Step 1: Analyzing the term \( \frac{\partial^2 \vec{r}}{\partial s^2} \) The position vector \( \vec{r}(s) \) represents the shape of the elastic rod, and \( s \) is the arc length, which has the dimension of length \( L \). The second derivative \( \frac{\partial^2 \vec{r}}{\partial s^2} \) represents the curvature of the rod. The curvature has the dimension of inverse length \( L^{-1} \), because it describes the rate of change of the angle per unit length. Thus, \( \left( \frac{\partial^2 \vec{r}}{\partial s^2} \right)^2 \) will have the dimension of \( L^{-2} \).
Step 2: Analyzing the integral term \( \int_0^l \left( \frac{\partial^2 \vec{r}}{\partial s^2} \right)^2 \, ds \) The integral is over the length of the rod, \( l \), which has the dimension of length \( L \). Since the integrand has the dimension of \( L^{-2} \), the entire integral will have the dimension of: \[ \left[ \int_0^l \left( \frac{\partial^2 \vec{r}}{\partial s^2} \right)^2 \, ds \right] = L^{-2} \times L = L^{-1}. \] Step 3: Analyzing the bending energy \( E \) The bending energy \( E \) has the dimension of energy, which is \( M L^2 T^{-2} \) (mass × length² × time⁻²). Step 4: Determining the dimension of \( K \) Now, we can equate the dimensions of both sides of the equation for bending energy: \[ E = K \times L^{-1}. \] Substituting the dimensions of \( E \) and \( L^{-1} \): \[ M L^2 T^{-2} = [K] \times L^{-1}. \] Solving for \( [K] \), we get: \[ [K] = M L^3 T^{-2}. \] Thus, the dimension of \( K \) is \( M L^3 T^{-2} \).
Match List-I with List-II.
| List-I (A) Coefficient of viscosity (B) Intensity of wave (C) Pressure gradient (D) Compressibility | List-II (I) [ML-1T-1] (II) [MT-3] (III) [ML-2T-2] (IV) [M-1LT2] |
The equation for real gas is given by $ \left( P + \frac{a}{V^2} \right)(V - b) = RT $, where $ P $, $ V $, $ T $, and $ R $ are the pressure, volume, temperature and gas constant, respectively. The dimension of $ ab $ is equivalent to that of: