Start Learning Free

Before You Begin

Question #42032

Difficulty: 8/10 | 🟢 Free

The Question

A particle of mass m=2 kgm = 2 \text{ kg} is constrained to move along the xx-axis under the influence of a conservative force field. The potential energy of the particle is given by U(x)=(−13x3+2x2−3x) JU(x) = \left(-\frac{1}{3}x^3 + 2x^2 - 3x\right) \text{ J}, where xx is the position in meters. If the particle is released from rest at the origin (x=0x = 0), what is its speed when its acceleration becomes zero for the first time?

Options

  • A.

    23 m/s\frac{2}{\sqrt{3}} \text{ m/s}

  • B.

    3 m/s\sqrt{3} \text{ m/s}

  • C.

    32 m/s\sqrt{\frac{3}{2}} \text{ m/s}

  • D.

    223 m/s\frac{2\sqrt{2}}{\sqrt{3}} \text{ m/s}

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

The Velocity-Position Identity|Conservative Force Field|Calculus (Integration)

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to transition from time-domain dynamics to spatial-domain dynamics in a conservative force field.

A common trap is attempting to use constant acceleration kinematic equations (like v2=u2+2asv^2 = u^2 + 2as) by incorrectly assuming the initial acceleration (a=1.5 m/s2a = 1.5 \text{ m/s}^2) remains constant, which leads directly to the trap answer 3 m/s\sqrt{3} \text{ m/s}.

By providing a non-linear potential energy function, the problem forces the explicit use of the vdvdxv \frac{dv}{dx} substitution (or equivalently, the work-energy theorem) to correctly integrate the position-dependent acceleration.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMotion in a Straight Line - Class 11 Part 1
ConceptThe Velocity-Position Identity
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree