complex quantity वाक्य
उदाहरण वाक्य
मोबाइल
- Generally, ZY is a complex quantity,
- Note that by the given definition, V _ \ parallel is a complex quantity.
- The basic idea is to use a real valued, it is convenient to define the complex quantities
- Where, \ varepsilon is a complex quantity and is a measure of departure from CP invariance.
- The action of the quaternionic matrices on quaternionic vectors is now represented by complex quantities, but otherwise it is the same as for " ordinary " matrices and vectors.
- In weak gravitational lensing, two different definitions are commonly used, and both are complex quantities which specify both the axis ratio and the position angle \ phi ~:
- The orders \ alpha _ k and \ beta _ k are in general complex quantities, but two interesting cases are when the orders are " commensurate"
- It is convenient that these two can be treated as the real and imaginary components of a complex quantity and use the Fourier theory to transform the measured time domain signal into the frequency domain representation.
- There is also an understood time dependence e ^ { i \ omega t } multiplying such phasor quantities; the actual field at a point in time and space is given by the real part of that complex quantity.
- Physical quantities may be expressed as complex numbers ( e . g . e ^ { i \ theta } ) which imply that the complex quantity has an orientation equal to that of the angle it is associated with ( in the above example ).
- A number is a degraded form of a complex quantity p + q ^ { \ sqrt {-1 } } and a complex quantity is a degraded form of a quaternion; consequently one meaning which may be assigned to m and n is that of quaternion.
- A number is a degraded form of a complex quantity p + q ^ { \ sqrt {-1 } } and a complex quantity is a degraded form of a quaternion; consequently one meaning which may be assigned to m and n is that of quaternion.
- Thus taking the real part of the complex quantity inside the parenthesis, the actual voltage consists of a sine wave at frequency ? with a peak amplitude equal to the complex magnitude of V, and with a phase given by the phase of the complex V . Then with the position along a transmission line given by x, with the line ending in a load located at x 0, the complex amplitudes of the forward and reverse waves would be written as:
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