Why do the headlights on the car become dim when the car is starting?

AI Thread Summary
The dimming of headlights when starting a car is primarily due to the high current demand from the starter motor, which presents low resistance and pulls a significant amount of current from the battery. This increased load causes the battery's terminal voltage to drop temporarily, resulting in reduced brightness for the headlights. The internal resistance of the battery also plays a crucial role; as the current increases, the voltage at the terminals decreases due to this resistance. Additionally, some vehicles turn off the headlights during starting to allocate more energy to the starter motor. Understanding these concepts helps clarify why headlights dim during engine startup.
zenterix
Messages
774
Reaction score
84
Homework Statement
From the perspective of electric circuits and electromagnetism, why do the headlights on the car become dim when the car is starting?
Relevant Equations
I'm not sure how a car engine works electrically.

So I would like to think about this problem in a simpler context.
Suppose we have 12V battery.

Though I can solve electric circuits, there are some very simple practical concepts that are gaping holes in my knowledge.

What does it mean for a circuit device to "pull a lot of current"?

What is a simple circuit element that when I connect it to the battery it will "pull" a lot of current?

If I connect a resistor to the terminals of the battery, then current flows according to Ohm's law. Thus, current depends on the voltage of the battery and resistance of the resistor.

The smaller the resistance, the larger the current.

If the resistance is extremely small, a huge amount of current can flow.

Suppose the resistor is the filament of a light bulb. It lights up.

Suppose the light bulb is connected in parallel to nine other light bulbs, but there is an open switch in the wire that leads to the nine other light bulbs.

The moment we close the switch, the equivalent resistance becomes ##R/10## and ten times more current flows, but the current to the first light bulb is still the same.

I imagine that the charge on the positive terminal of the battery is depleted rapidly. I imagine it takes time for the chemical reactions to re-establish the difference in potential.

Thus, the potential difference created by the battery decreases.

If ##i_1## is the current through the first light bulb, then initially ##i_1=\frac{\epsilon_0}{R}##. After the switch is closed, if the emf were to stay the same then the total current in the circuit would be ##i=\frac{\epsilon_0}{R_{eq}}=\frac{\epsilon_0}{R/10}=10i_1## and ##i_1=\frac{\epsilon_0}{R}## is the same as before.

But if ##\epsilon_0## decreases, then the total current is somewhat smaller than ##10i_1## and the current to the first light bulb is smaller than ##i_1##. Thus, it's brightness decreases.

Is this roughly why the lights in a car dim when we turn the car on? In other words, it is essentially because the battery electromotive force decreases temporarily because of the presence of extra small resistances in parallel with the headlights?
 
Physics news on Phys.org
zenterix said:
Is this roughly why the lights in a car dim when we turn the car on? In other words, it is essentially because the battery electromotive force decreases temporarily because of the presence of extra small resistances in parallel with the headlights?
Yes.

Starter motors take a large amount of current, but only very briefly, so the lights dim very briefly.
 
zenterix said:
So I would like to think about this problem in a simpler context.

Suppose we have 12V battery.

Though I can solve electric circuits, there are some very simple practical concepts that are gaping holes in my knowledge.

What does it mean for a circuit device to "pull a lot of current"?
An electric motor (the starter motor ), under a heavy mechanical load (turning the gas engine) , presents a very low resistance to the battery, thus "demanding" a lot of current to satisfy ohm's law.
Real batteries can be modeled as a Thevenin equivalent source: an "ideal" voltage source in series with a resistor. For a 12V car battery this "internal resistance" will be Rint≈0.1 Ω So ordinary circuit theory tells us that when the starter motor needs 30 A, the terminal voltage on the battery will be $$V_{terminal}=12V-30A(0.1 \Omega) =9V$$ which is what my car tells me every morning when I crank it.
An undercharged or damaged battery will exhibit a higher internal resistancen and fail to meet the voltage requirement under heavy load. Did I mention temperature? You get the picture I think.
 
Last edited:
Just to add to the above good replies...

You can learn more about the internal resistance of lead-acid car batteries here:

https://www.google.com/url?sa=t&rct...usg=AOvVaw1G_V2UaR1GsCtSrrNJxr5P&opi=89978449

But this is also a bit of a trick question as stated in your schoolwork problem. Some cars and most motorcycles actually turn off the headlights while the starter motor is cranking. This is done to provide more energy to the starter motor during the short time that you are starting the car or motorcycle. :wink:
 
  • Like
Likes Lnewqban and hutchphd
Sometimes I think a battery should be modeled by a Norton Equivalent (for the physics I mean......obviously equivalent means what it says for circuit purposes.)
 
I multiplied the values first without the error limit. Got 19.38. rounded it off to 2 significant figures since the given data has 2 significant figures. So = 19. For error I used the above formula. It comes out about 1.48. Now my question is. Should I write the answer as 19±1.5 (rounding 1.48 to 2 significant figures) OR should I write it as 19±1. So in short, should the error have same number of significant figures as the mean value or should it have the same number of decimal places as...
Thread 'Calculation of Tensile Forces in Piston-Type Water-Lifting Devices at Elevated Locations'
Figure 1 Overall Structure Diagram Figure 2: Top view of the piston when it is cylindrical A circular opening is created at a height of 5 meters above the water surface. Inside this opening is a sleeve-type piston with a cross-sectional area of 1 square meter. The piston is pulled to the right at a constant speed. The pulling force is(Figure 2): F = ρshg = 1000 × 1 × 5 × 10 = 50,000 N. Figure 3: Modifying the structure to incorporate a fixed internal piston When I modify the piston...
Thread 'A cylinder connected to a hanging mass'
Let's declare that for the cylinder, mass = M = 10 kg Radius = R = 4 m For the wall and the floor, Friction coeff = ##\mu## = 0.5 For the hanging mass, mass = m = 11 kg First, we divide the force according to their respective plane (x and y thing, correct me if I'm wrong) and according to which, cylinder or the hanging mass, they're working on. Force on the hanging mass $$mg - T = ma$$ Force(Cylinder) on y $$N_f + f_w - Mg = 0$$ Force(Cylinder) on x $$T + f_f - N_w = Ma$$ There's also...
Back
Top