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Question: A particle of mass $m$ moves on the x-axis as follows: It starts from rest at $t=0$ from the point $...

A particle of mass mm moves on the x-axis as follows: It starts from rest at t=0t=0 from the point x=0x=0, and comes to rest at t=1t=1 at the point x=1x=1. No other information is available about its motion at intermediate times (0<t<1)(0<t<1). If aa denotes the instantaneous acceleration of the particle, then:

A

aa cannot remain positive for all tt in the interval $0 \leq t \leq 1

B

a|a| cannot exceed 2 at any point in its path

C

a|a| must be 4\geq 4 at some point of points in its path

D

aa must change sign during the motion, but no other assertion can be made with the information given

Answer

Options A and C are correct.

Explanation

Solution

Let x(t)x(t), v(t)v(t), and a(t)a(t) be the position, velocity, and acceleration of the particle at time tt.

We are given the following conditions:

  1. x(0)=0x(0) = 0
  2. v(0)=0v(0) = 0 (starts from rest)
  3. x(1)=1x(1) = 1
  4. v(1)=0v(1) = 0 (comes to rest)

The motion is in the interval 0t10 \leq t \leq 1.

First, let's consider the average velocity:

vˉ=x(1)x(0)10=101=1\bar{v} = \frac{x(1) - x(0)}{1 - 0} = \frac{1 - 0}{1} = 1.

By the Mean Value Theorem for derivatives, there exists t0(0,1)t_0 \in (0, 1) such that v(t0)=vˉ=1v(t_0) = \bar{v} = 1.

Now consider the velocity function v(t)v(t). We have v(0)=0v(0) = 0, v(1)=0v(1) = 0, and v(t0)=1v(t_0) = 1 for some t0(0,1)t_0 \in (0, 1).

Since v(0)=0v(0) = 0 and v(t0)=1v(t_0) = 1, the velocity increases from 0 to 1 in the interval [0,t0][0, t_0].

Since v(t0)=1v(t_0) = 1 and v(1)=0v(1) = 0, the velocity decreases from 1 to 0 in the interval [t0,1][t_0, 1].

Consider Option A: aa cannot remain positive for all tt in the interval 0t10 \leq t \leq 1.

If a(t)>0a(t) > 0 for all t[0,1]t \in [0, 1], then v(t)=v(0)+0ta(τ)dτ=0ta(τ)dτv(t) = v(0) + \int_0^t a(\tau) d\tau = \int_0^t a(\tau) d\tau. Since a(τ)>0a(\tau) > 0 for τ>0\tau > 0, v(t)>0v(t) > 0 for t(0,1]t \in (0, 1]. This contradicts v(1)=0v(1) = 0.

If a(t)0a(t) \geq 0 for all t[0,1]t \in [0, 1], then v(t)v(t) is non-decreasing. Since v(0)=0v(0)=0, v(t)0v(t) \geq 0 for all t[0,1]t \in [0, 1]. If a(t)a(t) is not identically zero on [0,1][0, 1], then v(t)v(t) would be strictly increasing over some interval, leading to v(1)>0v(1) > 0. If a(t)=0a(t) = 0 for all tt, then v(t)=0v(t) = 0 for all tt, which means x(t)=x(0)=0x(t) = x(0) = 0 for all tt, contradicting x(1)=1x(1)=1. Thus, a(t)a(t) cannot be 0\geq 0 for all t[0,1]t \in [0, 1]. Similarly, a(t)a(t) cannot be 0\leq 0 for all t[0,1]t \in [0, 1] (this would lead to v(t)0v(t) \leq 0 and v(1)<0v(1) < 0 unless a(t)=0a(t)=0 everywhere).

Therefore, a(t)a(t) must take both positive and negative values in the interval (0,1)(0, 1). This means aa must change sign.

Option A is correct.

Consider Option D: aa must change sign during the motion, but no other assertion can be made with the information given.

We have shown that aa must change sign. However, we can make other assertions, as we will see by analyzing the magnitude of aa. So, the second part of Option D is incorrect.

Consider the acceleration a(t)=v(t)a(t) = v'(t).

By the Mean Value Theorem applied to v(t)v(t) on the interval [0,t0][0, t_0], there exists t1(0,t0)t_1 \in (0, t_0) such that a(t1)=v(t1)=v(t0)v(0)t00=10t0=1t0a(t_1) = v'(t_1) = \frac{v(t_0) - v(0)}{t_0 - 0} = \frac{1 - 0}{t_0} = \frac{1}{t_0}.

Since t0(0,1)t_0 \in (0, 1), 0<t0<10 < t_0 < 1, so a(t1)=1t0>1a(t_1) = \frac{1}{t_0} > 1.

