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Give step-by-step solution with explanation and final answer:2.17. Al the springs in Figure P2.17 are identical, each with spring constant K. The spring forces are zero when x; =x; =x3 =0. a. Draw the free-body diagrams, including the gravitational forces, and write the differential equations describing the system. b. Determine the constant elongation of each spring caused by the gravitational forces when the masses are stationary in position of static equilibrium and when fal) =0. g Ig Hi 3g gx B B . : al 3x i] i bd ; B EN By 2 3 Te 3 rv Jn Jo Figure P2.17 Figure P2.18

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Give step-by-step solution with explanation and final answer:Uploaded Image2.17. Al the springs in Figure P2.17 are identical, each with spring constant K. The spring forces are zero when x; =x; =x3 =0. a. Draw the free-body diagrams, including the gravitational forces, and write the differential equations describing the system. b. Determine the constant elongation of each spring caused by the gravitational forces when the masses are stationary in position of static equilibrium and when fal) =0. g Ig Hi 3g gx B B . : al 3x i] i bd ; B EN By 2 3 Te 3 rv Jn Jo Figure P2.17 Figure P2.18

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Asked by: Rahul
Created at: 2026-01-22 02:59:17

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Let's solve **Problem 2.17** step-by-step for **Figure P2.17**. --- ## (a) **Free-Body Diagrams and Differential Equations** ### **Free-Body Diagrams** #### **Mass \(M_1\):** - **Upward forces:** Spring force from top spring \(K(x_1)\) - **Downward forces:** Spring force from bottom spring \(K(x_1 - x_3)\), Damping \(B_1 \dot{x}_1\), Weight \(M_1 g\) #### **Mass \(M_2\):** - **Upward force:** Spring force from top spring \(K(x_2)\) - **Downward forces:** Spring force from bottom spring \(K(x_2 - x_3)\), Damping \(B_2 \dot{x}_2\), Weight \(M_2 g\) #### **Mass \(M_3\):** - **Upward forces:** Spring forces from both upper springs (\(K(x_1 - x_3)\) from left, \(K(x_2 - x_3)\) from right) - **Downward forces:** Weight \(M_3 g\), External force \(f_a(t)\) --- ### **Equations of Motion (Newton's Second Law)** #### **For \(M_1\):** \[ M_1 \ddot{x}_1 = -K x_1 - B_1 \dot{x}_1 + K(x_3 - x_1) - M_1 g \] \[ M_1 \ddot{x}_1 + B_1 \dot{x}_1 + 2K x_1 - K x_3 = -M_1 g \] #### **For \(M_2\):** \[ M_2 \ddot{x}_2 = -K x_2 - B_2 \dot{x}_2 + K(x_3 - x_2) - M_2 g \] \[ M_2 \ddot{x}_2 + B_2 \dot{x}_2 + 2K x_2 - K x_3 = -M_2 g \] #### **For \(M_3\):** \[ M_3 \ddot{x}_3 = -K(x_3 - x_1) - K(x_3 - x_2) - M_3 g + f_a(t) \] \[ M_3 \ddot{x}_3 + 2K x_3 - K x_1 - K x_2 = f_a(t) - M_3 g \] --- ## (b) **Static Equilibrium (Constant Elongation of Each Spring, \(f_a(t) = \))** At equilibrium, \(\ddot{x}_i = \), \(\dot{x}_i = \), \(f_a(t) = \): ### **Write Static Equations** 1. \(2K x_1 - K x_3 = -M_1 g\) 2. \(2K x_2 - K x_3 = -M_2 g\) 3. \(-K x_1 - K x_2 + 2K x_3 = -M_3 g\) ### **Solve the System** #### **Step 1:** Express \(x_1\) and \(x_2\) in terms of \(x_3\): From (1): \(2K x_1 - K x_3 = -M_1 g\) \(\rightarrow x_1 = \frac{K x_3 - M_1 g}{2K}\) From (2): \(2K x_2 - K x_3 = -M_2 g\) \(\rightarrow x_2 = \frac{K x_3 - M_2 g}{2K}\) #### **Step 2:** Substitute into (3): \[ -K x_1 - K x_2 + 2K x_3 = -M_3 g \] Substitute \(x_1\) and \(x_2\): \[ -K \left(\frac{K x_3 - M_1 g}{2K}\right) - K \left(\frac{K x_3 - M_2 g}{2K}\right) + 2K x_3 = -M_3 g \] \[ -\frac{K x_3 - M_1 g}{2} - \frac{K x_3 - M_2 g}{2} + 2K x_3 = -M_3 g \] \[ -\frac{K x_3 - M_1 g + K x_3 - M_2 g}{2} + 2K x_3 = -M_3 g \] \[ -\frac{2K x_3 - (M_1 + M_2)g}{2} + 2K x_3 = -M_3 g \] \[ -(K x_3 - \frac{(M_1 + M_2)g}{2}) + 2K x_3 = -M_3 g \] \[ -K x_3 + \frac{(M_1 + M_2)g}{2} + 2K x_3 = -M_3 g \] \[ K x_3 + \frac{(M_1 + M_2)g}{2} = -M_3 g \] \[ K x_3 = -M_3 g - \frac{(M_1 + M_2)g}{2} \] \[ x_3 = -\frac{M_3 g}{K} - \frac{(M_1 + M_2)g}{2K} \] #### **Step 3:** Plug \(x_3\) into \(x_1\) and \(x_2\): \[ x_1 = \frac{K x_3 - M_1 g}{2K} \] \[ x_1 = \frac{K \left(-\frac{M_3 g}{K} - \frac{(M_1 + M_2)g}{2K}\right) - M_1 g}{2K} \] \[ x_1 = \frac{-M_3 g - \frac{(M_1 + M_2) g}{2} - M_1 g}{2K} \] \[ x_1 = \frac{-M_3 g - M_1 g - \frac{(M_1 + M_2)g}{2}}{2K} \] \[ x_1 = \frac{-M_3 g - M_1 g - \frac{M_1 g}{2} - \frac{M_2 g}{2}}{2K} \] \[ x_1 = \frac{-M_3 g - \frac{3M_1 g}{2} - \frac{M_2 g}{2}}{2K} \] Similarly, for \(x_2\): \[ x_2 = \frac{K x_3 - M_2 g}{2K} \] \[ x_2 = \frac{-M_3 g - \frac{(M_1 + M_2) g}{2} - M_2 g}{2K} \] \[ x_2 = \frac{-M_3 g - M_2 g - \frac{M_1 g}{2} - \frac{M_2 g}{2}}{2K} \] \[ x_2 = \frac{-M_3 g - \frac{3M_2 g}{2} - \frac{M_1 g}{2}}{2K} \] --- ## **Final Answers** ### **(a) Differential Equations:** \[ \boxed{ \begin{aligned} &M_1 \ddot{x}_1 + B_1 \dot{x}_1 + 2K x_1 - K x_3 = -M_1 g \\ &M_2 \ddot{x}_2 + B_2 \dot{x}_2 + 2K x_2 - K x_3 = -M_2 g \\ &M_3 \ddot{x}_3 + 2K x_3 - K x_1 - K x_2 = f_a(t) - M_3 g \end{aligned} } \] ### **(b) Static Equilibrium (Elongations):** \[ \boxed{ \begin{aligned} x_1 &= \frac{-M_3 g - \frac{3M_1 g}{2} - \frac{M_2 g}{2}}{2K} \\ x_2 &= \frac{-M_3 g - \frac{3M_2 g}{2} - \frac{M_1 g}{2}}{2K} \\ x_3 &= -\frac{M_3 g}{K} - \frac{(M_1 + M_2)g}{2K} \end{aligned} } \] --- **Let me know if you need the solution for Figure P2.18 as well!**

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