Normal modes, 2 masses, 2 springs

AI Thread Summary
The discussion revolves around calculating the normal mode frequencies for a system of two masses and two springs. The user sets up the equations of motion for the two masses, leading to a determinant condition for finding the frequencies. They derive a formula for the squared frequencies, α², involving the spring constants and mass, but encounter difficulties when trying to solve for amplitude ratios. Additionally, the user seeks recommendations for simpler equation writing tools to enhance their experience. The thread highlights the complexities involved in solving normal mode problems in mechanical systems.
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Homework Statement


hey, this is my first time using this forum and was wondering if i could have some help with this normal modes question.

suspended from a ceiling is in order: a spring of spring constant (k_{2}), a mass (m), a spring with spring constant (k_{1}), and another mass (m)

calulate the normal mode frequencies \alpha_{1}, \alpha_{1} sorry can't find the omega symbol.

attempted solution:
let the displacement of the higher mass be x and the displacement of the lower mass be y.

m\ddot{x}=-k_{2}x + k_{1}(y-x)
m\ddot{y}=-k_{1}(y-x)

\left| \alpha^{2} - (\frac{k_{2}}{m} + \frac{k_{1}}{m}) -----\frac{k_{1}}{m} \right|
\left| \frac{k_{1}}{m} -------- \alpha^{2} - \frac{k_{1}}{m} \right| = 0

determinant = 0

so \alpha^{2} = 1/2[ (\frac{k_{2}}{m}+ \frac{2k_{1}}{m}) +- sqrt[(\frac{k_{2}}{m}+ \frac{2k_{1}}{m})^2 – 4(\frac{k_{2}*k_{1}}{m^2})]]

after simplifying it doesn't work when I use to try and solve for the amplitude ratios.
please advise, thanks.
p.s. is there a simpler equation writer i could download and use here or should i just persevere and try to use this embedded one?
 
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Homework Equations m*\ddot{x} = -k_{2}*x + k_{1}(y-x)m*\ddot{y} = -k_{1}(y-x)The Attempt at a Solution let the displacement of the higher mass be x and the displacement of the lower mass be y.m\ddot{x}=-k_{2}x + k_{1}(y-x)m\ddot{y}=-k_{1}(y-x)\left| \alpha^{2} - (\frac{k_{2}}{m} + \frac{k_{1}}{m}) -----\frac{k_{1}}{m} \right|\left| \frac{k_{1}}{m} -------- \alpha^{2} - \frac{k_{1}}{m} \right| = 0determinant = 0so \alpha^{2} = 1/2[ (\frac{k_{2}}{m}+ \frac{2k_{1}}{m}) +- sqrt[(\frac{k_{2}}{m}+ \frac{2k_{1}}{m})^2 – 4(\frac{k_{2}*k_{1}}{m^2})]]\alpha_{1,2} = 1/2[ (\frac{k_{2}}{m}+ \frac{2k_{1}}{m}) +- sqrt[(\frac{k_{2}}{m}+ \frac{2k_{1}}{m})^2 – 4(\frac{k_{2}*k_{1}}{m^2})]]^{\frac{1}{2}}
 
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