A spring-mass system consists of a mass of 5 kg and two springs of stiffness 8 N/mm and 12 N/mm. The system is arranged in different manners, that is: (i) the mass is suspended at the bottom of two springs in series, and (ii) the mass is fixed between two springs. The ratio of natural frequencies of the case (ii) to those of case (i) is approximately ___________.
2.0
This problem involves calculating the natural frequencies of a spring-mass system under two different configurations: springs in series and springs in parallel. We will then determine the ratio of these natural frequencies. A clear understanding of equivalent stiffness for different spring arrangements is crucial here.
First, let's convert the given spring stiffness values from N/mm to N/m, which is the standard SI unit for stiffness, as mass is given in kg.
The mass of the system is given as $$\small m = 5 \text{ kg}$$.
In case (i), the mass is suspended at the bottom of two springs connected in series.
For springs connected in series, the reciprocal of the equivalent stiffness ($$\small k_{eq,i}$$) is the sum of the reciprocals of individual stiffnesses.
The formula for equivalent stiffness in series is:
$$\small \frac{1}{k_{eq,i}} = \frac{1}{k_1} + \frac{1}{k_2}$$
Substituting the values:
$$\small \frac{1}{k_{eq,i}} = \frac{1}{8000 \text{ N/m}} + \frac{1}{12000 \text{ N/m}}$$
$$\small \frac{1}{k_{eq,i}} = \frac{3}{24000} + \frac{2}{24000}$$
$$\small \frac{1}{k_{eq,i}} = \frac{5}{24000}$$
$$\small k_{eq,i} = \frac{24000}{5} = 4800 \text{ N/m}$$
The natural frequency ($$\small \omega_n$$) of a spring-mass system is given by the formula:
$$\small \omega_n = \sqrt{\frac{k_{eq}}{m}}$$
For case (i), the natural frequency ($$\small \omega_{n,i}$$) is:
$$\small \omega_{n,i} = \sqrt{\frac{k_{eq,i}}{m}} = \sqrt{\frac{4800 \text{ N/m}}{5 \text{ kg}}}$$
$$\small \omega_{n,i} = \sqrt{960} \text{ rad/s}$$
$$\small \omega_{n,i} \approx 30.9838 \text{ rad/s}$$
In case (ii), the mass is fixed between two springs. This arrangement typically implies a parallel connection, where both springs contribute directly to the restoring force on the mass.
For springs connected in parallel, the equivalent stiffness ($$\small k_{eq,ii}$$) is the sum of the individual stiffnesses.
The formula for equivalent stiffness in parallel is:
$$\small k_{eq,ii} = k_1 + k_2$$
Substituting the values:
$$\small k_{eq,ii} = 8000 \text{ N/m} + 12000 \text{ N/m}$$
$$\small k_{eq,ii} = 20000 \text{ N/m}$$
For case (ii), the natural frequency ($$\small \omega_{n,ii}$$) is:
$$\small \omega_{n,ii} = \sqrt{\frac{k_{eq,ii}}{m}} = \sqrt{\frac{20000 \text{ N/m}}{5 \text{ kg}}}$$
$$\small \omega_{n,ii} = \sqrt{4000} \text{ rad/s}$$
$$\small \omega_{n,ii} \approx 63.2456 \text{ rad/s}$$
We need to find the ratio of natural frequencies of case (ii) to those of case (i).
Ratio $$= \frac{\omega_{n,ii}}{\omega_{n,i}}$$ Ratio $$= \frac{\sqrt{4000}}{\sqrt{960}}$$ Ratio $$= \sqrt{\frac{4000}{960}}$$ Ratio $$= \sqrt{\frac{400}{96}}$$ Ratio $$= \sqrt{\frac{100}{24}}$$ Ratio $$= \sqrt{\frac{25}{6}}$$ Ratio $$\approx \sqrt{4.16666...}$$ Ratio $$\approx 2.0412$$
The calculated ratio of natural frequencies of case (ii) to case (i) is approximately 2.0412.
Comparing this value with the given options:
| Option | Value |
|---|---|
| 1 | 0.5 |
| 2 | 1.0 |
| 3 | 2.0 |
| 4 | 1.5 |
The closest approximation to 2.0412 is 2.0.
Therefore, the ratio of natural frequencies of the case (ii) to those of case (i) is approximately 2.0.
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