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Question 6 The diagram below shows two small identical spheres, \( P \) and \( Q \), on insulated stands. The charge on sphere \( P \) is \( -3 \times 10^{-6} \mathrm{C} \) and the charge on sphere \( Q \) is unknown. \( -3 \times 10^{-6} \mathrm{C} \) 6.1.1. State the principle of charge quantization 6.1.2. Calculate the number of electrons in excess on sphere \( P \). The two spheres are brought into contact and are then returned to their original positions. Each sphere now carries a charge of \( -1 \times 10^{-6} \mathrm{C} \). 6.2. Calculate the original charge on sphere \( Q \) before the spheres were brought into contact. 6.3. Were electrons transferred from \( P \) to \( Q \) or from \( Q \) to \( P \) during contact? (1) [9]

Ask by Lewis Ryan. in South Africa
Feb 25,2025

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6.1.1. Charge quantization means that any charge is an integer multiple of the elementary charge. 6.1.2. Sphere P has about 1.9 × 10¹³ excess electrons. 6.2. Sphere Q originally had a charge of +1 × 10⁻⁶ C. 6.3. Electrons were transferred from sphere P to sphere Q during contact.

Solución

Below is a worked solution for each part: ────────────────────────────── 6.1.1. Principle of Charge Quantization The principle of charge quantization states that any charge must be an integer multiple of the elementary charge (e). In other words, the net charge Q on any object can only have values of Q = n · e, where n is an integer and e = 1.6 × 10⁻¹⁹ C. ────────────────────────────── 6.1.2. Number of Excess Electrons on Sphere P Sphere P has a charge of –3 × 10⁻⁶ C. Since each electron carries a charge of –1.6 × 10⁻¹⁹ C, the number of excess electrons (n) is given by   n = (Magnitude of total charge)/(Magnitude of one electron’s charge)     = (3 × 10⁻⁶ C)/(1.6 × 10⁻¹⁹ C)     ≈ 1.875 × 10¹³ Thus, there are approximately 1.9 × 10¹³ excess electrons on sphere P. ────────────────────────────── 6.2. Original Charge on Sphere Q When the spheres are brought into contact, charge redistributes equally between the two identical spheres. After separation, each sphere carries –1 × 10⁻⁶ C, so the total combined charge is   Total charge = (–1 × 10⁻⁶ C) + (–1 × 10⁻⁶ C) = –2 × 10⁻⁶ C. Before contact, the total charge was the sum of the charges on P and Q. Since sphere P was initially –3 × 10⁻⁶ C, let the original charge on Q be Q₀. Thus,   (–3 × 10⁻⁶ C) + Q₀ = –2 × 10⁻⁶ C Solve for Q₀:   Q₀ = (–2 × 10⁻⁶ C) – (–3 × 10⁻⁶ C)     = +1 × 10⁻⁶ C. So, sphere Q originally had a charge of +1 × 10⁻⁶ C. ────────────────────────────── 6.3. Direction of Electron Transfer Electrons are negatively charged. Initially, sphere P had a more negative charge (–3 × 10⁻⁶ C) and sphere Q had a positive charge (+1 × 10⁻⁶ C). When they were brought into contact, the charges equalized to –1 × 10⁻⁶ C on each sphere. Notice that: • Sphere P went from –3 × 10⁻⁶ C to –1 × 10⁻⁶ C, meaning it lost some negative charge (or lost electrons). • Sphere Q went from +1 × 10⁻⁶ C to –1 × 10⁻⁶ C, meaning it gained negative charge (gained electrons). Therefore, electrons were transferred from sphere P to sphere Q. ────────────────────────────── Summary of Answers: 6.1.1. Charge quantization means that the charge on any object is an integer multiple of the elementary charge (e = 1.6 × 10⁻¹⁹ C). 6.1.2. The number of excess electrons on sphere P is approximately 1.9 × 10¹³. 6.2. The original charge on sphere Q was +1 × 10⁻⁶ C. 6.3. Electrons were transferred from sphere P to sphere Q during contact.

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Bonus Knowledge

Every electric charge is quantized, meaning that it exists in discrete packets — specifically, it is a whole-number multiple of the elementary charge, which is approximately \( 1.6 \times 10^{-19} \mathrm{C} \). In simpler terms, charges cannot take on arbitrary values; they can only be integral multiples of the charge of an electron or proton. This principle explains why we observe certain charge values, as they must align with these fundamental quantities! To find the number of excess electrons on sphere \( P \) with a charge of \( -3 \times 10^{-6} \mathrm{C} \), you divide the total charge by the charge of a single electron. This calculation looks like this: \( -3 \times 10^{-6} \mathrm{C} \div -1.6 \times 10^{-19} \mathrm{C/electron} \approx 1.875 \times 10^{13} \) electrons. So, there are approximately \( 1.88 \times 10^{13} \) excess electrons on sphere \( P \)! After contact, charges redistribute equally, leading both spheres to carry \( -1 \times 10^{-6} \mathrm{C} \). Let \( Q \)'s original charge be \( q_Q \). Thus, \( -3 \times 10^{-6} + q_Q = -2 \times 10^{-6} \) which gives \( q_Q = 1 \times 10^{-6} \mathrm{C} \). When the spheres made contact, electrons flowed from \( Q \) to \( P \) since \( Q \) started at a positive charge, which indicates it had a deficiency of electrons compared to \( P \). So, electrons moved from the positively charged sphere \( Q \) to the negatively charged sphere \( P \) during contact!

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