To find the acceleration of a particle from the given velocity function \( v = 4\sqrt{x} \, \text{m/s} \), we need to calculate the derivative of velocity with respect to time \( t \), which will give us the acceleration \( a \).
Step 1: First, express velocity in terms of position using the chain rule:
\( v = \frac{dx}{dt} \) and \( a = \frac{dv}{dt} = \frac{dv}{dx} \cdot \frac{dx}{dt} \)
Step 2: Substitute \( v \) for \( \frac{dx}{dt} \):
\( a = v \cdot \frac{dv}{dx} \)
Step 3: Next, differentiate \( v = 4\sqrt{x} \) with respect to \( x \):
\[ \frac{dv}{dx} = \frac{d}{dx} \left( 4\sqrt{x} \right) = 4 \cdot \frac{1}{2\sqrt{x}} = \frac{2}{\sqrt{x}} \]
Step 4: Substituting this back into the expression for acceleration:
\( a = (4\sqrt{x}) \cdot \frac{2}{\sqrt{x}} = 8 \)
Final Answer: Thus, the acceleration of the particle is \( 8 \, \text{m/s}^2 \).
Verification: Verify that this value falls within the given range \( 8, 8 \)
Given: - Velocity of the particle: \( v = 4\sqrt{x} \, \mathrm{m/s} \) - The particle starts from rest at \( x = 0 \).
The velocity \( v \) is given by: \[ v = 4\sqrt{x} \] Squaring both sides: \[ v^2 = (4\sqrt{x})^2 = 16x \]
The acceleration \( a \) is given by: \[ a = v \frac{dv}{dx} \] Differentiating \( v^2 = 16x \) with respect to \( x \): \[ \frac{d(v^2)}{dx} = 16 \] Using the chain rule: \[ 2v \frac{dv}{dx} = 16 \] Rearranging: \[ v \frac{dv}{dx} = 8 \] Thus, the acceleration is: \[ a = 8 \, \mathrm{ms^{-2}} \]
Conclusion: The acceleration of the particle is \( 8 \, \mathrm{ms^{-2}} \).
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 : \(A_2 \rightleftharpoons 2A\)