The force constant ($k$) of a spring is inversely proportional to its length ($L$). This fundamental property means that the product of the force constant and length remains constant for segments derived from the same original spring. Mathematically, this is expressed as $k \propto \frac{1}{L}$, or $k \cdot L = \text{constant}$.
When a spring is cut, each resulting piece retains this characteristic. If the original spring has a force constant $k_{orig}$ and length $L$, and it is cut into pieces with lengths $L_1, L_2, \dots$ and corresponding force constants $k_1, k_2, \dots$, then the relationship $k_1 L_1 = k_2 L_2 = \dots = k_{orig} L$ holds true.
The problem states the spring is cut into two pieces with a length ratio of 1:3. Let the original length of the spring be $L$. The lengths of the two pieces ($L_1$ and $L_2$) are determined as follows:
The initial force constant of the spring is given as $k_{orig} = 15$ N/m. We can now calculate the force constants ($k_1$ and $k_2$) for the two pieces using the constant product principle ($k \cdot L = \text{constant}$):
The two pieces have calculated force constants of 60 N/m and 20 N/m. The piece with the smaller length ($L_1 = L/4$) has a force constant of 60 N/m, while the piece with the larger length ($L_2 = 3L/4$) has a force constant of 20 N/m. The question asks for the force constant of the smaller piece.
The calculated force constant is 20 N/m.
A cylindrical tube AB of length $l$, closed at both ends contains an ideal gas of 1 mol having molecular weight $M$. The tube is rotated in a horizontal plane with constant angular velocity $\omega$ about an axis perpendicular to AB and passing through the edge at end A, as shown in the figure. If $P_A$ and $P_B$ are the pressures at $A$ and $B$ respectively, then
(Consider the temperature is same at all points in the tube)

A uniform bar of length 12 cm and mass $20m$ lies on a smooth horizontal table. Two point masses $m$ and $2m$ are moving in opposite directions with same speed of $v$ and in the same plane as the bar, as shown in figure. These masses strike the bar simultaneously and get stuck to it. After collision the entire system is rotating with angular frequency $\omega$. The ratio of $v$ and $\omega$ is :
Match the LIST-I with LIST-II
| List-I: | List-II: |
| A. Magnetic induction | I. $[M L T^{-2} A^{-2}]$ |
| B. Magnetic flux | II. $[M L^2 T^{-2} A^{-2}]$ |
| C. Magnetic permeability | III. $[M L^0 T^{-2} A^{-1}]$ |
| D. Self inductance | IV. $[M L^2 T^{-2} A^{-1}]$ |
Choose the correct answer from the options given below:
A cylindrical tube AB of length $l$, closed at both ends contains an ideal gas of 1 mol having molecular weight $M$. The tube is rotated in a horizontal plane with constant angular velocity $\omega$ about an axis perpendicular to AB and passing through the edge at end A, as shown in the figure. If $P_A$ and $P_B$ are the pressures at $A$ and $B$ respectively, then
(Consider the temperature is same at all points in the tube)
