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International Baccalaureate · IB Diploma

Physics · SL

Papers, sampel, dan dokumen kurikulum untuk kursus ini.

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Lembar kerja · International Baccalaureate · IB Diploma · Physics · SL (20)
Lembar latihan · International Baccalaureate · IB Diploma · Physics · SL (37)
Salindia presentasi · International Baccalaureate · IB Diploma · Physics · SL (20)
Salindia panduan latihan · International Baccalaureate · IB Diploma · Physics · SL (37)
Panduan pengajaran · International Baccalaureate · IB Diploma · Physics · SL (1)
Lembar kerja · Fisika A-Level (25)
Lembar latihan · Fisika A-Level (106)
Salindia presentasi · Fisika A-Level (25)
Salindia panduan latihan · Fisika A-Level (202)

Unit kursus dan tujuan pembelajaran

Pelajaran ini mengajarkan tujuan kursus tertentu. Periksa kesenjangan cakupan yang tersisa; materi ini bukan program persiapan lengkap.

A.1 · Kinematika
  • Rate of change of displacement.
  • The gradient of a displacement-time graph is velocity. The area under a velocity-time graph gives displacement. A constant-acceleration formula is valid only when its assumption is justified.
  • Choose a positive direction and state it. Use a light gate or video with a known scale and frame interval for repeatable motion measurements. Avoid assuming hand timing is exact over very short intervals.
kecepatan (vektor)
Laju perubahan perpindahan
percepatan
Laju perubahan kecepatan
A.2 · Gaya dan momentum
  • Mass multiplied by velocity.
  • Impulse equals momentum change. Increasing stopping time for the same momentum change reduces average force. Identify external forces before applying momentum conservation.
  • Draw a free-body diagram containing only forces on the selected object. For spring measurements, add loads in steps within the elastic range and measure extension from the unloaded position.
momentum
Mass dikalikan dengan kecepatan
resultan gaya
Jumlah vektor gaya pada suatu benda
A.3 · Usaha, energi dan daya
  • Energy transferred per unit time.
  • Define the system and useful output before calculating efficiency. Doubling speed quadruples kinetic energy at constant mass. Power describes transfer per time, not total energy.
  • Measure a lifting height and load, time the lift, and record electrical input with suitable instruments. Repeat trials and account for heating or friction as transfers, not missing energy.
kuasa
Energi yang dipindahkan per satuan waktu
efisiensi
Output yang berguna dibagi dengan total input
B.1 · Transfer energi termal
  • Energy per mass per temperature rise.
  • Temperature relates to particle motion in a model; internal energy includes kinetic and potential contributions. During a change of state, energy can change particle arrangements rather than temperature.
  • Measure mass, electrical input and temperature change for an insulated block. Ensure the temperature sensor has good contact, allow time for equilibration, and consider energy transferred to the surroundings.
kapasitas panas spesifik
Energi per massa per kenaikan suhu
kalor laten
Energi yang terkait dengan perubahan wujud zat
B.2 · Efek rumah kaca
  • Actions addressing causes of environmental change.
  • Distinguish mitigation, which addresses drivers, from adaptation, which reduces harm from impacts. A policy assessment needs evidence about effectiveness, cost, equity and uncertainty; one criterion is not the entire decision.
  • Compare multi-year data using consistent baselines. State the region, timescale and uncertainty. At HL, connect a management decision to law, economics and ethics rather than treating these lenses as extra definitions only.
mitigasi
Tindakan yang menargetkan penyebab perubahan lingkungan
adaptasi
Tindakan yang mengurangi dampak buruk dari pengaruh lingkungan
B.3 · Hukum gas
  • Temperature on the kelvin scale.
  • At fixed amount and volume, pressure is proportional to kelvin temperature. At fixed temperature and amount, pressure is inversely proportional to volume. State which quantities are fixed before choosing a relationship.
  • Use approved apparatus with a temperature range and pressure limit set by the teacher. Allow thermal equilibrium and record pressure against kelvin temperature. Never heat an improvised sealed vessel.
suhu absolut
Suhu pada skala kelvin
gas ideal
Model gas dengan asumsi penyederhanaan tertentu
B.5 · Arus dan sirkuit
  • Rate of flow of charge.
  • Current is the same through components in series. Potential differences add around the series path. In parallel, branches share the same potential difference, while branch currents sum at a junction.
  • Place an ammeter in series and a voltmeter in parallel. For an I-V investigation, change voltage in steps, reverse polarity when appropriate and limit current to reduce heating.
