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Dot product of vectors

The dot (or scalar) product is actually the product of the magnitude of two vectors and the cosine between them. The cosine of 90° is equal to zero, so the dot product of vectors perpendicular (orthogonal) to each is equal to zero. The unit vectors in the Cartesian coordinates are in an orthogonal axes therefore, their mixed dot products are equal to zero. Thus,... [Pg.79]

Recall that L contains the frequency or (equation (B2.4.8)). To trace out a spectrum, equation (B2.4.11)) is solved for each frequency. In order to obtain the observed signal v, the sum of the two individual magnetizations can be written as the dot product of two vectors, equation (B2.4.12)). [Pg.2096]

In Liouville space, both the density matrix and the operator are vectors. The dot product of these Liouville space... [Pg.2100]

APPENDIX - SUMMARY OF VECTOR AND TENSOR ANALYSIS The scalar (dot) product of two vectors is a number found as... [Pg.254]

The vector (dot) product of a tensor with a vector is found as follows... [Pg.260]

The matrix A in Eq. (7-21) is comprised of orthogonal vectors. Orthogonal vectors have a dot product of zero. The mutually perpendicular (and independent) Cartesian coordinates of 3-space are orthogonal. An orthogonal n x n such as matr ix A may be thought of as n columns of n-element vectors that are mutually perpendicular in an n-dimensional vector space. [Pg.207]

The easiest way to proceed is to use vectors to describe this part of the problem. We represent the distance between the pair of scattering sites by the vector OP the length of which is simply r. To express di and d2 in terms of OP we construct the unit vectors a and b which are parallel to the incident and scattered directions, respectively. The projection of OP into direction a, given by the dot product of these two vectors, equals dj. Likewise, the projection of OP into direction b gives d2. Therefore we can write... [Pg.699]

In the final stage of this involved derivation, we have to free Eq. (10.78) from the dependence it contains on the geometry of Fig. 10.11. The problem lies in the dot product of the vector rj, -which replaces OP in Fig. 10.11-and... [Pg.700]

If the dot product of two vectors is equal to zero, those vectors are orthogonal (perpendicular) to each other. For example, the dot product of the vectors ... [Pg.165]

The force / and displacement s are vector quantities, and equation (2.5) indicates that the vector dot product of the two gives a scalar quantity. The result of this operation is equation (2.6)... [Pg.38]

The value of the dot product is a measure of the coalignment of two vectors and is independent of the coordinate system. The dot product therefore is a true scalar, the simplest invariant which can be formed from the two vectors. It provides a useful form for expressing many physical properties the work done in moving a body equals the dot product of the force and the displacement the electrical energy density in space is proportional to the dot product of electrical intensity and electrical displacement quantum mechanical observations are dot products of an operator and a state vector the invariants of special relativity are the dot products of four-vectors. The invariants involving a set of quantities may be used to establish if these quantities are the components of a vector. For instance, if AiBi forms an invariant and Bi are the components of a vector, then Az must be the components of another vector. [Pg.5]

Instead of the dot product the vector product of the nabla operator can also be formed to produce a function called curl or rot,... [Pg.28]

Four-vectors for which the square of the magnitude is greater than or equal to zero are called space-like when the squares of the magnitudes are negative they are known as time-like vectors. Since these characteristics arise from the dot products of the vectors with reference to themselves, which are world scalars, the designations are invariant under Lorentz transformation[17], A space-like 4-vector can always be transformed so that its fourth component vanishes. On the other hand, a time-like four-vector must always have a fourth component, but it can be transformed so that the first three vanish. The difference between two world points can be either space-like or time-like. Let be the difference vector... [Pg.147]

It is to be expected that the equations relating electromagnetic fields and potentials to the charge current, should bear some resemblance to the Lorentz transformation. Stating that the equations for A and (j> are Lorentz invariant, means that they should have the same form for any observer, irrespective of relative velocity, as long as it s constant. This will be the case if the quantity (Ax, Ay, Az, i/c) = V is a Minkowski four-vector. Easiest would be to show that the dot product of V with another four-vector, e.g. the four-gradient, is Lorentz invariant, i.e. to show that... [Pg.151]

