Examples of sinusoidal in the following topics:

 The sinusoids are capillaries that develop after implantation to allow the exchange of gas and nutrients with the mother.
 A sinusoid is a small blood vessel that is a type of capillary similar to a fenestrated endothelium.
 Sinusoids are actually classified as a type of open pore capillary (that is, discontinuous) as opposed to fenestrated.
 Sinusoids are found in the liver, lymphoid tissue, endocrine organs, and hematopoietic organs, such as the bone marrow and the spleen.
 Sinusoids found within terminal villi of the placenta are not comparable to these because they possess a continuous endothelium and complete basal lamina.

 The solutions to the equations of motion of simple harmonic oscillators are always sinusoidal, i.e., sines and cosines.
 These are all sinusoidal solutions .
 Uniform circular motion is therefore also sinusoidal, as you can see from .
 Only the top graph is sinusoidal.
 Review factors responsible for the sinusoidal behavior of uniform circular motion

 The sinusoidal function $A cos( \omega t + \phi)$ can be written as a phasor: $Ae^{j \theta}$ .
 This can be particularly useful because the frequency factor (which includes the timedependence of the sinusoid) is often common to all the components of a linear combination of sinusoids.
 Sinusoids can be represented mathematically as the sum of two complexvalued functions:
 Sinusoidal Steady State and the Series RLC CircuitPhasors may be used to analyze the behavior of electrical and mechanical systems that have reached a kind of equilibrium called sinusoidal steady state.
 In the sinusoidal steady state, every voltage and current (or force and velocity) in a system is sinusoidal with angular frequency ω.

 For instance, when we studied the forced harmonic oscillator, we first solved the problem by assuming the forcing function was a sinusoid (or complex exponential).
 We then argued that since the equations were linear this was enough to let us build the solution for an arbitrary forcing function if only we could represent this forcing function as a sum of sinusoids.
 Later, when we derived the continuum limit of the coupled spring/mass system we saw that separation of variables led us to a solution, but only if we could somehow represent general initial conditions as a sum of sinusoids.

 Sinusoidal  Sinusoidal capillaries are a special type of fenestrated capillaries that have larger openings (3040 μm in diameter) in the endothelium.
 Sinusoid blood vessels are primarily located in the bone marrow, lymph nodes, and adrenal gland.
 Some sinusoids are special in that they do not have tight junctions between cells.
 These are called discontinuous sinusoidal capillaries, present in the liver and spleen where greater movement of cells and materials is necessary.

 Blood from either source passes into cavities between the hepatocytes of the liver called sinusoids, which feature a fenestrated, discontinuous endothelium allowing for the effecient transfer and processing of nutrients in the liver.
 Sinusoid of a rat liver with fenestrated endothelial cells.
 Fenestrae are approx 100nm diameter, and sinusoidal width 5 microns.

 This looks like the equation of a damped sinusoid.
 But the second term may or may not be a sinusoid, depending on whether the square root is positive.
 First if $\frac{\gamma}{2\omega_0} < 1$ , corresponding to small damping, then the argument of the square root is positive and indeed we have a damped sinusoid.

 The extrema (peaks and troughs) of a sinusoid of frequency $f_s$ will lie exactly $1/2f_s$ apart.
 Figure 4.9: A sinusoid sampled at less than the Nyquist frequency gives rise to spurious periodicities.

 ., sinusoids.The RMS value of a set of values (or a continuoustime function such as a sinusoid) is the square root of the arithmetic mean of the squares of the original values (or the square of the function).
 We can see from the above equations that we can express the average power as a function of the peak voltage and current (in the case of sinusoidally varying current and voltage):
 The RMS values are also useful if the voltage varies by some waveform other than sinusoids, such as with a square, triangular or sawtooth waves .
 The voltage and current are sinusoidal and are in phase for a simple resistance circuit.

 This equation can be solved exactly for any driving force, using the solutions z(t) which satisfy the unforced equation: $\frac{\mathrm{d}^2z}{\mathrm{d}t^2} + 2\zeta\omega_0\frac{\mathrm{d}z}{\mathrm{d}t} + \omega_0^2 z = 0$, and which can be expressed as damped sinusoidal oscillations $z(t) = A \mathrm{e}^{\zeta \omega_0 t} \ \sin \left( \sqrt{1\zeta^2} \ \omega_0 t + \varphi \right)$in the case where ζ ≤ 1.
 In the case of a sinusoidal driving force: $\frac{\mathrm{d}^2x}{\mathrm{d}t^2} + 2\zeta\omega_0\frac{\mathrm{d}x}{\mathrm{d}t} + \omega_0^2 x = \frac{1}{m} F_0 \sin(\omega t)$, where $\!
 \omega$ is the driving frequency for a sinusoidal driving mechanism.