arus
Tingkat aliran muatan listrik
beda potensial
Energi yang dipindahkan per satuan muatan
C.1 · Gerak Harmonik Sederhana
  • A large response to periodic forcing near a natural frequency.
  • Velocity is greatest near equilibrium for ideal SHM, while acceleration magnitude is greatest at extreme displacement. Resonance can occur near the natural frequency under periodic driving, with amplitude limited by damping.
  • Measure time for several complete oscillations and divide. Define a cycle consistently and use a small displacement when the model requires it. Keep pendulum paths clear and record damping effects rather than assuming perfect motion.
resonansi
Respon besar terhadap pemaksaan periodik di dekat frekuensi alami
redaman
Transfer energi keluar dari sistem bergetar
C.2 · Model gelombang
  • Distance between successive points in phase.
  • At a boundary, frequency stays fixed by the source. A change of speed changes wavelength. Refraction follows from speed differences; angles are measured from the normal.
  • Measure several wavelengths and divide to reduce fractional reading uncertainty. Use a ray box with a normal drawn at the boundary. Keep the beam away from eyes and record incident and refracted angles clearly.
panjang gelombang
Jarak antara titik-titik berurutan dalam fase
frekuensi
Jumlah osilasi per satuan waktu
C.3 · Fenomena gelombang
  • Distance between successive points in phase.
  • At a boundary, frequency stays fixed by the source. A change of speed changes wavelength. Refraction follows from speed differences; angles are measured from the normal.
  • Measure several wavelengths and divide to reduce fractional reading uncertainty. Use a ray box with a normal drawn at the boundary. Keep the beam away from eyes and record incident and refracted angles clearly.
panjang gelombang
Jarak antara titik-titik berurutan dalam fase
frekuensi
Jumlah osilasi per satuan waktu
C.4 · Gelombang diam dan resonansi
  • A large response to periodic forcing near a natural frequency.
  • Velocity is greatest near equilibrium for ideal SHM, while acceleration magnitude is greatest at extreme displacement. Resonance can occur near the natural frequency under periodic driving, with amplitude limited by damping.
  • Measure time for several complete oscillations and divide. Define a cycle consistently and use a small displacement when the model requires it. Keep pendulum paths clear and record damping effects rather than assuming perfect motion.
resonansi
Respon besar terhadap pemaksaan periodik di dekat frekuensi alami
redaman
Transfer energi keluar dari sistem bergetar
C.5 · Efek Doppler
  • Shift of an identified line toward longer wavelength.
  • Compare a identified line with its laboratory rest wavelength. Use z = (observed−rest)/rest, then v approximately cz in the stated low-speed model. Do not apply this approximation without checking the regime or treating a cosmological redshift as a simple exact velocity.
  • Use attributed spectra with calibration and line identification. Compare several lines for a consistent shift. State uncertainty and distinguish relative line-of-sight motion from an unmeasured transverse component.
pergeseran merah
Pergeseran garis yang teridentifikasi menuju panjang gelombang lebih panjang
panjang gelombang diam
Panjang gelombang garis tersebut diukur tanpa adanya gerak relatif sumber
D.1 · Medan Gravitasi
  • A description of gravitational force per unit mass.
  • For a point mass or outside a spherical mass, field strength follows an inverse-square distance dependence. Use distance from the centre, not height above the surface alone.
  • State the circular-orbit approximation and ignore atmospheric drag only when justified. Draw the force toward the central body and velocity tangential to the orbit. Do not add an outward force merely because the path is circular.
medan gravitasi
Deskripsi gaya gravitasi per satuan massa
kekuatan sentripetal
Gaya resultan menuju pusat lintasan melengkung
D.2 · Medan listrik dan magnetik
  • Electric force per unit positive test charge.
  • In a uniform field between ideal parallel plates, E = V/d away from edge effects. The force is F = qE, so its direction reverses for a negative charge. Coulomb force between ideal point charges decreases with separation squared.
  • Sketch labelled plate polarities, field arrows and the charge before calculating. Convert separation to metres. In school, use simulations or approved low-voltage electrostatic models rather than exposed high-voltage equipment.
kekuatan medan listrik
Gaya listrik per satuan muatan uji positif
muatan uji
Muatan kecil yang digunakan untuk meneliti medan listrik
D.3 · Gerak dalam medan elektromagnetik
