A proton travels in the x direction and enters a region where a constant uniform electric field is directed in the y direction. Derive an equation which describes the x and y cooedinates of the proton in the field as a function of time t.

The x component of velocity will remain unchanged.

The y component of velocity will start at zero and then accelerate at a rate eE/m in the -y direction. E is the electric field. e and m are the electron charege and mass.

The x and y coordinates are the integrals of the corresponding V coordinates.

You should be able to take it from there.

To derive the equation that describes the x and y coordinates of the proton in the electric field as a function of time, we need to consider the forces acting on the proton.

The proton experiences two types of forces: the electric force due to the electric field and the inertial force due to its mass and acceleration.

The electric force experienced by a charged particle in an electric field is given by the equation F = qE, where F is the force, q is the charge of the particle, and E is the electric field.

In this case, since the electric field is directed in the y direction and the proton travels in the x direction, only the y component of the electric force will have an effect on the proton's motion. Therefore, the equation for the y component of the electric force is Fy = qEy.

The inertial force experienced by an object due to its mass and acceleration is given by the equation F = ma, where F is the force, m is the mass of the object, and a is the acceleration.

The acceleration of the proton can be determined using Newton's second law, which states that the net force acting on an object is equal to the mass of the object multiplied by its acceleration. In this case, the net force is the y component of the electric force, so we have ma = qEy.

Next, we need to solve this equation for acceleration. Since acceleration is the second derivative of position with respect to time, we can rewrite the equation as a = (d^2y/dt^2) = (qEy/m).

To solve this second-order differential equation, we need to assume an initial condition for the proton's position and velocity. Let's assume that at t = 0, the proton's initial position is x = x0 and y = y0, and its initial velocity is vx0 in the x direction and vy0 in the y direction.

To solve for the x and y coordinates as functions of time, we need to integrate the equations of motion.

For the x direction, the proton experiences no force, so its velocity remains constant, resulting in the equation: x = x0 + vx0t.

For the y direction, we need to integrate twice to obtain the equation: y = y0 + vy0t + (qEy/m)t^2/2.

So, the derived equation that describes the x and y coordinates of the proton in the electric field as a function of time t are: x = x0 + vx0t and y = y0 + vy0t + (qEy/m)t^2/2.