Question #97219
A 40gm mass hangs at the end of a spring. When a 20gm mass is added the spring stretches by an additional 5cm.
a) What is the force constant of the spring?
b) What is the frequency with which the 40gm mass vibrates?
1
Expert's answer
2019-10-24T09:45:53-0400

We can find the displacement relative to the equilibrium position using the Hooke's law


F=kΔlF = k\Delta l

Where FF is the magnitude of the force acting on the spring (exclude the spring itself), Δl\Delta l - displacement and kk - the force constant of the spring.

a) Let's use that F=mgF = mg and write down the Hooke's law equation for the two cases (we let g10[ms2]g \approx 10[\frac{{\text{m}}}{{{{\text{s}}^{\text{2}}}}}])


{40103[kg]10[ms2]=kΔl(40+20)103[kg]10[ms2]=k(Δl+5102[m])\begin{cases} 40 \cdot {10^{ - 3}}[{\text{kg}}] \cdot 10[\frac{{\text{m}}}{{{{\text{s}}^{\text{2}}}}}] = k\Delta l \\ (40 + 20)\cdot {10^{ - 3}}[{\text{kg}}] \cdot 10[\frac{{\text{m}}}{{{{\text{s}}^{\text{2}}}}}] = k(\Delta l + 5 \cdot {10^{ - 2}}[{\text{m}}]) \end{cases}

From the first equation we've got


Δl=0.4k[kgms2]\Delta l = \frac{{0.4}}{k}[\frac{{{\text{kg}} \cdot {\text{m}}}}{{{{\text{s}}^{\text{2}}}}}]

Substitute in to the second


0.6[kgms2]=0.4[kgms2]+5102[m]k0.6[\frac{{{\text{kg}} \cdot {\text{m}}}}{{{{\text{s}}^{\text{2}}}}}] = 0.4[\frac{{{\text{kg}} \cdot {\text{m}}}}{{{{\text{s}}^{\text{2}}}}}] + 5 \cdot {10^{ - 2}}[{\text{m}}] \cdot k

Thus


k=0.2[kgms2]5102[m]=4[kgs2]k = \frac{{0.2[\frac{{{\text{kg}} \cdot {\text{m}}}}{{{{\text{s}}^{\text{2}}}}}]}}{{5 \cdot {{10}^{ - 2}}[{\text{m}}]}} = 4[\frac{{{\text{kg}}}}{{{{\text{s}}^{\text{2}}}}}]

b)The Hooke's law can be written as


Fx=kx{F_x} = - kx

(now we use projection of the force Fx{F_x} to the x-axis, thus we have that minus sign, means that the force is "trying" to return the spring in the equilibrium state, xx - displacement)

Then using the Newton's second law


mx¨=kxm\ddot x = - kx

And can be rewritten as


x¨+kmx=0\ddot x + \frac{k}{m}x = 0

It's general solution is


x(t)=Asin(tkm+φ0)x(t) = A\sin (t\sqrt {\frac{k}{m}} + {\varphi _0})

Thus the circular frequency is

ω=km=4[kgs2]0.04[kg]=10[1s1]\omega = \sqrt {\frac{k}{m}} = \sqrt {\frac{{4[\frac{{{\text{kg}}}}{{{{\text{s}}^{\text{2}}}}}]}}{{0.04[{\text{kg}}]}}} = 10[\frac{{\text{1}}}{{{{\text{s}}^{ - 1}}}}]

Sometimes under frequency they mean the quantity


ν=ω2π=5π[Hz]1.6[Hz]\nu = \frac{\omega }{{2\pi }} = \frac{5}{\pi }[{\text{Hz}}] \approx 1.6[{\text{Hz}}]

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