A Level Physics 2020

AQA A Level Physics 2020

PHYSICS 7407/1 Paper 1

Section A
Answer all questions in this section.

01 One strong interaction that occurs when two high-energy protons collide is

[math]p + p → p + π^+ + π^− + X[/math]

01.1 Determine the lepton number, strangeness and charge of particle X.

[2 marks] 

Explanation:

[math]p + p → p + π^+ + π^− + X[/math]

Strangeness Number: All particles have a strangeness number of 0.
Lepton Number: All particles have a lepton number of 0

In the reaction [math]p + p → p + π^+ + π^- + X[/math], the total charge on both sides must be equal to satisfy charge conservation.
On the left-hand side, we have two protons (p), each carrying a charge of +1. So the total charge on the left-hand side is +2.
On the right-hand side, we have a proton (p) and a positively charged pion ([math]π^+[/math]), each carrying a charge of +1, and a negatively charged pion ([math]π^-[/math]) carrying a charge of -1.
Additionally, we have the X particle with a charge number of +1.

Conclusion:
Based on the charge conservation in the reaction, the X particle with a charge number of +1

Strangeness is one of the quantum numbers Strangeness plays a role in understanding the properties and behavior of particles with strange quarks, such as their decay modes and lifetimes. Strangeness is conserved in strong and electromagnetic interactions, meaning the total strangeness remains constant (zero)

Explanation:

  •  Strangeness Number: All particles have a strangeness number of 0.
  • Lepton Number: All particles have a lepton number of 0.
  • Charge Number: Protons and the positively charged pion have a charge number of

+1, the negatively charged pion has a charge number of -1, and (X) has a charge number
of +1.

lepton number =                0                 
strangeness =                0                 
charge =            + 1                  

01.2 Identify particle X. 

[1 mark]

Explanation:

[math]p + p → p + π^+ + π^− + X[/math]

Conclusion:

  • Based on the charge conservation in the reaction, the X particle with a charge number of +1 must be a proton.

01.3 A possible decay of a negative pion is

[math]π^− → e^− + Y [/math]

What is particle Y?
Tick ([math]\square[/math]) one box.

[1 mark]

[math]�e\qquad \square[/math]

[math]v_e \qquad \square[/math]

[math]π^0 \qquad \square[/math]

[math] {}^{0}_{1}\mathrm{n} \qquad \square[/math]

In the decay of a negative pion ([math]π^-[/math]) to an electron ([math]e^-[/math]) and Y, the particle Y is an antineutrino, specifically an electron antineutrino ([math]v \overline{e}[/math]).

[math] π^− → e^− + Y [/math]

L: 0 → +1 -1
Q: -1 → -1 + 0

Answer: (νe)

01.4 Some subatomic particles are classified as hadrons. There are two classes of hadrons. 

Discuss the nature of hadrons.
Your answer should include:

  • the identifying properties of hadrons
  • the structure of a hadron in each class
  • a discussion of the stability of free hadrons.

[6 marks]

Hadrons are a class of subatomic particles that play a fundamental role in the composition of atomic nuclei and are an important part of the standard model of particle physics. Hadrons are characterized by certain identifying properties, are divided into two main classes, and have distinctive structures. Additionally, their stability when free (not bound within atomic nuclei) is an important aspect of their behavior.

Identifying Properties of Hadrons:
Hadrons are strongly interacting particles, which means they participate in the strong nuclear force, one of the fundamental forces of nature.
Hadrons have fractional electric charges. This is in contrast to leptons (e.g., electrons and neutrinos), which have integral electric charges.
Hadrons experience the strong force and electromagnetic interactions.

Structure of Hadrons in Each Class:
Hadrons are divided into two classes based on their intrinsic properties:

A. Baryons:

Baryons are one class of hadrons, and they include protons and neutrons, which are the building blocks of atomic nuclei.
Baryons are made up of three quarks. These quarks are held together by the exchange of particles called gluons, which mediate the strong force. For example, a proton consists of two up quarks and one down quark, while a neutron consists of two down quarks and one up quark.

