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Jump to JupiterThe gravitational potential energy of a 1kg object is plotted versus position from Earth’s surface to the surface of Jupiter. Mostly it is due to the two planets.


Make the crude approximation that this is a rectangular barrier of widthm and approximate height of4X108j/kg. Your mass is 65 kg, and you launch your-self from Earth at an impressive 4 m/s. What is the probability that you can jump to Jupiter?

Short Answer

Expert verified

The probability that one can jump to Jupiter ise-2x1052 using the concept of transmission probability.

Step by step solution

01

Tunneling  

The transmission or tunneling probability can be determined using transmitted intensity and the incident intensity.

In the case of tunneling barriers being wide, it can be found as follows.

T16EU0(1-EU0)e-2L2m(U0-E1)/ħ

Here E is the jump energy, U0is barrier energy, L is the length of the tunnel, and m is the mass of the particle.

02

Given quantities

The given values are: -

  • length of the barrier,L=6X1011m.
  • Height of the barrier,h=4X108J/kg.
  • The mass of the jumper ism=65kg.
  • Launch velocity is given as v=4m/s.
03

Finding the jump energy and the barrier energy

Estimate the jump energy for the launch velocity, v=4 m/sas:

E=12mv2=12x65x4=520J

Find the barrier energy by multiplying the mass with potential height as:

U0=65x4x108=2.6x1010J

04

Finding the transmission probability for the jump

Estimate the value of transmission probability for the jump by putting the obtained values as:

T116E1U0E1U0e-2L2mU0-E1lħ=16x5202.6x1010x1-5202.6x1010e-2x6x10112x652.61010-520/1.05x10-34e-2x1052

Therefore, the probability of the jump to Jupiter will practically be e-2x1052.

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Most popular questions from this chapter

Reflection and Transmission probabilities can be obtained from equations (6-12). The first step is substituting -fork'. (a) Why? (b) Make the substitutions and then use definitions of k and α to obtain equation (6-16).

The equations for Rand T in the E>U0barrier essentially the same as light through a transparent film. It is possible to fabricate a thin film that reflects no light. Is it possible to fabricate one that transmits no light? Why? Why not?

In the E>Uopotential barrier, there should be no reflection when the incident wave is at one of the transmission resonances. Prove this by assuming that a beam of particles is incident at the first transmission resonance, E=Uo+(π2h2/2mL2), and combining continuity equations to show thatB=0. (Note: k’ is particularly simple in this special case, which should streamline your work.)

Could the situation depicted in the following diagram represent a particle in a bound state? Explain.

Solving the potential barrier smoothness conditions for relationships among the coefficients A,B and Fgiving the reflection and transmission probabilities, usually involves rather messy algebra. However, there is a special case than can be done fairly easily, through requiring a slight departure from the standard solutions used in the chapter. Suppose the incident particles’ energyEis preciselyU0.

(a) Write down solutions to the Schrodinger Equation in the three regions. Be especially carefull in the region0<x<L. It should have two arbitrary constants and it isn’t difficult – just different.

(b) Obtain the smoothness conditions, and from these findR and T.

(c) Do the results make sense in the limitL?

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