\( \frac{2}{3} \)
\( \frac{1}{2} \)
The work done \( W \) by a force \( \mathbf{F} \) on a particle moving through a displacement \( \mathbf{r} \) is given by the dot product: \[ W = \mathbf{F} \cdot \mathbf{r}. \] Given: \[ \mathbf{F} = 2\hat{i} + b\hat{j} + \hat{k}, \quad \mathbf{r} = \hat{i} - 2\hat{j} - \hat{k}. \] The dot product \( \mathbf{F} \cdot \mathbf{r} \) is: \[ W = (2\hat{i} + b\hat{j} + \hat{k}) \cdot (\hat{i} - 2\hat{j} - \hat{k}). \] Using the properties of the dot product: \[ W = 2(1) + b(-2) + 1(-1) = 2 - 2b - 1 = 1 - 2b. \] For the work to be zero: \[ 1 - 2b = 0 \quad \Rightarrow \quad b = \frac{1}{2}. \] Thus, the value of \( b \) is \( \boxed{\frac{1}{2}} \).
Step 1: Formula for work done.
Work done by a constant force is given by the dot product:
\[
W = \mathbf{F} \cdot \mathbf{r}.
\]
Step 2: Substitute the given vectors.
\[
\mathbf{F} = 2\hat{i} + b\hat{j} + \hat{k}, \quad
\mathbf{r} = \hat{i} - 2\hat{j} - \hat{k}.
\]
\[
W = (2)(1) + (b)(-2) + (1)(-1).
\]
Simplify:
\[
W = 2 - 2b - 1 = 1 - 2b.
\]
Step 3: Use the given condition.
Work done \( W = 0 \), so:
\[
1 - 2b = 0.
\]
\[
b = \frac{1}{2}.
\]
Hence, the correct value of \( b \) is \( \dfrac{1}{2} \).
\[ \boxed{b = \dfrac{1}{2}} \]
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,


A heavy iron bar of weight 12 kg is having its one end on the ground and the other on the shoulder of a man. The rod makes an angle \(60^\circ\) with the horizontal, the weight experienced by the man is :
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 : \(A_2 \rightleftharpoons 2A\)