  • Force due to a magnetic field on a moving charge or current.
  • Equate magnetic force with mv²/r to obtain r = mv/(|q|B) for perpendicular motion. A stronger field makes a smaller radius at fixed momentum. Parallel entry gives zero magnetic force in this model.
  • Draw velocity, field and force as separate arrows using stated into/out-of-page conventions. Use supplied beam data or a simulation. Do not treat a current-carrying wire direction as identical to electron-motion direction.
Gaya magnetik
Gaya akibat medan magnet pada muatan bergerak atau arus listrik
momentum
Massa dikalikan dengan kecepatan dalam model klasik
E.1 · Struktur atom
  • Wavelength pattern of radiation emitted by a source.
  • An emitted photon corresponds to a transition to a lower energy level. Absorption requires a compatible energy difference. Rutherford scattering supported a small dense nucleus, but that experiment alone did not establish the complete quantum model.
  • Read a labelled energy-level diagram before calculating. Keep joules and electronvolts distinct and use the given constants. Compare attributed spectra at a common wavelength scale and avoid looking at unsafe light sources.
spektrum emisi
Pola panjang gelombang radiasi yang dipancarkan oleh sumber
tingkat energi
Keadaan energi yang diizinkan dalam suatu model
E.3 · Peluruhan radioaktif
  • Time for activity or undecayed population to halve.
  • Subtract background counts measured over the same time interval. Distinguish irradiation from contamination. Shielding, distance and reduced exposure time can reduce risk under a school-controlled procedure.
  • Use teacher-managed sources and the school radiation rules. Record count duration and repeat background measurements. Do not extrapolate a half-life from one nucleus or from uncorrected readings.
waktu paruh
Waktu yang dibutuhkan agar aktivitas atau populasi yang tidak terurai menjadi setengahnya
radiasi latar belakang
Radiasi yang diukur terpisah dari sumber yang sedang diteliti
E.4 · Fisi
  • Splitting of a heavy nucleus into lighter nuclei.
  • Separate conservation of nucleon number from conservation of total energy. Released neutrons may initiate further fissions, escape or be absorbed. A controlled reactor and an uncontrolled chain reaction have different neutron-management conditions.
  • Balance a supplied nuclear equation, use the specified mass data and identify the system. Analyse models or published reactor data; this is not a school attempt to produce fission or handle reactor materials.
fisi
Pembelahan inti berat menjadi inti-inti yang lebih ringan
reaksi berantai
Urutan di mana produk memicu peristiwa selanjutnya
E.5 · Fusi dan bintang-bintang
  • Total emitted power.
  • For isotropic emission without absorption, flux follows an inverse-square relationship with distance. Observed brightness alone therefore cannot establish luminosity.
  • Keep distance units consistent, identify which quantities are intrinsic to the star, and distinguish observational evidence from a model of stellar evolution. Do not confuse a red giant stage with every possible final remnant.
luminositas
Total daya yang dipancarkan
fluks
Daya yang diterima per satuan area
Practical · Program eksperimen
  • A quantified limitation on a measured result.
  • For a product or quotient, adding fractional uncertainties is a common maximum-uncertainty approximation. For a difference, add absolute uncertainties. A nonzero intercept can reveal an offset or an incomplete model.
  • Show units on axes and choose a sensible scale. Plot uncertainty bars where justified, draw a best-fit line rather than joining every point, and estimate steepest and shallowest plausible gradients when the course method calls for them.
ketidakpastian
Keterbatasan terkuantifikasi pada hasil pengukuran
kesalahan sistematis
Bias pengukuran yang konsisten

Menyiapkan diri untuk kualifikasi ini

  • Use themes A–E and no old optional-topic model.
  • SL excludes A.4, A.5, B.4, D.4 and E.2. A.2, B.5, C.1/C.3/C.5, D.1/D.2 and E.1/E.3 include additional HL scope.
  • SL Paper 1: 1.5 h, Paper 2: 1.5 h; HL: 2 h, 2.5 h. Papers weigh 36% and 44%; individual investigation 20%, 3,000 words.
  • A clean current Physics data booklet and calculator are available in examinations; the booklet itself remains an acquisition item.
  • Practical work 20 h plus collaborative sciences project 10 h and investigation 10 h.

Cakupan pengajaran masih diperlukan

  • Remaining understandings and guidance in the acquired 2025 Physics guide require complete authored coverage; exclude AHL statements even within mixed topics.
  • All tools/inquiry objectives and data booklet require complete assessment-linked coverage.

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