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rewrite same all the content given below line Here’s the **entire derivation** of the transfer function for the 3-tank system in a **single part**, step-by-step: --- ### **Step 1: Understand the System and Flow Direction** * **Input flow** enters the **middle tank (Tank 1)**. * Liquid flows from **Tank 1 → Tank 2 (left tank) → Tank 3 (right tank)**. * Then it exits the system as **output flow** $q_o(t)$. **Flow Path:** $$ \text{Tank 1} \rightarrow \text{Tank 2} \rightarrow \text{Tank 3} \rightarrow q_o(t) $$ **Let:** * $h_1(t), h_2(t), h_3(t)$: liquid heights in tanks 1, 2, 3 * $C_1, C_2, C_3$: capacitance (cross-sectional area) of each tank * $R_1, R_2, R_3$: flow resistances between tanks and at outlet --- ### **Step 2: Write Mass Balance Equations** We apply: $$ C \cdot \frac{dh(t)}{dt} = \text{Inflow} - \text{Outflow} $$ $$ q = \frac{h_{\text{up}} - h_{\text{down}}}{R} $$ #### ✅ Tank 1 (Middle Tank): * Inflow: $q(t)$ * Outflow to Tank 2: $q_1(t) = \frac{h_1(t) - h_2(t)}{R_1}$ $$ C_1 \frac{dh_1(t)}{dt} = q(t) - \frac{h_1(t) - h_2(t)}{R_1} $$ --- #### ✅ Tank 2 (Left Tank): * Inflow: $q_1(t)$ * Outflow to Tank 3: $q_2(t) = \frac{h_2(t) - h_3(t)}{R_2}$ $$ C_2 \frac{dh_2(t)}{dt} = \frac{h_1(t) - h_2(t)}{R_1} - \frac{h_2(t) - h_3(t)}{R_2} $$ --- #### ✅ Tank 3 (Right Tank): * Inflow: $q_2(t)$ * Outflow: $q_o(t) = \frac{h_3(t)}{R_3}$ $$ C_3 \frac{dh_3(t)}{dt} = \frac{h_2(t) - h_3(t)}{R_2} - \frac{h_3(t)}{R_3} $$ --- ### **Step 3: Apply Laplace Transform** Let: $$ \frac{dh(t)}{dt} \rightarrow sH(s), \quad q(t) \rightarrow Q(s) $$ #### Equation 1 (Tank 1): $$ C_1 s H_1(s) = Q(s) - \frac{H_1(s) - H_2(s)}{R_1} $$ #### Equation 2 (Tank 2): $$ C_2 s H_2(s) = \frac{H_1(s) - H_2(s)}{R_1} - \frac{H_2(s) - H_3(s)}{R_2} $$ #### Equation 3 (Tank 3): $$ C_3 s H_3(s) = \frac{H_2(s) - H_3(s)}{R_2} - \frac{H_3(s)}{R_3} $$ #### Equation 4 (Output relation): $$ Q_o(s) = \frac{H_3(s)}{R_3} \Rightarrow H_3(s) = R_3 Q_o(s) $$ --- ### **Step 4: Make a Simplifying Assumption** Assume **identical tanks**: * $R_1 = R_2 = R_3 = R$ * $C_1 = C_2 = C_3 = C$ Then the **time constant**: $$ \tau = RC $$ --- ### **Step 5: Use Transfer Functions of First-Order Systems** Each tank is a first-order system: $$ \frac{\text{Output}}{\text{Input}} = \frac{1}{\tau s + 1} $$ Since tanks are in **series**, multiply their transfer functions: $$ \frac{Q_o(s)}{Q(s)} = \left( \frac{1}{\tau s + 1} \right)^3 = \frac{1}{(RCs + 1)^3} $$ --- ### ✅ **Final Answer:** $$ \boxed{\frac{Q_o(s)}{Q(s)} = \frac{1}{(RCs + 1)^3}} $$ This is the **overall transfer function** of the 3-tank system with identical parameters.