By the Mean Value Theorem applied to v(t)v(t) on the interval [t0,1][t_0, 1], there exists t2(t0,1)t_2 \in (t_0, 1) such that a(t2)=v(t2)=v(1)v(t0)1t0=011t0=11t0a(t_2) = v'(t_2) = \frac{v(1) - v(t_0)}{1 - t_0} = \frac{0 - 1}{1 - t_0} = \frac{-1}{1 - t_0}.

Since t0(0,1)t_0 \in (0, 1), 0<1t0<10 < 1 - t_0 < 1, so a(t2)=11t0<1a(t_2) = \frac{-1}{1 - t_0} < -1.

Thus, a(t1)=1t0|a(t_1)| = \frac{1}{t_0} and a(t2)=11t0|a(t_2)| = \frac{1}{1 - t_0}.

Since t0(0,1)t_0 \in (0, 1), we have 1t0>1\frac{1}{t_0} > 1 and 11t0>1\frac{1}{1 - t_0} > 1.

At least one of these values must be 2\geq 2. If 1t0<2\frac{1}{t_0} < 2 and 11t0<2\frac{1}{1 - t_0} < 2, then t0>1/2t_0 > 1/2 and 1t0>1/21 - t_0 > 1/2, so t0<1/2t_0 < 1/2. This is a contradiction.

Thus, max(1t0,11t0)2\max(\frac{1}{t_0}, \frac{1}{1 - t_0}) \geq 2.

So, there exists a point where a2|a| \geq 2. This means Option B: a|a| cannot exceed 2 at any point in its path, is incorrect.

Now consider the minimum value that max(a(t1),a(t2))\max(|a(t_1)|, |a(t_2)|) can take. This minimum occurs when 1t0=11t0\frac{1}{t_0} = \frac{1}{1 - t_0}, which implies t0=1/2t_0 = 1/2. In this case, a(t1)=2|a(t_1)| = 2 and a(t2)=2|a(t_2)| = 2. So, there are points where a2|a| \geq 2.

Let M=supt[0,1]a(t)M = \sup_{t \in [0, 1]} |a(t)|. We have Ma(t1)=1/t0M \geq |a(t_1)| = 1/t_0 and Ma(t2)=1/(1t0)M \geq |a(t_2)| = 1/(1-t_0).

So, Mmax(1t0,11t0)M \geq \max(\frac{1}{t_0}, \frac{1}{1-t_0}). Since this holds for any t0t_0 such that v(t0)=1v(t_0)=1, and we know such a t0t_0 exists, Mmint0(0,1)max(1t0,11t0)M \geq \min_{t_0 \in (0, 1)} \max(\frac{1}{t_0}, \frac{1}{1-t_0}). The minimum value is 2, occurring at t0=1/2t_0 = 1/2.

So, the maximum magnitude of acceleration must be at least 2.

Let's try to get a stronger bound using integration.

We have v(t)=0ta(τ)dτv(t) = \int_0^t a(\tau) d\tau.

x(1)x(0)=01v(t)dt=1x(1) - x(0) = \int_0^1 v(t) dt = 1.

Also, v(1)v(0)=01a(t)dt=0v(1) - v(0) = \int_0^1 a(t) dt = 0.

Consider the integral 01ta(t)dt\int_0^1 t a(t) dt. Using integration by parts:

01ta(t)dt=01tv(t)dt=[tv(t)]0101v(t)dt=(1v(1)0v(0))01v(t)dt=(1000)1=1\int_0^1 t a(t) dt = \int_0^1 t v'(t) dt = [t v(t)]_0^1 - \int_0^1 v(t) dt = (1 \cdot v(1) - 0 \cdot v(0)) - \int_0^1 v(t) dt = (1 \cdot 0 - 0 \cdot 0) - 1 = -1.

So, 01ta(t)dt=1\int_0^1 t a(t) dt = -1.

Similarly, consider the integral 01(1t)a(t)dt\int_0^1 (1-t) a(t) dt. Using integration by parts:

01(1t)a(t)dt=01(1t)v(t)dt=[(1t)v(t)]0101(1)v(t)dτ=(0v(1)1v(0))+01v(t)dt=(00)+1=1\int_0^1 (1-t) a(t) dt = \int_0^1 (1-t) v'(t) dt = [(1-t) v(t)]_0^1 - \int_0^1 (-1) v(t) d\tau = (0 \cdot v(1) - 1 \cdot v(0)) + \int_0^1 v(t) dt = (0 - 0) + 1 = 1.

So, 01(1t)a(t)dt=1\int_0^1 (1-t) a(t) dt = 1.

Let M=supt[0,1]a(t)M = \sup_{t \in [0, 1]} |a(t)|.

From 01ta(t)dt=1\int_0^1 t a(t) dt = -1, we have 01ta(t)dt=1|\int_0^1 t a(t) dt| = 1.

