To solve the given problem, we need to understand the behavior of the velocity of a particle whose displacement is described by the equation:
x = ae^{-\alpha t} + be^{\beta t}
where a, b, \alpha, and \beta are positive constants.
- First, let's find the expression for velocity v. Velocity is the time derivative of displacement, so we differentiate x with respect to time t:
v = \frac{dx}{dt} = \frac{d}{dt}(ae^{-\alpha t} + be^{\beta t})
Using the chain rule, we have:
v = -a\alpha e^{-\alpha t} + b\beta e^{\beta t}
- Now, let's analyze the behavior of the velocity over time:
- The term -a\alpha e^{-\alpha t} exponentially decays to zero as time t increases since e^{-\alpha t} decreases.
- The term b\beta e^{\beta t} exponentially increases with time since e^{\beta t} increases.
- Therefore, as time progresses, the positive term b\beta e^{\beta t} will dominate the negative term, causing the overall velocity v to increase over time.
From this analysis, we can conclude that the velocity of the particle goes on increasing with time, thus justifying the correct answer:
go on increasing with time
The incorrect options can be ruled out as follows:
- "be independent of \beta": This is incorrect because \beta directly affects the growth rate of the positive exponential term b\beta e^{\beta t}.
- "drop to zero when \alpha = \beta": While velocities can cancel under specific conditions, in this scenario, the terms will not generally cancel at \alpha = \beta, especially since a and b could still be different.
- "go on decreasing with time": This is incorrect as the velocity's positive term grows with time and will eventually dominate.