Second order differential - Tanks in series cooling coil

  • #1
gmaverick2k
42
3
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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  • #2
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  • #3
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  • #4
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
 
  • #5
Can you please provide the original problem statement?
 
  • #6
Problem statement below. Final two pages in posts #2 & 3

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  • #7
Note for XXIII, I got 159.6 for the right hand sided term instead of 309 (see post #2) although the coeffcients remained unchanged
 
  • #8
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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  • #9
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*
IMG_20240315_195941281.jpg


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
 

FAQ: Second order differential - Tanks in series cooling coil

What is a second order differential equation in the context of tanks in series with a cooling coil?

A second order differential equation in this context typically represents the dynamic response of the temperature in a system of interconnected tanks, each with a cooling coil. The equation takes into account the rate of change of temperature and the interactions between the tanks and the cooling coils, capturing the system's behavior over time.

How do you derive the second order differential equation for a system of tanks in series with a cooling coil?

To derive the second order differential equation, you start by applying the principles of mass and energy balance to each tank. For each tank, you consider the rate of heat transfer due to the cooling coil and the flow of fluid between tanks. By combining these balances and eliminating intermediate variables, you obtain a single second order differential equation that describes the entire system.

What are the typical boundary conditions for solving the second order differential equation in this system?

Typical boundary conditions may include the initial temperatures of the fluid in each tank, the temperature of the cooling medium, and the flow rates of the fluid between tanks. These conditions help to uniquely determine the solution to the differential equation, allowing for the prediction of temperature profiles over time.

How can numerical methods be used to solve the second order differential equation for tanks in series with a cooling coil?

Numerical methods, such as finite difference methods, Runge-Kutta methods, or finite element methods, can be used to approximate the solution to the second order differential equation. These methods discretize the time and/or space domain and iteratively solve the equations, providing an approximate solution that can be analyzed and used for system design or optimization.

What are some common applications of second order differential equations in tanks in series with a cooling coil?

Common applications include chemical processing industries, where precise temperature control is crucial for reactions; HVAC systems, where multiple cooling stages may be used to achieve desired temperatures; and environmental engineering, where such systems can be employed for wastewater treatment or thermal regulation. Understanding the dynamics through second order differential equations helps in designing efficient and effective systems.

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