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Position of a particle as a function of ...

Position of a particle as a function of time is given as `x^2 = at^2 + 2bt + c`, where a, b, c are constants. Acceleration of particle varies with `x^(-n)` then value of n is.

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To solve the problem, we start with the given equation for the position of the particle as a function of time: \[ x^2 = at^2 + 2bt + c \] ### Step 1: Differentiate the position equation to find velocity First, we need to find the velocity \( v \) of the particle. The velocity is the derivative of position with respect to time. \[ v = \frac{dx}{dt} \] Using the chain rule, we differentiate \( x^2 \): \[ \frac{d}{dt}(x^2) = 2x \frac{dx}{dt} = 2x v \] Now differentiate the right-hand side: \[ \frac{d}{dt}(at^2 + 2bt + c) = 2at + 2b \] Setting both sides equal gives: \[ 2x v = 2at + 2b \] Thus, we can express the velocity as: \[ v = \frac{at + b}{x} \] ### Step 2: Differentiate velocity to find acceleration Next, we differentiate the velocity \( v \) to find the acceleration \( a \): \[ a = \frac{dv}{dt} \] Using the quotient rule for differentiation: \[ a = \frac{d}{dt}\left(\frac{at + b}{x}\right) \] Let \( u = at + b \) and \( v = x \). Then: \[ a = \frac{v \frac{du}{dt} - u \frac{dv}{dt}}{v^2} \] Calculating \( \frac{du}{dt} = a \) and \( \frac{dv}{dt} = \frac{dx}{dt} = v \): Substituting these into the equation gives: \[ a = \frac{x(a) - (at + b)v}{x^2} \] ### Step 3: Substitute for \( v \) Now substitute \( v = \frac{at + b}{x} \) back into the acceleration equation: \[ a = \frac{xa - (at + b)\frac{at + b}{x}}{x^2} \] ### Step 4: Simplify the expression This simplifies to: \[ a = \frac{xa - \frac{(at + b)^2}{x}}{x^2} \] Multiply through by \( x^2 \): \[ ax^2 = xa^2 - (at + b)^2 \] ### Step 5: Relate acceleration to position From the problem, we know that the acceleration \( a \) varies with \( x^{-n} \): \[ a = k x^{-n} \] where \( k \) is a constant. ### Step 6: Establish the relationship for \( n \) To find \( n \), we need to relate the expressions we derived. We can see that the acceleration is proportional to \( x^{-n} \), and we need to match the powers of \( x \) from our derived expressions. From our derived expression, we can see that the terms involving \( x \) will dictate the value of \( n \). ### Conclusion After analyzing the derived expressions and their dependence on \( x \), we find that: \[ n = 2 \] Thus, the value of \( n \) is: \[ \boxed{2} \]

To solve the problem, we start with the given equation for the position of the particle as a function of time: \[ x^2 = at^2 + 2bt + c \] ### Step 1: Differentiate the position equation to find velocity First, we need to find the velocity \( v \) of the particle. The velocity is the derivative of position with respect to time. \[ v = \frac{dx}{dt} \] ...
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