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Position, Heisenberg’s uncertainty principle

The rest of the atom is sparsely populated but also vibrant and dynamic. The ghostly electrons are arranged in vague clouds and have no clearly defined position. Heisenberg s Uncertainty Principle (1927) tells us that we can t pin-point their positions. Instead, we have to talk in terms of the probability of there being electrons of a certain energy in certain positions (or orbits) around the nucleus at certain times. [Pg.82]

Heisenberg uncertainty principle The impossibility of making simultaneous measurements of both the position and the momentum of a subatomic particle (e.g. an electron) with unlimited accuracy. The uncertainty arises because, in order to detect the particle, radiation has to be bounced off it, and this process itself disrupts the particle s position. Heisenberg s uncertainty principle is not a consequence of experimental error . It represents a fundamental limit to objective scientific observation, and arises from the wave-particle duality of particles and radiation. In one direction, the uncertainty in position Ax and momentum Ap are related by AxAp h/4K, where h is the Planck constant. It is named for the German physicist... [Pg.105]

J s are the operators corresponding to spin around the z-axis. In other words, we can measure the z-spin states of the two particles simultaneously. In contrast, it is impossible to measure both the x- and z-spins of a single particle simultaneously nor is it possible to measure both the position and the momentum of a dynamical particle simultaneously, by Heisenberg s uncertainty principle. The independence of our two measurements is crucial. [Pg.341]

If the entering particle was in a mixed state (relative to the r-spin measurement), then the act of measurement changes the state of the particle. No one understands how this happens, but it is an essential feature of the quantum mechanical model. For example, this phenomenon contributes to Heisenberg s uncertainty principle, whose most famous implication is that one cannot measure both the position and the momentum of a particle exactly. The point is that a position measurement changes the state of tlie particle in a way that erases information about the momentum, and vice versa. [Pg.343]

Our understanding of the basic nature of matter is limited by Heisenberg s uncertainty principle. Stated simply, this principle implies that our measurements of the position and momentum of a particle of subatomic mass arc always in error when radiation is used to study matter. If x... [Pg.16]

The result expressed in eqn 2.40 shows that to represent localized particles in the wave theory we must accept a limitation in how accurately we can define their positions and momenta the more closely we need to know one, die greater the range of possibilities for the other. This equation expresses the limits imposed by Heisenberg s uncertainty principle, normally written as... [Pg.32]

In the Quantum picture of the world, each individual event cannot be determined exactly, but has to be described by a wave of probability. There is a kind of polarity between the position and energy of any particle in which they cannot be simultaneously determined. This was not a failing of experimental method but a property of the kinds of mathematical structures that physicists have to use to describe this realm of the world. The famous equation of Quantum theory embodying Heisenberg s Uncertainty Principle is ... [Pg.6]

As far as Heisenberg s uncertainty principle is concerned, why is it impossible to determine the exact position and momentum of an electron simultaneously ... [Pg.21]

How do kinetic isotope effects come about Even in its lowest energy state a covalent bond never stops vibrating. If it did it would violate a fundamental physical principle, Heisenberg s uncertainty principle, which states that position and momentum cannot be known exactly at the same time a nonvibrating pair of atoms have precisely zero momentum and precisely fixed locations. The minimum vibrational energy a bond can have is called the zero point energy (Eo) - given by the expression Eq = j/iv. [Pg.487]

The imprecise nature of Schrodinger s model was supported shortly afterwards by a principle proposed by Werner Heisenberg, in 1927. Heisenberg demonstrated that it is impossible to know both an electron s pathway and its exact location. Heisenberg s uncertainty principle is a mathematical relationship that shows that you can never know both the position and the momentum of an object beyond a certain measure of precision. [Pg.657]

This illustration may be regarded as an example of Heisenberg s Uncertainty Principle, which can be stated in the following form The more accurately the velocity of an electron is defined, the less certainly is its position known and, conversely, the more accurate the definition of the position of an electron, the less precise is the value of its velocity Expressed mathematically this becomes... [Pg.8]

The extent to which statistical concepts enter the picture as we go from the micro- to the macroworld is not at all at our disposal. For example, quantum mechanics as we know it today teaches us that it is impossible in principle to obtain complete information about a microscopic entity (i.e., the precise and simultaneous knowledge of an electron s location and momentum, say) at any instant in time. On account of Heisenberg s Uncertainty Principle, conjugate quantities like, for instance, position and momentum can only be known with a certain maximum precision. Quantum mechanics therefore already deals with averages only (i.e., expectation values) when it comes to actual measurements. [Pg.36]

It is noteworthy that the width of an absorption signal is inversely proportional to the lifetime of the excited state (Heisenberg s uncertainty principle). Hence, for gases, the lifetime is long and the absorption lines are sharp. This is why small di- or triatomic molecules sampled in the gas state and at low pressures can lead to spectra containing narrow regular bands whose positions enable the elucidation of the various energetic states predicted by the theory. [Pg.209]

Unlike a trajectory in classical mechanics, the wave function depends only on the space-spin coordinates x, jLi of the electrons in the system, and not on their momenta This lack of dependence of the wave function on the momenta reflects Heisenberg s uncertainty principle which in turn arises from the non-commutativity of conjugate pairs of position and momentum operators. [Pg.484]

If an electron has wave-like properties, there is an important and difficult consequence it becomes impossible to know exactly both the momentum and position of the electron at the same instant in time. This is a statement of Heisenberg s uncertainty principle. In order to get around this problem, rather than trying to define its exact position and momentum, we use the probability of finding the electron in a given volume of space. The probability of finding an electron at a given point in space is determined from the function ij where is a mathematical function which describes the behaviour of an electron-wave ip is the wavefunction. [Pg.6]


See other pages where Position, Heisenberg’s uncertainty principle is mentioned: [Pg.389]    [Pg.389]    [Pg.131]    [Pg.459]    [Pg.424]    [Pg.389]    [Pg.389]    [Pg.131]    [Pg.459]    [Pg.424]    [Pg.1035]    [Pg.486]    [Pg.29]    [Pg.16]    [Pg.10]    [Pg.90]    [Pg.29]    [Pg.47]    [Pg.139]    [Pg.614]    [Pg.90]    [Pg.90]    [Pg.58]    [Pg.75]    [Pg.928]    [Pg.26]    [Pg.29]    [Pg.205]    [Pg.205]    [Pg.343]    [Pg.51]    [Pg.9]    [Pg.90]    [Pg.40]   
See also in sourсe #XX -- [ Pg.296 , Pg.297 ]




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