B. Mesons:

Mesons are the other class of hadrons, and they include particles like pions and kaons. Mesons are composed of a quark and an antiquark. They also interact via the strong force and are held together by the exchange of gluons. For instance, a pion can consist of an up quark and an anti-down quark or vice versa.

Stability of Free Hadrons:
Free hadrons, when not bound within atomic nuclei, are generally unstable. This means they have a finite lifetime and eventually decay into other particles.
The relatively short lifetime of free hadrons is due to the strong force, which mediates their interactions. The strong force is very powerful at short distances but weakens rapidly as particles move away from each other.
When free hadrons exist, they eventually undergo a process called hadron decay, where they transform into other particles, typically leptons (e.g., electrons, neutrinos) or other hadrons. This is a fundamental aspect of the behavior of hadrons, and it is a consequence of their strong interactions.

02 A spacecraft entering the atmosphere of Mars must decelerate to land undamaged on the surface.

Figure 1

02.1 Figure 1 shows the spacecraft of total mass 610 kg entering the atmosphere at a speed of [math]5.5 km s^{−1}[/math]. box

Calculate the kinetic energy of the spacecraft as it enters the atmosphere.
Give your answer to an appropriate number of significant figures.

[3 marks] 

Explanation:

To calculate the kinetic energy of the spacecraft, we can use the formula:
[math]\text{Kinetic Energy }= (1/2) \times \text{mass} \times \text{velocity}^2 [/math]
Given: Mass of the spacecraft (m) = 610 kg Velocity of the spacecraft (v) = 5.5
km/s
Converting the velocity from km/s to m/s: 5.5 km/s * 1000 m/km = 5500 m/s
Now we can substitute the values into the formula and calculate the kinetic energy:
[math]\text{Kinetic Energy} = \frac{1}{2} \times 610 \, \text{kg} \times (5500 \, \text{m/s})^2 \\
\text{Kinetic Energy} \approx 0.5 \times 610 \, \text{kg} \times 30250000 \, \text{m}^2/\text{s}^2 \\ \text{Kinetic Energy} \approx 9295250000 \, \text{kg} \cdot \text{m}^2/\text{s}^2 [/math]
Rounding to an appropriate number of significant figures: Kinetic Energy [math] ≈ 9.30 × 10^9 J[/math]

Therefore, the kinetic energy of the spacecraft as it enters the atmosphere is approximately [math] 9.30 × 10^9 joules[/math].

kinetic energy =    9.30 x 109 J 

02.2 A parachute opens during the spacecraft’s descent through the atmosphere.

Figure 2 shows the parachute–spacecraft system, with the open parachute displacing the atmospheric gas. This causes the system to decelerate.

Figure 2

Explain, with reference to Newton’s laws of motion, why displacing the atmospheric gas causes a force on the system and why this force causes the system to decelerate.

Explanation:

  1. Newton’s third law: When the parachute displaces atmospheric gas, the gas particles exert an equal and opposite force on the parachute according to Newton’s third law of motion.
  2. Momentum transfer: The collision of the parachute with the gas particles results in a transfer of momentum between them. The gas particles gain momentum due to the force imparted by the parachute.
  3. Change in momentum: The change in momentum (∆p) of the gas particles is given by ∆p = F * ∆t, where F is the force exerted by the parachute and ∆t is the time interval of the collision.
  4.  Force on the parachute: Applying Newton’s second law of motion (F = ∆p/∆t), we find that the change in momentum (∆(mv)) of the gas particles during the collision results in a force (F) being exerted on the parachute.
  5. Equal and opposite forces: Newton’s third law implies that the force exerted by the gas particles on the parachute is equal in magnitude but opposite in direction to the force exerted by the parachute on the gas particles.
  6. Deceleration: As a consequence of the equal and opposite forces, the parachute (part of the system) experiences a force in the opposite direction to its motion, leading to deceleration or a reduction in velocity.
  7. Net force and acceleration: The net force acting on the system is the difference between the forward force of the spacecraft and the opposing drag force. This net force causes the system to decelerate as described by Newton’s second law (F = ma).

In summary,
the collision between the parachute and gas particles results in a force that causes deceleration, as explained by Newton’s third law and the equation for momentum transfer.

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