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University Physics I · unit UPI-11

Angular Momentum

Connect the ideas, make your working visible, and test the result. Use the hints when you need a starting point; open the full solution after your attempt.

Extra challenging questions

A selection from this pathway. Open a topic below for its complete practice and challenge set.

Extra challenging · 01

Angular Momentum of a Particle: infer an input with uncertainty

The angular momentum of a particle about a point O is L = r×p, the cross product of its position vector measured from O with its linear momentum; its magnitude is the momentum times the perpendicular distance from O to the particle's line of motion. Use the supplied topic model Y_out = hypot(s,h), where Y_out is DISTANCE r FROM O (m). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; hypot(a,b) means √(a²+b²). h is Origin offset from the line h, measured in m. Keep s (Particle position along the line s) = -3.3 m; v (Speed v (mass 2.0 kg)) = 2 m s⁻¹ fixed. For this exercise use only -1.18125 m ≤ h ≤ -0.07875 m on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. A reading gives Y_out = 3.338982 m, with a bounded reading uncertainty ±0.0057064 m. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown h by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.00011025 m, using a numerical bracket if required. Find the full input interval consistent with the bounded reading uncertainty and compare it with a symmetric input-error assumption. Do not assume that the supplied calibration points prove monotonicity outside this branch.

Explore the question data

DISTANCE r FROM O against h

Predictions from the supplied Angular Momentum of a Particle model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): DISTANCE r FROM O / m

DISTANCE r FROM O against hPredictions from the supplied Angular Momentum of a Particle model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: h: Origin offset from the line h / m. Vertical axis: DISTANCE r FROM O / m. Exact values are available in the data table below.3.29283.34793.4033.45813.5132-1.225-0.9277-0.63-0.3323-0.03465xy

Horizontal axis (x): h: Origin offset from the line h / m

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1h: Origin offset from the line h / m: -1.181DISTANCE r FROM O / m: 3.505
Read the exact data as a table
DISTANCE r FROM O against h — supplied values
h: Origin offset from the line h / mDISTANCE r FROM O / m
-1.181253.505046584925798
-0.90562499999999993.4220106137510733
-0.62999999999999993.359598190260258
-0.35437499999999993.3189729797973646
-0.078749999999999883.3009394969462864

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

The model's endpoint predictions bracket the reading. Solve Y_out(h) = Y_measured and then solve again at Y_measured − u and Y_measured + u; a nonlinear inverse can give unequal input deviations.

Reveal the worked solution
  1. Endpoint predictions are Y_out(-1.18125) = 3.50505 m and Y_out(-0.07875) = 3.30094 m. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives h_line = -1.18125 + (3.33898 − 3.50505)(-0.07875 − -1.18125)/(3.30094 − 3.50505) = -0.284239 m. This estimates the inverse of the endpoint chord, rather than assuming that chord is the physical model.
  3. Use the actual equation, not the chord, and bracket its root. Evaluating the midpoint and retaining the sign-changing half-interval gives h = -0.508725 m; substituting back gives Y_out = 3.338982 m.
  4. The interpolation error in the input is |h_line − h| = 0.224485 m. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 3.3332756 m and 3.3446884 m. Sort the roots even if the response decreases: -0.544922 m ≤ h ≤ -0.469815 m.
  6. The lower and upper input deviations are 0.0361978 m and 0.0389096 m. They differ because the inverse response is nonlinear; a symmetric error bar would only be a local approximation. This interval includes reading uncertainty only, not model error or uncertainty in fixed inputs.

Answer h ≈ -0.508725 m; compatible interval [-0.544922, -0.469815] m. Endpoint interpolation gives -0.284239 m.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.

Extra challenging · 02

Angular Momentum of a Rigid Body: infer an input with uncertainty

A rigid body's angular momentum is the sum of r × mv over all of its mass; for rotation about a fixed axis, its component along that axis is L_z = Iω, where I = ∫R² dm. Use the supplied topic model Y_out = 2*0.5*a^2*w*sind(theta)*cosd(theta), where Y_out is ACROSS THE AXLE L_⊥ (kg m² s⁻¹). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sind/cosd/tand use degrees. theta is Tilt θ between rod and axle, measured in °. Keep w (Spin rate ω) = 6 rad s⁻¹; a (Half-length a of the rod) = 0.25 m fixed. For this exercise use only 27.4375 ° ≤ theta ≤ 43.975 ° on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. A reading gives Y_out = 0.18115401 kg m² s⁻¹, with a bounded reading uncertainty ±0.0009339 kg m² s⁻¹. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown theta by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.00165375 °, using a numerical bracket if required. Find the full input interval consistent with the bounded reading uncertainty and compare it with a symmetric input-error assumption. Do not assume that the supplied calibration points prove monotonicity outside this branch.

