Step 1: Apply the principle of homogeneity of dimensions.
The principle of homogeneity of dimensions states that in a valid physical equation, the dimensions of each term on both sides of the equation must be the same. Also, quantities that are added or subtracted must have the same dimensions. The given equation for velocity \(v\) is: \[ v = at + \frac{b}{t+c} \] The dimension of velocity \([v]\) is \(LT^{-1}\) (Length per unit Time). The dimension of time \([t]\) is \(T\).
Step 2: Determine the dimension of \(c\).
In the term \((t+c)\) in the denominator, \(t\) and \(c\) are added. For quantities to be added, they must have the same dimensions.
Therefore, the dimension of \(c\) must be the same as the dimension of \(t\). \[ [c] = [t] = T \]
Step 3: Determine the dimension of \(a\).
Consider the term \(at\). According to the principle of homogeneity, the dimension of \(at\) must be equal to the dimension of \(v\). \[ [at] = [v] \] \[ [a][t] = LT^{-1} \] Substitute the dimension of \(t\): \[ [a]T = LT^{-1} \] Solve for \([a]\): \[ [a] = \frac{LT^{-1}}{T} = LT^{-1}T^{-1} = LT^{-2} \]
Step 4: Determine the dimension of \(b\).
Consider the term \(\frac{b}{t+c}\). Its dimension must also be equal to the dimension of \(v\). \[ \left[\frac{b}{t+c}\right] = [v] \] We already found that \([t+c] = T\) (since \(t\) and \(c\) have dimension \(T\)). \[ \frac{[b]}{T} = LT^{-1} \] Solve for \([b]\): \[ [b] = LT^{-1} \cdot T = L \]
Step 5: Summarize the dimensions.
The dimensions are:
Dimension of a: \(LT^{-2}\)
Dimension of b: \(L\)
Dimension of c: \(T\)
Thus, the dimensions of a, b, c are respectively \(LT^{-2}, L, T\).
The final answer is $\boxed{LT^{-2}, L, T}$.
A temperature difference can generate e.m.f. in some materials. Let $ S $ be the e.m.f. produced per unit temperature difference between the ends of a wire, $ \sigma $ the electrical conductivity and $ \kappa $ the thermal conductivity of the material of the wire. Taking $ M, L, T, I $ and $ K $ as dimensions of mass, length, time, current and temperature, respectively, the dimensional formula of the quantity $ Z = \frac{S^2 \sigma}{\kappa} $ is:
If \( \vec{u}, \vec{v}, \vec{w} \) are non-coplanar vectors and \( p, q \) are real numbers, then the equality:
\[ [3\vec{u} \quad p\vec{v} \quad p\vec{w}] - [p\vec{v} \quad \vec{w} \quad q\vec{u}] - [2\vec{w} \quad q\vec{v} \quad q\vec{u}] = 0 \]
holds for:
Statement-I: In the interval \( [0, 2\pi] \), the number of common solutions of the equations
\[ 2\sin^2\theta - \cos 2\theta = 0 \]
and
\[ 2\cos^2\theta - 3\sin\theta = 0 \]
is two.
Statement-II: The number of solutions of
\[ 2\cos^2\theta - 3\sin\theta = 0 \]
in \( [0, \pi] \) is two.
If \( A \) and \( B \) are acute angles satisfying
\[ 3\cos^2 A + 2\cos^2 B = 4 \]
and
\[ \frac{3 \sin A}{\sin B} = \frac{2 \cos B}{\cos A}, \]
Then \( A + 2B = \ ? \)