State the initial value problem describing the mass's motion upon starting from its release, Solution: Displacement y from equilibrium solves the equation given in the lecture y" the initial values given in the problem are y(0) = 0 and y'(0) = 0.01. Solve the initial value problem formulated in (b). Solution: The root oquation has solutions I k ===y=-500y, m 500 So the general coltuion is

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Author:Erwin Kreyszig
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Chapter2: Second-order Linear Odes
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Can you explain step by step how to do PART C pls

**Problem 2:** A 100 gram mass, when attached to a spring hanging vertically, stretches the spring 2 cm. The mass is then released from the equilibrium position with an initial velocity of 1 cm/s. Assume that there is no damping.

**(a) Determine the spring constant \( k \),**

**Solution:** Equating the gravitational force and spring force, we get

\[
k = \frac{mg}{\Delta x} = \frac{10 \times 0.1}{0.02} = 50 \, \text{N/m}.
\]

**(b) State the initial value problem describing the mass’s motion upon starting from its release,**

**Solution:** Displacement \( y \) from equilibrium solves the equation given in the lecture

\[
y'' = -\frac{k}{m}y = -500y,
\]

the initial values given in the problem are \( y(0) = 0 \) and \( y'(0) = 0.01 \).

**(c) Solve the initial value problem formulated in (b).**

**Solution:** The root equation has solutions \( \lambda = \pm \sqrt{500}i \). So the general solution is

\[
y(t) = C_1 \sin(\sqrt{500}t) + C_2 \cos(\sqrt{500}t).
\]

Using the initial values, I get \( C_2 = 0 \) and \( \sqrt{500}C_1 = 0.01 \), so

\[
y(t) = \frac{0.01}{\sqrt{500}} \sin(\sqrt{500}t).
\]
Transcribed Image Text:**Problem 2:** A 100 gram mass, when attached to a spring hanging vertically, stretches the spring 2 cm. The mass is then released from the equilibrium position with an initial velocity of 1 cm/s. Assume that there is no damping. **(a) Determine the spring constant \( k \),** **Solution:** Equating the gravitational force and spring force, we get \[ k = \frac{mg}{\Delta x} = \frac{10 \times 0.1}{0.02} = 50 \, \text{N/m}. \] **(b) State the initial value problem describing the mass’s motion upon starting from its release,** **Solution:** Displacement \( y \) from equilibrium solves the equation given in the lecture \[ y'' = -\frac{k}{m}y = -500y, \] the initial values given in the problem are \( y(0) = 0 \) and \( y'(0) = 0.01 \). **(c) Solve the initial value problem formulated in (b).** **Solution:** The root equation has solutions \( \lambda = \pm \sqrt{500}i \). So the general solution is \[ y(t) = C_1 \sin(\sqrt{500}t) + C_2 \cos(\sqrt{500}t). \] Using the initial values, I get \( C_2 = 0 \) and \( \sqrt{500}C_1 = 0.01 \), so \[ y(t) = \frac{0.01}{\sqrt{500}} \sin(\sqrt{500}t). \]
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