Finding the amplitude of the sum vector

chilge
Messages
8
Reaction score
0

Homework Statement


A signal E(t) is made up of three terms, each having the same frequency but differing in phase:

E(t) = E0cos(ωt) + E0cos(ωt + δ) + E0cos(ωt + 2δ)

It is possible to find the amplitude of the sum vector by summing each vector described as a magnitude multiplied by a phase. The sum will therefore contain three terms. You can simplify this to express the sum as a real number times a phase. The real number is the amplitude of the sum vector. Make a plot of the amplitude of the sum vector as a function of δ as δ varies from 0 to 2∏.


Homework Equations



A signal can be represented as the real part of a complex number z,
z = Aei(wt+∅) = A[cos(wt+∅) + jsin(wt+∅)]


The Attempt at a Solution



E(t) = E0cos(ωt) + E0cos(ωt + δ) + E0cos(ωt + 2δ)
E(t) = E0exp(iωt) + E0exp(i(ωt + δ)) + E0exp(i(ωt + 2δ))
E(t) = E0exp(iωt) * (1 + exp(iδ) + exp(i2δ))
E(t) = E0cos(ωt) * (1 + exp(iδ) + exp(i2δ))

I can't think of a way to simplify it any further to put it in the form real number * a phase term. Am I missing something?
 
Physics news on Phys.org
First of all, this equation really makes no sense:
chilge said:
Aei(wt+∅) = A[cos(wt+∅) + jsin(wt+∅)]
because you are using two different notations for the imaginary unit in the same expression. If you use i to denote the imaginary unit, you should have:
Aei(wt+∅) = A[cos(wt+∅) + i sin(wt+∅)]

Second, between the first and second steps in your attempt at a solution, you incorrectly applied that formula. You have changed a real expression into an expression with a real part and a non-zero imaginary part.

If you do some simple algebra you should see that you can represent cos(x) as
cos(x) = (eix+e-ix)/2
Alternatively, you could write cos(x) as the real part of eix, e.g.
cos(x)+cos(y) = Re[eix + eiy]

Try applying those formulae and see if you can make any more progress. And feel free to post again if you get stuck. But you should make a better attempt before I give you any more hints.
 
Last edited:
chilge said:

Homework Statement


A signal E(t) is made up of three terms, each having the same frequency but differing in phase:

E(t) = E0cos(ωt) + E0cos(ωt + δ) + E0cos(ωt + 2δ)

It is possible to find the amplitude of the sum vector by summing each vector described as a magnitude multiplied by a phase. The sum will therefore contain three terms. You can simplify this to express the sum as a real number times a phase. The real number is the amplitude of the sum vector. Make a plot of the amplitude of the sum vector as a function of δ as δ varies from 0 to 2∏.


Homework Equations



A signal can be represented as the real part of a complex number z,
z = Aei(wt+∅) = A[cos(wt+∅) + jsin(wt+∅)]


The Attempt at a Solution



E(t) = E0cos(ωt) + E0cos(ωt + δ) + E0cos(ωt + 2δ)
E(t) = E0exp(iωt) + E0exp(i(ωt + δ)) + E0exp(i(ωt + 2δ))
E(t) = E0exp(iωt) * (1 + exp(iδ) + exp(i2δ))
[STRIKE]E(t) = E0cos(ωt) * (1 + exp(iδ) + exp(i2δ))[/STRIKE]

I can't think of a way to simplify it any further to put it in the form real number * a phase term. Am I missing something?

You can not use the same notation for the real E(t) and the complex one. Write E(t)=Re(Z) where Z=E0exp(iωt) + E0exp(i(ωt + δ)) + E0exp(i(ωt + 2δ)), and make it equal to Aexp(i(ωt+θ)), where A and θ ( both real) are to be determined.

You need to transform the factor 1 + exp(iδ) + exp(i2δ) into the exponential form, 1 + exp(iδ) + exp(i2δ)=Cexp(iψ). For that, expand the exponentials exp(iδ)=cosδ+isinδ. Note that exp(i2δ)=[exp(iδ)]2. Collect the real and imaginary parts of the sum, and find the amplitude and phase.

ehild
 
Last edited:
the solution is much easier if you factor out E0exp(iωt)exp(iδ):

\hat Z(t)=E_0 e^{i \omega t}+E_0 e^{i (\omega t+\delta)}+E_0 e^{i (\omega t+2\delta)}=E_0 e^{i (\omega t+\delta)} (e^{-i\delta}+1+e^{i\delta})

But e^{-i\delta}+1+e^{i\delta}=1+2\cos \delta, a real quantity. That makes

\hat Z(t)=E_0 (1+2\cos \delta)e^{i (\omega t+\delta)}

ehild
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top