- #1
DottZakapa
- 239
- 17
in particular:
the following, i don't get why do i need such partial derivative
following, i don't understand why that minus in front of the partial derivative
Is there anyone so kindly patient to help?
thanks
i agree with that so as you say it isDelta2 said:Yes that is the decomposition of the two vectors. What's the problem with it?
We don't have to know if they point left or right or up or down. The reason that they become negative when we take the dot product ##\vec{B}\cdot d\vec{l}## is that the vector ##d\vec{l}## (which always points counterclockwise) becomes negative with respect to the positive unit vector ##u_x## or ##u_y##. So for example at the segment PQ it is ##d\vec{l}=dx\vec{u_x}## while at the segment RS it is ##d\vec{l}=-dx\vec{u_x}##
Ampere's law in differential form is a mathematical equation that describes the relationship between an electric current and the magnetic field it produces. It is a fundamental law in electromagnetism and is used to calculate the magnetic field at a given point in space.
The main difference between Ampere's law in integral form and differential form is the way the equation is expressed. In integral form, the equation is written as a line integral around a closed loop, while in differential form, it is expressed as a partial derivative of the magnetic field with respect to position.
Ampere's law in differential form is derived from the integral form using the Stokes' theorem. This theorem relates a line integral around a closed loop to a surface integral over the area enclosed by the loop. By applying this theorem to Ampere's law in integral form, we can derive the differential form.
Ampere's law in differential form is only valid for steady-state situations where the magnetic field does not change over time. It also assumes that the current is confined to a region where the magnetic field is being calculated. If these conditions are not met, the law may not accurately predict the magnetic field.
Ampere's law in differential form is used in various practical applications, such as designing and analyzing electric motors and generators, calculating the magnetic field of a solenoid, and understanding the behavior of electromagnetic waves. It is also used in the development of magnetic resonance imaging (MRI) technology in medicine.