Question:

rewrite same all the content given below line Here’s the **entire derivation** of the transfer function for the 3-tank system in a **single part**, step-by-step: --- ### **Step 1: Understand the System and Flow Direction** * **Input flow** enters the **middle tank (Tank 1)**. * Liquid flows from **Tank 1 → Tank 2 (left tank) → Tank 3 (right tank)**. * Then it exits the system as **output flow** $q_o(t)$. **Flow Path:** $$ \text{Tank 1} \rightarrow \text{Tank 2} \rightarrow \text{Tank 3} \rightarrow q_o(t) $$ **Let:** * $h_1(t), h_2(t), h_3(t)$: liquid heights in tanks 1, 2, 3 * $C_1, C_2, C_3$: capacitance (cross-sectional area) of each tank * $R_1, R_2, R_3$: flow resistances between tanks and at outlet --- ### **Step 2: Write Mass Balance Equations** We apply: $$ C \cdot \frac{dh(t)}{dt} = \text{Inflow} - \text{Outflow} $$ $$ q = \frac{h_{\text{up}} - h_{\text{down}}}{R} $$ #### ✅ Tank 1 (Middle Tank): * Inflow: $q(t)$ * Outflow to Tank 2: $q_1(t) = \frac{h_1(t) - h_2(t)}{R_1}$ $$ C_1 \frac{dh_1(t)}{dt} = q(t) - \frac{h_1(t) - h_2(t)}{R_1} $$ --- #### ✅ Tank 2 (Left Tank): * Inflow: $q_1(t)$ * Outflow to Tank 3: $q_2(t) = \frac{h_2(t) - h_3(t)}{R_2}$ $$ C_2 \frac{dh_2(t)}{dt} = \frac{h_1(t) - h_2(t)}{R_1} - \frac{h_2(t) - h_3(t)}{R_2} $$ --- #### ✅ Tank 3 (Right Tank): * Inflow: $q_2(t)$ * Outflow: $q_o(t) = \frac{h_3(t)}{R_3}$ $$ C_3 \frac{dh_3(t)}{dt} = \frac{h_2(t) - h_3(t)}{R_2} - \frac{h_3(t)}{R_3} $$ --- ### **Step 3: Apply Laplace Transform** Let: $$ \frac{dh(t)}{dt} \rightarrow sH(s), \quad q(t) \rightarrow Q(s) $$ #### Equation 1 (Tank 1): $$ C_1 s H_1(s) = Q(s) - \frac{H_1(s) - H_2(s)}{R_1} $$ #### Equation 2 (Tank 2): $$ C_2 s H_2(s) = \frac{H_1(s) - H_2(s)}{R_1} - \frac{H_2(s) - H_3(s)}{R_2} $$ #### Equation 3 (Tank 3): $$ C_3 s H_3(s) = \frac{H_2(s) - H_3(s)}{R_2} - \frac{H_3(s)}{R_3} $$ #### Equation 4 (Output relation): $$ Q_o(s) = \frac{H_3(s)}{R_3} \Rightarrow H_3(s) = R_3 Q_o(s) $$ --- ### **Step 4: Make a Simplifying Assumption** Assume **identical tanks**: * $R_1 = R_2 = R_3 = R$ * $C_1 = C_2 = C_3 = C$ Then the **time constant**: $$ \tau = RC $$ --- ### **Step 5: Use Transfer Functions of First-Order Systems** Each tank is a first-order system: $$ \frac{\text{Output}}{\text{Input}} = \frac{1}{\tau s + 1} $$ Since tanks are in **series**, multiply their transfer functions: $$ \frac{Q_o(s)}{Q(s)} = \left( \frac{1}{\tau s + 1} \right)^3 = \frac{1}{(RCs + 1)^3} $$ --- ### ✅ **Final Answer:** $$ \boxed{\frac{Q_o(s)}{Q(s)} = \frac{1}{(RCs + 1)^3}} $$ This is the **overall transfer function** of the 3-tank system with identical parameters.