Table 1.1 Conjugate pairs of variables in work terms for the fundamental equation for the internal energy U. Here/is force of elongation, Z is length in the direction of the force, <7 is surface tension, As is surface area, , is the electric potential of the phase containing species i, qi is the contribution of species i to the electric charge of a phase, E is electric field strength, p is the electric dipole moment of the system, B is magnetic field strength (magnetic flux density), and m is the magnetic moment of the system. The dots indicate scalar products of vectors. Table 1.1 Conjugate pairs of variables in work terms for the fundamental equation for the internal energy U. Here/is force of elongation, Z is length in the direction of the force, <7 is surface tension, As is surface area, <Z>, is the electric potential of the phase containing species i, qi is the contribution of species i to the electric charge of a phase, E is electric field strength, p is the electric dipole moment of the system, B is magnetic field strength (magnetic flux density), and m is the magnetic moment of the system. The dots indicate scalar products of vectors.
There are established criteria for obtaining b by using diffraction contrast (23). Briefly, the dislocation intensity (contrast) is mapped in several Bragg reflections (denoted by vector, g) by tilting the crystal to different reflections and determining the dot product of the vectors g and b (called the g b product analysis). [Pg.202]

Equation (A.7) is referred to as the inner product, or dot product, of two vectors. If the two vectors are orthogonal, then xTy = 0. In two or three dimensions, this means that the vectors x and y are perpendicular to each other. [Pg.587]

The reason why the relationship in Equation 7.41 is called the differential virial theorem is because if we take the dot product of both sides with vector r, multiply both sides by pir), and then integrate over the entire volume, it gives... [Pg.99]

The trace of a scalar is the scalar itself. Since the inner (dot) product of two vectors xn and y is a scalar, we can write... [Pg.61]

In the virtual mineral space, the rock composition is projected onto the plane made by the vectors enstatite [0,1,0]T and diopside [0,0,1]T. Although these vectors are not orthogonal in the original oxide composition space, which can be verified by constructing the dot product of columns 2 and 3 in the matrix BT, the particular choice of the projection makes the vectors orthogonal in the transformed space. According to the projector theory developed above, we project the rock composition onto the column-space of the matrix A such that... [Pg.71]

As a particular case, the gradient of a scalar quantity obtained as the dot product of the constant column vector nfiij,...,u ) and the column vector x (x1 ...,x ) is the vector itself for... [Pg.138]

It is possible to be consistent with our E and C equation and view intermolecular interactions in terms of concepts we could call hardness, softness and strength. However, in doing this, we will have to modify the qualitative ideas presented by Pearson (2) about what hardness and softness mean, vide infra. The approach involves converting the E and C equation to polar coordinates. Our acids and bases are represented as vectors in E and C space in Fig. 7. The dot product of these two vectors is given as... [Pg.126]

Problem 8-12. Verify that if -ip is an eigenfunction of H with eigenvalue , then the expectation value of the energy is equal to . The expression (/, g) is called the inner product of fund g. It has a number of properties analogous to those of the dot product of two vectors. These are illustrated in Table 8.2. [Pg.77]

This expression now defines the dot or inner product (Hermitian inner product) for vectors which can have complex valued components. We use this definition so the dot product of a complex valued vector with itself is real. [Pg.615]

You can treat the characters of matrices as vectors and take the dot product of Ai with Dd)... [Pg.676]


See other pages where Dot product of vectors is mentioned: [Pg.12]    [Pg.323]    [Pg.251]    [Pg.95]    [Pg.96]    [Pg.270]    [Pg.132]    [Pg.225]    [Pg.12]    [Pg.323]    [Pg.251]    [Pg.95]    [Pg.96]    [Pg.270]    [Pg.132]    [Pg.225]    [Pg.277]    [Pg.264]    [Pg.5]    [Pg.21]    [Pg.106]    [Pg.382]    [Pg.5]    [Pg.181]    [Pg.26]    [Pg.31]    [Pg.38]    [Pg.62]   
See also in sourсe #XX -- [ Pg.85 ]




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