Given the particle's displacement \(x\) and time \(t\) are related by \(x^2 = 1 + t^2\). The particle's acceleration is expressed as \(x^{-n}\). Determine the value of \(n\).
The calculation requires determining the particle's acceleration, defined as the second derivative of displacement with respect to time. The core steps involve:
Step 1: Calculate the velocity (\(v\)) by differentiating the provided equation with respect to time \(t\).
The governing relation is:
\[x^2 = 1 + t^2\]Differentiating both sides with respect to \(t\):
\[\frac{d}{dt}(x^2) = \frac{d}{dt}(1 + t^2)\]Applying the chain rule on the left side yields:
\[2x \frac{dx}{dt} = 2t\]Substituting \(v = \frac{dx}{dt}\):
\[2xv = 2t\]Solving for \(v\):
\[v = \frac{t}{x}\]Step 2: Determine the acceleration (\(a\)) by differentiating the velocity with respect to time \(t\).
Using \(a = \frac{dv}{dt}\) and the quotient rule for \(v = \frac{t}{x}\):
\[a = \frac{d}{dt}\left(\frac{t}{x}\right) = \frac{x \frac{d(t)}{dt} - t \frac{d(x)}{dt}}{x^2}\]Given that \(\frac{d(t)}{dt} = 1\) and \(\frac{dx}{dt} = v\), the expression simplifies to:
\[a = \frac{x(1) - t(v)}{x^2} = \frac{x - tv}{x^2}\]Step 3: Substitute the expression for velocity \(v\) into the acceleration equation.
Replacing \(v\) with \(\frac{t}{x}\) in the acceleration equation:
\[a = \frac{x - t\left(\frac{t}{x}\right)}{x^2} = \frac{x - \frac{t^2}{x}}{x^2}\]Simplifying the compound fraction by multiplying the numerator and denominator by \(x\):
\[a = \frac{x^2 - t^2}{x^3}\]Step 4: Rewrite the acceleration solely in terms of \(x\).
From the initial equation \(x^2 = 1 + t^2\), it follows that \(t^2 = x^2 - 1\). Substituting this into the acceleration expression:
\[a = \frac{x^2 - (x^2 - 1)}{x^3}\]\[a = \frac{x^2 - x^2 + 1}{x^3} = \frac{1}{x^3}\]Step 5: Equate the derived acceleration with the given form to solve for \(n\).
The computed acceleration is \(a = \frac{1}{x^3}\), which is equivalent to:
\[a = x^{-3}\]Comparing this with the provided acceleration form \(x^{-n}\):
\[x^{-n} = x^{-3}\]This comparison directly yields \(n = 3\).
The value of \(n\) is 3.
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 