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Oscillations Of A Spring-mass System MCQ - Practice Questions with Answers

Edited By admin | Updated on Sep 25, 2023 25:23 PM | #NEET

Quick Facts

  • Oscillations in combination of springs is considered one the most difficult concept.

  • Spring System is considered one of the most asked concept.

  • 25 Questions around this concept.

Solve by difficulty

A mass M is suspended from a spring of negligible mass. The spring is pulled a little and then released so that the mass executes SHM of time period T. If the mass is increased by m, the time period becomes 5T/3. Then the ratio of m/M is :

A 1 kg block attached to a spring vibrates with a frequency of 1 Hz on a frictionless horizontal table.  Two springs identical to the original spring are attached in parallel to an 8 kg block placed on the same table. So, the frequency of vibration of the 8 kg block is :

 

Two springs, of force constants k_{1} and k_{2} are connected to a mass m as shown. The frequency of oscillation of the mass is f.      If both k_{1} and k_{2} are made four times their original values, the frequency of oscillation becomes

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Concepts Covered - 2

Spring System

Spring Force:-

  • Spring force is also called restoring force.

  • F= -kx 

           where k is the spring constant and its unit is N/m and x is net elongation or compression in the spring.

           Spring constant (k) is a measure of stiffness or softness of the spring

  • Here -ve sign is because the force exerted by the spring is always in the opposite direction to the displacement. 

The time period of the Spring mass system-

1. Oscillation of a spring in a verticle plane-

Finding Time period of spring using Force method.

Let x_{0}  be the deformation in the spring in equilibrium. Then k x_{0}=m g . When the block is further displaced by x , the net restoring force is given by F=-\left[k\left(x+x_{0}\right)-m g\right] as shown in the below figure.

using  F=-\left[k\left(x+x_{0}\right)-m g\right] and k x_{0}=m g .

we get F=-kx

comparing it with the equation of SHM i.e F=-m\omega ^2x

we get  \omega^{2}=\frac{k}{m} \Rightarrow T=2 \pi \sqrt{\frac{m}{k}}

similarly \text { Frequency } =n=\frac{1}{2 \pi} \sqrt{\frac{k}{m}}

2.Oscillation of spring in the horizontal  plane

For the above figure, Using force method we get a Time period of spring as T=2 \pi \sqrt{\frac{m}{k}} and  \text { Frequency } =n=\frac{1}{2 \pi} \sqrt{\frac{k}{m}}

  • Key points

      1. The time period of a spring-mass system  depends on the mass suspended  

                T \propto \sqrt{m} \quad \text { or } \quad n \propto \frac{1}{\sqrt{m}}

     2.  The time period of a spring-mass system depends on the force constant k of the spring 

           T \propto \frac{1}{\sqrt{k}} \quad \text { or } \quad n \propto \sqrt{k}

   3. The time of a spring pendulum is independent of acceleration due to gravity.

  4. The spring constant k is inversely proportional to the spring length.

    \text { As } \quad k \propto \frac{1}{\text { Extension }} \propto \frac{1}{\text { Length of spring }(l)}

i.e kl=constant

That means if the length of spring is halved then its force constant becomes double.

  5.  When a spring of length l is cut in two pieces of length l1 and l2 such that  l_1=nl_2

     So using

 l_1+l_2=l \\ \begin{array}{l} nl_{2}+l_{2}=l \\ (n+1) l_{2}=l \Rightarrow l_2=\frac{l}{n+1}\\ \\ \text{similarly} \ \l_{1}=nl_2 \Rightarrow l_1=\frac{l*n}{(n+1)} \end{array}

 If the constant of a spring is k then

using kl=constant

i.e k_1l_1=k_2l_2=kl

we get

  \begin{array}{l}{\text { Spring constant of first part } k_{1}=\frac{k(n+1)}{n}} \\ {\text { Spring constant of second part } k_{2}=(n+1) k}\end{array}

\text { and ratio of spring constant } \frac{k_{1}}{k_{2}}=\frac{1}{n}

   6.  If the spring has a mass M and mass m is suspended from it, then its effective mass is given by m_{e f f}=m+\frac{M}{3}

     and T=2 \pi \sqrt{\frac{m_{e f f}}{k}}

 

 

 

Oscillations in combination of springs

1. Series combination of spring

If 2 springs of different force constant are connected in series as shown in the below figure

then k=equivalent force constant is given by 

\frac{1}{K_{eq}}=\frac{1}{K}= \frac{1}{K_{1}}+ \frac{1}{K_{2}}

Where K_{1}and\ K_{2} are spring constants of spring 1 & 2 respectively.

Similarly, If n springs of different force constant are connected in series having force constant k_{1}, k_{2}, k_{3} \ldots \ldots respectively

then \frac{1}{k_{e f f}}=\frac{1}{k_{1}}+\frac{1}{k_{2}}+\frac{1}{k_{3}}+\ldots \ldots \ldots

If all the n spring have the same spring constant as K_{1} then   \frac{1}{k_{e f f}}=\frac{n}{k_{1}}

2.The parallel combination of spring

If 2 springs of different force constant are connected in parallel as shown in the below figure

then k=equivalent force constant is given by 

K_{eq}=K=K_{1}+K_{2}

where K_{1}and\ K_{2} are spring constants of spring 1 & 2 respectively.

Similarly, If n springs of different force constant are connected in parallel having force constant k_{1}, k_{2}, k_{3} \ldots \ldots respectively

then K_{eq}=K_{1}+K_{2}+K_{3}....

If all the n spring have the same spring constant as K_{1} then   K_{eq}=nK_{1}

Study it with Videos

Spring System
Oscillations in combination of springs

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Spring System

Physics Part II Textbook for Class XI

Page No. : 352

Line : 53

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