Math Problem Statement

When a direct voltage is connected to a circuit, the current does not start flowing smoothly immediately, but follows the equation L*(dI/dt)+RI=V where L is the inductance of the circuit, R is the resistance, I is the current and V is the voltage. Voltage is switched at time t = 0, so that I(0) = 0. Determine I(t) and its limit value limt→∞ I(t). When has the current in the circuit reached 50% of this limit value?

Solution

To solve the equation given by

LdIdt+RI=V,L \frac{dI}{dt} + RI = V,

we'll follow these steps:

  1. Rewrite the equation: This is a first-order linear ordinary differential equation (ODE). Rearranging it gives:

dIdt+RLI=VL.\frac{dI}{dt} + \frac{R}{L}I = \frac{V}{L}.

  1. Identify the integrating factor: The integrating factor, μ(t)\mu(t), is given by:

μ(t)=eRLdt=eRLt.\mu(t) = e^{\int \frac{R}{L} dt} = e^{\frac{R}{L}t}.

  1. Multiply the ODE by the integrating factor:

eRLtdIdt+RLeRLtI=VLeRLt.e^{\frac{R}{L}t} \frac{dI}{dt} + \frac{R}{L} e^{\frac{R}{L}t} I = \frac{V}{L} e^{\frac{R}{L}t}.

  1. Rewrite the left-hand side:

ddt(eRLtI)=VLeRLt.\frac{d}{dt} \left( e^{\frac{R}{L}t} I \right) = \frac{V}{L} e^{\frac{R}{L}t}.

  1. Integrate both sides:

eRLtI=VLeRLtdt=VReRLt+C,e^{\frac{R}{L}t} I = \int \frac{V}{L} e^{\frac{R}{L}t} dt = \frac{V}{R} e^{\frac{R}{L}t} + C,

where CC is a constant of integration.

  1. Solve for I(t)I(t):

I(t)=VR+CeRLt.I(t) = \frac{V}{R} + Ce^{-\frac{R}{L}t}.

  1. Apply the initial condition I(0)=0I(0) = 0:

At t=0t = 0:

0=VR+C    C=VR.0 = \frac{V}{R} + C \implies C = -\frac{V}{R}.

Thus, the expression for I(t)I(t) becomes:

I(t)=VRVReRLt=VR(1eRLt).I(t) = \frac{V}{R} - \frac{V}{R} e^{-\frac{R}{L}t} = \frac{V}{R} \left( 1 - e^{-\frac{R}{L}t} \right).

Limit of I(t)I(t)

To find the limit as tt approaches infinity:

limtI(t)=VR(10)=VR.\lim_{t \to \infty} I(t) = \frac{V}{R} \left( 1 - 0 \right) = \frac{V}{R}.

Time to reach 50% of the limit value

To find when I(t)I(t) reaches 50% of its limit value VR\frac{V}{R}:

0.5VR=VR(1eRLt).0.5 \cdot \frac{V}{R} = \frac{V}{R} \left( 1 - e^{-\frac{R}{L}t} \right).

Dividing both sides by VR\frac{V}{R} (assuming V0V \neq 0) gives:

0.5=1eRLt.0.5 = 1 - e^{-\frac{R}{L}t}.

Solving for eRLte^{-\frac{R}{L}t}:

eRLt=0.5    RLt=ln(0.5)    t=LRln(0.5).e^{-\frac{R}{L}t} = 0.5 \implies -\frac{R}{L}t = \ln(0.5) \implies t = -\frac{L}{R} \ln(0.5).

This simplifies to:

t=LRln(2).t = \frac{L}{R} \ln(2).

Summary

  • The current I(t)I(t) is given by:

I(t)=VR(1eRLt).I(t) = \frac{V}{R} \left( 1 - e^{-\frac{R}{L}t} \right).

  • The limit value is VR\frac{V}{R}.
  • The time to reach 50% of this limit is t=LRln(2)t = \frac{L}{R} \ln(2).

Do you want more details or have any questions? Here are some related questions you might consider:

  1. What physical principles are illustrated by the behavior of current in this circuit?
  2. How does changing the resistance RR affect the time to reach 50% of the limit value?
  3. What happens to the current if the voltage VV is increased?
  4. How does the inductance LL influence the transient response of the circuit?
  5. Can you explain the concept of time constant in the context of this circuit?

Tip: Understanding how inductors and resistors interact in circuits can provide insights into more complex electrical systems.

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Math Problem Analysis

Mathematical Concepts

Differential Equations
Circuit Analysis

Formulas

L * (dI/dt) + RI = V
I(t) = (V/R) * (1 - e^(-R/L * t))
lim(t→∞) I(t) = V/R
t = (L/R) * ln(2)

Theorems

First-order Linear Differential Equation

Suitable Grade Level

Grades 11-12