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Asked by: mohit
Created at: 2025-08-02 03:41:17

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Certainly! Here’s the **complete derivation** of the transfer function for the 3-tank system, presented as a unified, step-by-step process: --- ### **Step 1: System Overview and Flow Sequence** * The **input flow** enters the **central tank (Tank 1)**. * Liquid moves sequentially from **Tank 1 → Tank 2 (left) → Tank 3 (right)**. * The liquid then exits from Tank 3 as the **output flow** $q_o(t)$. **Flow Direction:** $$ \text{Tank 1} \longrightarrow \text{Tank 2} \longrightarrow \text{Tank 3} \longrightarrow q_o(t) $$ **Definitions:** * $h_1(t), h_2(t), h_3(t)$: liquid levels in tanks 1, 2, and 3 * $C_1, C_2, C_3$: capacitance (cross-sectional area) for each tank * $R_1, R_2, R_3$: flow resistances between tanks and at the outlet --- ### **Step 2: Formulate Mass Balance Equations** For each tank, the general balance is: $$ C \cdot \frac{dh(t)}{dt} = \text{Inflow} - \text{Outflow} $$ and the flow through a resistance is: $$ q = \frac{h_{\text{up}} - h_{\text{down}}}{R} $$ #### Tank 1 (Middle): * **Inflow:** $q(t)$ * **Outflow to Tank 2:** $q_1(t) = \frac{h_1(t) - h_2(t)}{R_1}$ $$ C_1 \frac{dh_1(t)}{dt} = q(t) - \frac{h_1(t) - h_2(t)}{R_1} $$ #### Tank 2 (Left): * **Inflow:** $q_1(t)$ * **Outflow to Tank 3:** $q_2(t) = \frac{h_2(t) - h_3(t)}{R_2}$ $$ C_2 \frac{dh_2(t)}{dt} = \frac{h_1(t) - h_2(t)}{R_1} - \frac{h_2(t) - h_3(t)}{R_2} $$ #### Tank 3 (Right): * **Inflow:** $q_2(t)$ * **Outflow:** $q_o(t) = \frac{h_3(t)}{R_3}$ $$ C_3 \frac{dh_3(t)}{dt} = \frac{h_2(t) - h_3(t)}{R_2} - \frac{h_3(t)}{R_3} $$ --- ### **Step 3: Apply the Laplace Transform** Let: $$ \frac{dh(t)}{dt} \rightarrow sH(s), \quad q(t) \rightarrow Q(s) $$ After Laplace transformation: #### Tank 1: $$ C_1 s H_1(s) = Q(s) - \frac{H_1(s) - H_2(s)}{R_1} $$ #### Tank 2: $$ C_2 s H_2(s) = \frac{H_1(s) - H_2(s)}{R_1} - \frac{H_2(s) - H_3(s)}{R_2} $$ #### Tank 3: $$ C_3 s H_3(s) = \frac{H_2(s) - H_3(s)}{R_2} - \frac{H_3(s)}{R_3} $$ #### Output Flow: $$ Q_o(s) = \frac{H_3(s)}{R_3} \implies H_3(s) = R_3 Q_o(s) $$ --- ### **Step 4: Assume Identical Parameters for Simplicity** Assume all tanks and resistances are identical: * $R_1 = R_2 = R_3 = R$ * $C_1 = C_2 = C_3 = C$ Then, the **time constant** is: $$ \tau = RC $$ --- ### **Step 5: Recognize Series of First-Order Systems** Each tank behaves as a first-order system: $$ \frac{\text{Output}}{\text{Input}} = \frac{1}{\tau s + 1} $$ With the tanks connected in **series**, their transfer functions multiply: $$ \frac{Q_o(s)}{Q(s)} = \left[\frac{1}{\tau s + 1}\right]^3 = \frac{1}{(RCs + 1)^3} $$ --- ### **Final Transfer Function:** $$ \boxed{ \frac{Q_o(s)}{Q(s)} = \frac{1}{(RCs + 1)^3} } $$ This is the **overall transfer function** for the 3-tank system assuming all tanks and resistances are identical.

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