To solve this question, we need to find the velocity of a body after it has been influenced by a constant force for a specific duration.
Given:
To find the final velocity, we can use the equation of motion under constant acceleration:
\(\vec{v}_{\text{final}} = \vec{v}_{\text{in}} + \vec{a} \cdot t\)
First, let's calculate the acceleration using Newton's second law:
\(\vec{F} = m \cdot \vec{a} \Longrightarrow \vec{a} = \frac{\vec{F}}{m} = \frac{6 \hat{k}}{2} = 3 \hat{k} \, \text{ms}^{-2}\)
Substitute the values into the velocity equation:
\(\vec{v}_{\text{final}} = (3 \hat{i} + 4 \hat{j}) + (3 \hat{k}) \cdot \frac{5}{3}\)
Further simplify the equation:
\(\vec{v}_{\text{final}} = 3 \hat{i} + 4 \hat{j} + 5 \hat{k}\)
Thus, the velocity of the body when it emerges from the force field is: \(3 \hat{i} + 4 \hat{j} + 5 \hat{k}\).
Hence, the correct answer is:
\( 3 \hat{i} + 4 \hat{j} + 5 \hat{k} \)
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,



The driver sitting inside a parked car is watching vehicles approaching from behind with the help of his side view mirror, which is a convex mirror with radius of curvature \( R = 2 \, \text{m} \). Another car approaches him from behind with a uniform speed of 90 km/hr. When the car is at a distance of 24 m from him, the magnitude of the acceleration of the image of the side view mirror is \( a \). The value of \( 100a \) is _____________ m/s\(^2\).
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 : \(A_2 \rightleftharpoons 2A\)