To determine the value of \( \beta \), we must compute the work performed by the force \( F = \alpha + \beta x^2 \) over a displacement of 1 meter.
Work done by a force is defined as the integral of the force with respect to displacement:
\(W = \int F \, dx = \int (\alpha + \beta x^2) \, dx\)
The following are given:
We now evaluate the integral:
\(W = \int_0^1 (1 + \beta x^2) \, dx = \left[ x + \frac{\beta x^3}{3} \right]_0^1\)
Applying the limits of integration:
\(W = \left( 1 + \frac{\beta}{3} \right) - \left( 0 + 0 \right) = 1 + \frac{\beta}{3}\)
Equating this result to the given work done:
\(1 + \frac{\beta}{3} = 5\)
Solving for \( \beta \):
Consequently, the determined value for \( \beta \) is 12 N/m².
This value corresponds to the correct answer among the provided options.
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).