 23.3 = 119.1°C

T2*(t) = T2(0) - T2(t) = 94.9 - T2(t)
T2*(∞) = T2(0) - T2(∞) = 94.9 - 39.8 = 55.1°C
T2*(1) = T2(0) - T2(1) = 94.9 - 20.3 = 74.6°C

I calculate:
T1(1) = 119.1°C
T2(1) = 74.6°C

Apologies, post #'s 19 & 20 are incorrect and should be ignored
We are going. to first solve the two homogeneous coupled differential equation in post #19 subject to the initial conditions: $$T_1^*(0)=63.1$$ and $$T_2^*(0)=55.1$$If we substitute these values into the two differential equations, we can obtain the initial conditions on the first derivatives of ##T_1^*## and ##T_2^*## at time t = 0: $$\left[\frac{dT_1^*}{dt}\right]_{t=0}=-3.094T_1^*(0)+1.489T_2^*(0)=-113.2$$ and $$\left[\frac{dT_2^*}{dt}\right]_{t=0}=T_1^*(0)-2.991T_2^*(0)=-101.7$$

The next step is to solve the second equation post #19 for ##T_1^*## in the 2nd differential equation in terms of ##T_2^*## and its first derivative: $$T_1^*=\frac{dT_2^*} {dt}+2.991 T_2^*$$We can then eliminate ##T_1^*## by substituting this into the first differential equation in post #19: $$\frac{d^2T_2^*}{dt^2}+2.991\frac{dT_2^*}{dt}=-3.094\left(\frac{dT_2^*}{dt}+2.991 T_2^*\right)+1.489T_2^*$$or $$\frac{d^2T_2^*}{dt^2}+6.085\frac{dT_2^*}{dt}-7.7652T_2^*=0$$The solution to this homogeneous linear ODE is of the form ##e^{\lambda t}##, with the two exponential terms satisfying $$\lambda^2+6.085\lambda+7.7652=0$$The solution to this quadratic equation for ##\lambda## is $$\lambda=\frac{-6.0850\pm\sqrt{(6.0850)^2-4(7.7652)}}{2}=-4.2638\ and\ -1.8212$$So, $$T_2^*(t)=Ae^{-1.8212t}+Be^{-4.2638t}$$where A and B are constants to be determined from the initial conditions: $$T_2^*(0)=A+B=55.1$$and
$$\left[\frac{dT_2^*}{dt}\right]_{t=0}=-1.8212A-1.4638B=-101.7$$Solving these two linear algebraic equation for the constants A and B gives: $$A=54.3$$ and $$B=0.8$$So, we have $$T_2^*(t)=54.3e^{-1.8212t}+0.8e^{-4.2638t}$$The solution for ##T_2## is then $$T_2=T_2(\infty)+T_2^*=39.8+54.3e^{-1.8212t}+0.8e^{-4.2638t}$$
 
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  • #26
Chestermiller said:
We are going. to first solve the two homogeneous coupled differential equation in post #19 subject to the initial conditions: $$T_1^*(0)=63.1$$ and $$T_2^*(0)=55.1$$If we substitute these values into the two differential equations, we can obtain the initial conditions on the first derivatives of ##T_1^*## and ##T_2^*## at time t = 0: $$\left[\frac{dT_1^*}{dt}\right]_{t=0}=-3.094T_1^*(0)+1.489T_2^*(0)=-113.2$$ and $$\left[\frac{dT_2^*}{dt}\right]_{t=0}=T_1^*(0)-2.991T_2^*(0)=-101.7$$

The next step is to solve the second equation post #19 for ##T_1^*## in the 2nd differential equation in terms of ##T_2^*## and its first derivative: $$T_1^*=\frac{dT_2^*} {dt}+2.991 T_2^*$$We can then eliminate ##T_1^*## by substituting this into the first differential equation in post #19: $$\frac{d^2T_2^*}{dt^2}+2.991\frac{dT_2^*}{dt}=-3.094\left(\frac{dT_2^*}{dt}+2.991 T_2^*\right)+1.489T_2^*$$or $$\frac{d^2T_2^*}{dt^2}+6.085\frac{dT_2^*}{dt}-7.7652T_2^*=0$$The solution to this homogeneous linear ODE is of the form ##e^{\lambda t}##, with the two exponential terms satisfying $$\lambda^2+6.085\lambda+7.7652=0$$The solution to this quadratic equation for ##\lambda## is $$\lambda=\frac{-6.0850\pm\sqrt{(6.0850)^2-4(7.7652)}}{2}=-4.2638\ and\ -1.8212$$So, $$T_2^*(t)=Ae^{-1.8212t}+Be^{-4.2638t}$$where A and B are constants to be determined from the initial conditions: $$T_2^*(0)=A+B=55.1$$and
$$\left[\frac{dT_2^*}{dt}\right]_{t=0}=-1.8212A-1.4638B=-101.7$$Solving these two linear algebraic equation for the constants A and B gives: $$A=54.3$$ and $$B=0.8$$So, we have $$T_2^*(t)=54.3e^{-1.8212t}+0.8e^{-4.2638t}$$The solution for ##T_2## is then $$T_2=T_2(\infty)+T_2^*=39.8+54.3e^{-1.8212t}+0.8e^{-4.2638t}$$
Thank you. Apologies, had a family emergency last week so wasn't able to get back on this
 
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