2023 A/L Physics Past Paper · Question 18 (English Medium)

Heating time of a thicker and longer heater wire

An immersion heater made of a wire of length LL and diameter dd takes 44 minutes to raise the temperature of a given mass of water by 40 ∘C40\ ^\circ\text{C}. How much time is taken for heating a same amount of water by 40 ∘C40\ ^\circ\text{C} using another immersion heater made of a wire with the same material, but having length 2L2L and diameter 2d2d? (Neglect heat loss to the surroundings)

  1. (1) 0.5 min0.5\ \text{min}
  2. (2) 1 min1\ \text{min}
  3. (3) 1.5 min1.5\ \text{min}
  4. (4) 2 min2\ \text{min}
  5. (5) 8 min8\ \text{min}
Answer and explanation

Answer: (4) 2 min2\ \text{min}

What the question asks

What we know:

The first heater has a wire of length LL and diameter dd. It takes 4 min4\ \text{min} to warm the water by 40 ∘C40\ ^\circ\text{C}.

The second heater has a wire of the same material, with length 2L2L and diameter 2d2d. It warms the same amount of water by the same 40 ∘C40\ ^\circ\text{C}.

No heat is lost to the surroundings.

The question does not give the supply voltage. We take it as the same for both heaters, as if both were plugged into one socket.

We want: the time t2t_2 the second heater takes.

What each letter means:

LL (m\text{m}): the length of the first wire.

dd (m\text{m}): the diameter of the first wire.

AA (m2\text{m}^2): the area of the cross section of a wire.

ρ\rho (Ω m\Omega\ \text{m}): the resistivity of the material.

RR (Ω\Omega): the resistance of a wire.

VV (V\text{V}): the potential difference across the heater.

WW (J\text{J}): the heat energy that the water needs.

tt (min\text{min}): the time the heater takes.

Relevant theory

(1) When the length of a conductor increases its resistance increases. (2) When the area of cross-section of a conductor increases its resistance decreases.

The constant p represents the contribution from the material of the conductor to its resistance and is known as the "resistivity" of the material.

Heat is mainly liberated when a current passes through a resistor and this is known as "joule heating".

Passive resistors are those resistors in which the electrical energy flowing through them gets completely converted into heat.

The first two quotes tell us how the resistance of a wire depends on its length, its area and its material. The last two quotes say that the electrical energy that flows through a heater wire is completely changed into heat.

So the heat the water gets is the electrical energy W=VItW = VIt that the wire uses.

We also know the resistance of the wire, V=IRV = IR. Put I=VRI = \dfrac{V}{R} in W=VItW = VIt, and we get W=V2tRW = \dfrac{V^2t}{R}.

The same water must get the same heat, and VV is the same. So the time tt goes with the resistance RR.

Required equations

R=ρlAR = \rho\dfrac{l}{A}

A=πd24A = \dfrac{\pi d^2}{4}

W=VItW = VIt

I=VRI = \dfrac{V}{R}

W=V2tRW = \dfrac{V^2 t}{R}

Reasoning and calculation

What stays the same: the material, so ρ\rho is the same. The water and the 40 ∘C40\ ^\circ\text{C} rise are the same, so the heat WW is the same. The voltage VV is the same.

What changes: the length and the diameter of the wire. So RR changes, and with it the time tt.

For example, think of two taps filling the same bucket from one water supply.

A long, narrow pipe lets the water through slowly, so the bucket takes a long time. A short, wide pipe lets a lot through, so the bucket fills fast.

A heater wire is like the pipe. A wire that is harder to push the current through lets less current flow, so it needs more time to give the same heat.

Write the time for each heater, then divide.

t1=WR1V2t2=WR2V2t_1 = \dfrac{WR_1}{V^2} \qquad t_2 = \dfrac{WR_2}{V^2}

t2t1=R2R1\dfrac{t_2}{t_1} = \dfrac{R_2}{R_1}

The WW and the VV cancel.

The resistance of each wire is R=ρlAR = \rho\dfrac{l}{A} with A=πd24A = \dfrac{\pi d^2}{4}. The ρ\rho and the π\pi cancel too, so

R2R1=l2l1×(d1d2)2\dfrac{R_2}{R_1} = \dfrac{l_2}{l_1} \times \left(\dfrac{d_1}{d_2}\right)^2

The second wire is twice as long, and twice as wide.

l2l1=2d1d2=12\dfrac{l_2}{l_1} = 2 \qquad \dfrac{d_1}{d_2} = \dfrac{1}{2}

Put them in:

R2R1=2×(12)2=2×14=12\dfrac{R_2}{R_1} = 2 \times \left(\dfrac{1}{2}\right)^2 = 2 \times \dfrac{1}{4} = \dfrac{1}{2}

So the second time is half of the first:

t2=12×4 min=2 mint_2 = \dfrac{1}{2} \times 4\ \text{min} = 2\ \text{min}

Reading the options

The second heater takes 2 min2\ \text{min}. That is option (4).

Option (2) is what the wider wire gives without the longer length, and option (5) is what the longer wire gives without the wider wire.

Checks

Dimension check:

t2t1\dfrac{t_2}{t_1} is a time divided by a time, and R2R1\dfrac{R_2}{R_1} is a resistance divided by a resistance. Both are plain numbers, so they can be put equal.

t1∗l/(d∗d)t1 * l / (d * d)

Does it make sense?

The second wire is half the resistance, so at the same voltage twice as much current flows. The heater gives heat twice as fast.

The same heat at twice the rate takes half the time. That is 2 min2\ \text{min}.

Conclusion

t2=2 mint_2 = 2\ \text{min}

t2t1=R2R1=2×14=12\dfrac{t_2}{t_1} = \dfrac{R_2}{R_1} = 2 \times \dfrac{1}{4} = \dfrac{1}{2}, so t2=2 mint_2 = 2\ \text{min}.

The answer is (4).

For the same heat and the same voltage, the time goes with the resistance. So find R2R1\dfrac{R_2}{R_1}.

Length goes on top, and the diameter goes underneath as a square: R2R1=l2l1(d1d2)2\dfrac{R_2}{R_1} = \dfrac{l_2}{l_1}\left(\dfrac{d_1}{d_2}\right)^2.

Exam tip

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