Why voltage in a circuit is in a sinusoid form?

AI Thread Summary
Voltage in a circuit is often expressed in sinusoidal form due to its relationship with Fourier analysis, which allows for the decomposition of complex waveforms into simpler sinusoidal components. While the general form of a sinusoidal voltage can include a phase shift, it is common to simplify this by assigning one voltage a phase of zero for ease of analysis. The phase of a voltage is always relative to another voltage or current in the circuit, particularly in relation to impedance. Sinusoids are favored in circuit analysis because they facilitate linear operations and the superposition principle, enabling the combination of multiple voltage sources. Understanding why voltage is represented this way is crucial for effective circuit analysis and design.
jeff1evesque
Messages
312
Reaction score
0

Homework Statement


Could someone explain to me why voltage in a circuit is in a sinusoid form?

Homework Equations


(voltage)(sinusoid) \Rightarrow V_Scos(\omega t)

The Attempt at a Solution


Shouldn't all sinusoidal voltages in a circuit be in the form V_Scos(\omega t + \theta), or is V_Scos(\omega t) correct? I mean it's trivial, but the former notation is better because we can assign \theta = 0 which is the same as the latter.

thanks,

JL
 
Physics news on Phys.org


It isn't always in that form. You'll sometimes see voltage written in phasor form, which includes the phase. But what typically matters is the phase relative to other voltages in a circuit so for simplicity you can arbitrarily assign one of the voltages to have zero phase shift.

At least, that's my take on it; I'm not an EE.
 


When you start observing a variable voltage which changes just like a sine function, if the voltage is zero at t=0, then we say that the phase of the voltage is zero. If the voltage is not zero, then we say there is a phase θ. That is the difference between the two expressions.
 


JaWiB said:
It isn't always in that form. You'll sometimes see voltage written in phasor form, which includes the phase. But what typically matters is the phase relative to other voltages in a circuit so for simplicity you can arbitrarily assign one of the voltages to have zero phase shift.

At least, that's my take on it; I'm not an EE.

Ok got it. So when a voltage is in that form, it's in phasor notation- which is known to have it's parameters constant. Now I just have to search the web to find out why a voltage is multiplied with a sinusoid.

Thanks,

Jeff
 


I would comment that any single voltage or current does not "have a phase". Phases are always relative to something. Probably the most commonly encountered phase in circuit analysis is the impedance phase, which is the phase of the voltage across some element relative to the current through that element, at a given frequency (sinusoidal voltage and current).

If you are wondering why sinusoid, as opposed to any other arbitrary functional form:

Sinusoids are used because they are the basis for Fourier (frequency) analysis. The lowest order approximation for a circuit is to assume that it is "linear", or at least has linear modes of operation. This means that, for example, you can connect two different voltage sources, and then add the results as if you had connected each one individually. There's some kind of mathematical theorem or something that claims that you can construct (pretty much) arbitrary functions by adding up sinusoids in the appropriate way. (See Fourier Series/Transform.)
 
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
Back
Top