Mechanics questions from Oxford Physics entrance exam.

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SUMMARY

The discussion centers on a mechanics question from the Oxford Physics entrance exam involving a point-like object with mass m = 1 kg, starting from rest at x0 = 10 m, and subject to a force F(x) that varies with position. Participants analyze how to derive velocity as a function of time, noting the challenges posed by the transition from ballistic motion in x ≥ 0 to sinusoidal oscillation in x < 0. The force is defined piecewise, with F(x) = -10 for x ≥ 0 and F(x) = -10 - x for x < 0, leading to a second-order differential equation that describes the motion.

PREREQUISITES
  • Understanding of Newton's second law (F = ma)
  • Familiarity with ordinary differential equations (ODEs)
  • Knowledge of kinetic energy and its graphical representation
  • Concepts of ballistic motion and harmonic oscillation
NEXT STEPS
  • Study the derivation of velocity and acceleration from second-order differential equations
  • Explore the relationship between force, mass, and motion in one-dimensional systems
  • Learn about piecewise functions and their applications in physics
  • Investigate the principles of energy conservation in oscillatory systems
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Physics students preparing for entrance exams, educators teaching mechanics, and anyone interested in advanced concepts of motion and forces in one-dimensional systems.

Mr.A.Gibson
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I'm ok with this question up until a3, I have no idea how to get velocity as a function of time from the information available. This question is taken from the Oxford Physics entrance exam. I'm not sure if it's a miss-print, perhaps the questions should be as a function of x, because that seems a lot easier and a similar level to questions from other years. Or perhaps I'm missing something.

22. A point like object with mass m = 1 kg starts from rest at point x0 = 10 m and moves without any friction under a force F which depends on the coordinate x as illustrated in figure below. The motion is confined to one dimension along x.

http://theonlinephysicstutor.com/Blog/Entries/2012/7/12_Entry_1_files/shapeimage_2.png

a1 What is its speed at x=0? [2]
a2 Sketch its kinetic energy as a function of x. [4]
a3 Sketch its velocity as well as its acceleration as a function of time t. [6]

Now consider a case when, in addition, a friction force of a magnitude of 1 N is present for x ≥ 0.
b1 Sketch how the velocity depends on x in that case. [6]
b2 How many meters this point like object traveled during the time when its position coordinate x was ≥ 0? [2]
 
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Mr.A.Gibson said:
I'm ok with this question up until a3, I have no idea how to get velocity as a function of time from the information available. This question is taken from the Oxford Physics entrance exam. I'm not sure if it's a miss-print, perhaps the questions should be as a function of x, because that seems a lot easier and a similar level to questions from other years. Or perhaps I'm missing something.

22. A point like object with mass m = 1 kg starts from rest at point x0 = 10 m and moves without any friction under a force F which depends on the coordinate x as illustrated in figure below. The motion is confined to one dimension along x.

http://theonlinephysicstutor.com/Blog/Entries/2012/7/12_Entry_1_files/shapeimage_2.png

a1 What is its speed at x=0? [2]
a2 Sketch its kinetic energy as a function of x. [4]
a3 Sketch its velocity as well as its acceleration as a function of time t. [6]

You are given the force on the object and told its mass. Thus you have
<br /> ma = F(x)<br />
or
<br /> m\ddot x = F(x)<br />
You can determine an expression for F(x) from the graph. From there you can hopefully solve the resulting ODE for x, and then determine \dot x and \ddot x by differentiation.
 
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Surely that will give you acceleration and velocity as a function of displacement not time? Since F and x vary with time i can't see how to make the differential work, in fact I cannot get any equation as a function of time.
 
Based on the graph,
<br /> F(x) = \begin{cases}<br /> -10, &amp; x \geq 0 \\<br /> -10 - x, &amp; x &lt; 0<br /> \end{cases}<br />

Conveniently m = 1\,\mathrm{kg} so we have
<br /> \frac{d^2x}{dt^2} = \begin{cases}<br /> -10, &amp; x \geq 0 \\<br /> -10 - x, &amp; x &lt; 0<br /> \end{cases}<br />

It's not necessary to solve this ODE so long as you recognise this as ballistic motion in x \geq 0 and sinusoidal oscillation about x = -10 in x &lt; 0. Basically when x &gt; 0 the particle behaves as it would under constant gravity, but in x &lt; 0 it's suddenly attached to a Hookean spring. Both of these should be covered in either A-level physics or maths/further maths, so should be familiar to someone sitting an Oxford physics entrance paper.

The difficulty is to patch together ballistic motion in x &gt; 0 with sinusoidal motion in x &lt; 0 in such a manner that both velocity and acceleration are continuous when the particle is at the origin. This requires finding the times at which x(t) = 0. In fact the motion is periodic in time; this follows from consideration of the KE graph.
 
pasmith said:
so long as you recognise this as ballistic motion in x \geq 0 and sinusoidal oscillation about x = -10 in x &lt; 0.

Thanks, that's the part I missed.
 

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