
To solve this problem, we need to calculate the maximum compression in the spring when the block hits it. We'll use energy conservation principles, factoring in gravitational potential energy, work done by friction, and spring potential energy.
Therefore, the maximum compression in the spring when the block hits the spring is \(2 \, \text{m}\).
Using the work-energy theorem, the total work done by all forces is equal to the change in kinetic energy (\(\Delta KE\)) of the system. Here:
\[w_g + w_{Fr} + w_s = \Delta KE.\]
Substituting the given values:
\[5 \times 10 \times 5 - 0.5 \times 5 \times 10 \times x - \frac{1}{2} Kx^2 = 0 - 0.\]
Simplifying:
\[250 - 25x - 50x^2 = 0.\]
Rewriting:
\[2x^2 + x - 10 = 0.\]
Solving this quadratic equation gives:
\[x = 2.\]
Thus, the maximum compression in the spring is \(x = 2\) m.
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,


What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)