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Shkiper50 [21]
2 years ago
9

I NEED AT LEAST A LIST OF 10 SONGS OF BEETHOVEN'S​

Physics
2 answers:
kompoz [17]2 years ago
6 0
Some of Beethoven’s most influential songs include:
1. Piano Concerto No. 2 in B flat major
2. Piano Sonata No. 14 Moonlight
3. Symphony No. 3 in E flat
4. Symphony No. 9 in C minor
5. Violin Concerto in D
6. Symphony No. 6 in F
7. Bagatelle in A minor, ‘Fur Elise’
8. Piano Sonata No. 29, ‘Hammerklavier’
9. Symphony No. 9, ‘Choral’
10. String Quartet in B flat Op. 130
DanielleElmas [232]2 years ago
3 0

Answer:

<u>Here are some of the songs of Beethoven's</u>:–

  • Septet.
  • Moonlight Sonata.
  • Pathetique Sonata.
  • Adelaide (Most popular).
  • Eroica Symphony.
  • Fifth Symphony.
  • Fidelio.
  • Emperor piano concerto.

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A car speeds up from 18.54 m/s to<br> 29.52 m/s in 13.84 s.<br> The acceleration of the car is:
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A uniformly charged, one-dimensional rod of length L has total positive charge Q. Itsleft end is located at x = ????L and its ri
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Answer:

|\vec{F}| = \frac{1}{4\pi\epsilon_0}\frac{qQ}{L}(\ln(L+x_0)-\ln(x_0))

Explanation:

The force on the point charge q exerted by the rod can be found by Coulomb's Law.

\vec{F} = \frac{1}{4\pi\epsilon_0}\frac{q_1q_2}{r^2}\^r

Unfortunately, Coulomb's Law is valid for points charges only, and the rod is not a point charge.

In this case, we have to choose an infinitesimal portion on the rod, which is basically a point, and calculate the force exerted by this point, then integrate this small force (dF) over the entire rod.

We will choose an infinitesimal portion from a distance 'x' from the origin, and the length of this portion will be denoted as 'dx'. The charge of this small portion will be 'dq'.

Applying Coulomb's Law:

d\vec{F} = \frac{1}{4\pi\epsilon_0}\frac{qdq}{x + x_0}(\^x)

The direction of the force on 'q' is to the right, since both charges are positive, and they repel each other.

Now, we have to write 'dq' in term of the known quantities.

\frac{Q}{L} = \frac{dq}{dx}\\dq = \frac{Qdx}{L}

Now, substitute this into 'dF':

d\vec{F} = \frac{1}{4\pi\epsilon_0}\frac{qQdx}{L(x+x_0)}(\^x)

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3 years ago
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