\( \frac{2}{3} \)
\( \frac{1}{2} \)
The work \( W \) performed by a force \( \mathbf{F} \) over a displacement \( \mathbf{r} \) is computed via the dot product: \[ W = \mathbf{F} \cdot \mathbf{r}. \] The provided force and displacement vectors are: \[ \mathbf{F} = 2\hat{i} + b\hat{j} + \hat{k}, \quad \mathbf{r} = \hat{i} - 2\hat{j} - \hat{k}. \] Calculating the dot product \( \mathbf{F} \cdot \mathbf{r} \): \[ W = (2\hat{i} + b\hat{j} + \hat{k}) \cdot (\hat{i} - 2\hat{j} - \hat{k}). \] Applying the dot product properties: \[ W = 2(1) + b(-2) + 1(-1) = 2 - 2b - 1 = 1 - 2b. \] For the work to be zero: \[ 1 - 2b = 0 \quad \Rightarrow \quad b = \frac{1}{2}. \] Consequently, \( b \) equals \( \boxed{\frac{1}{2}} \).
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).