Confused how to use calculus in physics

Click For Summary
SUMMARY

The discussion clarifies the application of calculus in physics, specifically in calculating electric fields from uniform charge distributions. The integral E_x=∫dEcosθ represents the summation of differential electric field contributions, where dE is a vector and cosθ projects it onto the x-axis. The integral signifies the need to express variables in terms of each other, facilitating the addition of contributions from an infinite number of charge points through superposition. Understanding this concept is crucial for effectively applying calculus in physics problems involving continuous charge distributions.

PREREQUISITES
  • Understanding of basic calculus concepts, including integration and differentiation.
  • Familiarity with electric field concepts and vector projections.
  • Knowledge of superposition principle in physics.
  • Ability to interpret geometric relationships in physics problems.
NEXT STEPS
  • Study the concept of vector fields in electromagnetism.
  • Learn about the application of line integrals in calculating electric fields.
  • Explore the principles of superposition in continuous charge distributions.
  • Investigate the geometric interpretation of integrals in physics contexts.
USEFUL FOR

Students and professionals in physics, particularly those focusing on electromagnetism, as well as educators seeking to clarify the integration of calculus in physical applications.

jaydnul
Messages
558
Reaction score
15
I understand simple concepts, like \frac{dx}{dt}=v and why that is, but when I'm doing, for example, uniform charge distributions, I don't understand what the integral is actually doing. For example:

E_x=∫dEcosθ

From what I learned in calculus, the dE means with respect to. So when taking an integral you usually have the form ∫y(x)dx and the interval is [a,b], which are x values.

Why isn't the integral above in that form then? I mean at the very least, ∫dθcosθ would make more sense to me.
 
Physics news on Phys.org
Why isn't it in that form? Because you haven't made it into that form yet, that is your goal. You need to express E in terms of theta, or theta in terms of E, by looking at the geometry of the situation.

Every little point in a charge distribution contributes to the overall electric field. If you just had 2 point charges you would add the fields in accordance with superposition. But now that you have an infinite number of points in a larger distribution, you need to do an integral to add them all up.
 
Jd0g33,

∫ means a "sum" over differential amounts.

In ∫dE cosθ the differential amount is dE cosθ

dE is a vector and dE x cosθ is its projection on the x-axis.

Adding up all the projections of every dE, you get E_{x}.

When taking ∫y(x)dx, the differential amount being added up is y(x)dx, that is, y(x) times dx.
This is the "area" under the point y(x).

In this explanation, I have used some loose terms, but I hope I could pass the message.
 

Similar threads

  • · Replies 9 ·
Replies
9
Views
3K
  • · Replies 22 ·
Replies
22
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 33 ·
2
Replies
33
Views
4K
  • · Replies 17 ·
Replies
17
Views
10K
Replies
2
Views
2K
  • · Replies 26 ·
Replies
26
Views
6K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 16 ·
Replies
16
Views
3K