01ta(t)dt01ta(t)dt=01ta(t)dt01tMdt=M01tdt=M[t22]01=M12|\int_0^1 t a(t) dt| \leq \int_0^1 |t a(t)| dt = \int_0^1 t |a(t)| dt \leq \int_0^1 t M dt = M \int_0^1 t dt = M [\frac{t^2}{2}]_0^1 = M \cdot \frac{1}{2}.

So, 1M/21 \leq M/2, which implies M2M \geq 2.

From 01(1t)a(t)dt=1\int_0^1 (1-t) a(t) dt = 1, we have 01(1t)a(t)dt=1|\int_0^1 (1-t) a(t) dt| = 1.

01(1t)a(t)dt01(1t)a(t)dt=01(1t)a(t)dt01(1t)Mdt=M01(1t)dt=M[tt22]01=M(112)=M12|\int_0^1 (1-t) a(t) dt| \leq \int_0^1 |(1-t) a(t)| dt = \int_0^1 (1-t) |a(t)| dt \leq \int_0^1 (1-t) M dt = M \int_0^1 (1-t) dt = M [t - \frac{t^2}{2}]_0^1 = M (1 - \frac{1}{2}) = M \cdot \frac{1}{2}.

So, 1M/21 \leq M/2, which implies M2M \geq 2.

This method only guarantees M2M \geq 2.

Let's consider the integral 01(t1/2)a(t)dt\int_0^1 (t - 1/2) a(t) dt.

01(t1/2)a(t)dt=01ta(t)dt1201a(t)dt=112(0)=1\int_0^1 (t - 1/2) a(t) dt = \int_0^1 t a(t) dt - \frac{1}{2} \int_0^1 a(t) dt = -1 - \frac{1}{2}(0) = -1.

So, 01(t1/2)a(t)dt=1|\int_0^1 (t - 1/2) a(t) dt| = 1.

01(t1/2)a(t)dt01t1/2a(t)dt01t1/2Mdt=M01t1/2dt|\int_0^1 (t - 1/2) a(t) dt| \leq \int_0^1 |t - 1/2| |a(t)| dt \leq \int_0^1 |t - 1/2| M dt = M \int_0^1 |t - 1/2| dt.

01t1/2dt=01/2(t1/2)dt+1/21(t1/2)dt=01/2(1/2t)dt+1/21(t1/2)dt\int_0^1 |t - 1/2| dt = \int_0^{1/2} -(t - 1/2) dt + \int_{1/2}^1 (t - 1/2) dt = \int_0^{1/2} (1/2 - t) dt + \int_{1/2}^1 (t - 1/2) dt

=[t2t22]01/2+[t22t2]1/21=(1418)(00)+(1212)(1814)=18+(0)(18)=18+18=14= [\frac{t}{2} - \frac{t^2}{2}]_0^{1/2} + [\frac{t^2}{2} - \frac{t}{2}]_{1/2}^1 = (\frac{1}{4} - \frac{1}{8}) - (0 - 0) + (\frac{1}{2} - \frac{1}{2}) - (\frac{1}{8} - \frac{1}{4}) = \frac{1}{8} + (0) - (-\frac{1}{8}) = \frac{1}{8} + \frac{1}{8} = \frac{1}{4}.

So, 1M141 \leq M \cdot \frac{1}{4}, which implies M4M \geq 4.

Thus, the maximum magnitude of acceleration a|a| must be at least 4 at some point in the path.

This means a|a| must be 4\geq 4 at some point or points in its path.

Option C: a|a| must be 4\geq 4 at some point of points in its path, is correct.

Option B: a|a| cannot exceed 2 at any point in its path. This is incorrect as M4M \geq 4.

Let's summarize:

Option A is correct because aa must change sign.

Option B is incorrect because a|a| must be at least 4 at some point.

Option C is correct because a|a| must be at least 4 at some point.

Option D is incorrect because we can make other assertions (like a4|a| \geq 4 at some point).

Since the question asks for the correct option(s), and this is a multiple choice question, we should check if multiple options can be correct. Based on our analysis, A and C are correct. However, in JEE/NEET, usually only one option is correct unless explicitly stated otherwise. Let's re-read the question and options carefully. The wording suggests that we need to choose one or more assertions that are true.

Let's consider if there's a possibility that only one option is intended to be correct. Option A states that aa cannot remain positive for all tt. This is true and implies aa must change sign (or be zero everywhere, which is ruled out). Option C states that a|a| must be 4\geq 4 at some point. This is a stronger statement about the magnitude of aa. Option D says aa must change sign, but no other assertion can be made. This is false because we could assert a4|a| \geq 4 at some point.

If this were a single-choice question, there might be an issue with the options provided, as both A and C seem correct. However, Option C provides a more specific and stronger conclusion about the motion, which is derived from the given conditions. Option A is a consequence of the velocity starting and ending at zero while displacement is non-zero. Option C is a consequence of the specific values of displacement and time interval.

If forced to choose a single option, Option C is a stronger statement than Option A.

Final Answer: The final answer is A,C\boxed{A, C}