Explore the question data

ACROSS THE AXLE L_⊥ against theta

Predictions from the supplied Angular Momentum of a Rigid Body model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): ACROSS THE AXLE L_⊥ / kg m² s⁻¹

ACROSS THE AXLE L_⊥ against thetaPredictions from the supplied Angular Momentum of a Rigid Body model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: theta: Tilt θ between rod and axle / °. Vertical axis: ACROSS THE AXLE L_⊥ / kg m² s⁻¹. Exact values are available in the data table below.0.1520.16120.17040.17960.188726.7831.2435.7140.1744.64xy

Horizontal axis (x): theta: Tilt θ between rod and axle / °

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1theta: Tilt θ between rod and axle / °: 27.44ACROSS THE AXLE L_⊥ / kg m² s⁻¹: 0.1534
Read the exact data as a table
ACROSS THE AXLE L_⊥ against theta — supplied values
theta: Tilt θ between rod and axle / °ACROSS THE AXLE L_⊥ / kg m² s⁻¹
27.43750.15335601490861786
31.5718750.1672767638218028
35.706250.17771962004632624
39.8406250.18446746356813368
43.9750.18737999829879923

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

The model's endpoint predictions bracket the reading. Solve Y_out(theta) = Y_measured and then solve again at Y_measured − u and Y_measured + u; a nonlinear inverse can give unequal input deviations.

Reveal the worked solution
  1. Endpoint predictions are Y_out(27.4375) = 0.153356 kg m² s⁻¹ and Y_out(43.975) = 0.18738 kg m² s⁻¹. The target lies between them. On the selected branch the response is strictly increasing.
  2. Endpoint interpolation gives theta_line = 27.4375 + (0.181154 − 0.153356)(43.975 − 27.4375)/(0.18738 − 0.153356) = 40.9488 °. This estimates the inverse of the endpoint chord, rather than assuming that chord is the physical model.
  3. Use the actual equation, not the chord, and bracket its root. Evaluating the midpoint and retaining the sign-changing half-interval gives theta = 37.5254 °; substituting back gives Y_out = 0.18115401 kg m² s⁻¹.
  4. The interpolation error in the input is |theta_line − theta| = 3.42345 °. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 0.18022011 kg m² s⁻¹ and 0.18208791 kg m² s⁻¹. Sort the roots even if the response decreases: 36.9909 ° ≤ theta ≤ 38.1001 °.
  6. The lower and upper input deviations are 0.534495 ° and 0.574771 °. They differ because the inverse response is nonlinear; a symmetric error bar would only be a local approximation. This interval includes reading uncertainty only, not model error or uncertainty in fixed inputs.

Answer theta ≈ 37.5254 °; compatible interval [36.9909, 38.1001] °. Endpoint interpolation gives 40.9488 °.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.

Extra challenging · 03

Torque & Angular-Momentum Change: infer an input with uncertainty

The net external torque about a point is the rate at which a system's angular momentum about that same point changes, τ⃗ₑₓₜ = dL⃗/dt, so a torque acting for a time changes L⃗ by the angular impulse ∫τ⃗ dt. Use the supplied topic model Y_out = deg(atan2(((imp*sind(phi)*1000000)/1000000), (spin+imp*cosd(phi)))), where Y_out is L⃗ TURNED BY (before display rounding) (°). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793; sind/cosd/tand use degrees; deg converts radians to degrees; atan2(y,x) is the angle of the vector (x,y), in radians. phi is Angle from L⃗₀ to τ⃗, φ, measured in °. Keep spin (Initial angular momentum L₀) = 4 kg m² s⁻¹; imp (Angular impulse τΔt) = 2 N m s fixed. For this exercise use only 123.075 ° ≤ phi ≤ 160.875 ° on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. A reading gives Y_out = 25.474639 °, with a bounded reading uncertainty ±0.67143 °. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown phi by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.00378 °, using a numerical bracket if required. Find the full input interval consistent with the bounded reading uncertainty and compare it with a symmetric input-error assumption. Do not assume that the supplied calibration points prove monotonicity outside this branch.

Explore the question data

L⃗ TURNED BY (before display rounding) against phi

Predictions from the supplied Torque & Angular-Momentum Change model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): L⃗ TURNED BY (before display rounding) / °

L⃗ TURNED BY (before display rounding) against phiPredictions from the supplied Torque & Angular-Momentum Change model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: phi: Angle from L⃗₀ to τ⃗, φ / °. Vertical axis: L⃗ TURNED BY (before display rounding) / °. Exact values are available in the data table below.16.7420.1723.627.0330.46121.6131.8142152.2162.4xy

Horizontal axis (x): phi: Angle from L⃗₀ to τ⃗, φ / °

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1phi: Angle from L⃗₀ to τ⃗, φ / °: 123.1L⃗ TURNED BY (before display rounding) / °: 29.95
Read the exact data as a table
L⃗ TURNED BY (before display rounding) against phi — supplied values
phi: Angle from L⃗₀ to τ⃗, φ / °L⃗ TURNED BY (before display rounding) / °
123.0749999999999929.950848610670448
132.5249999999999829.100147672077064
141.97526.937264249209097
151.42523.092089752378275
160.87517.249195132642292

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

The model's endpoint predictions bracket the reading. Solve Y_out(phi) = Y_measured and then solve again at Y_measured − u and Y_measured + u; a nonlinear inverse can give unequal input deviations.

Reveal the worked solution
  1. Endpoint predictions are Y_out(123.075) = 29.9508 ° and Y_out(160.875) = 17.2492 °. The target lies between them. On the selected branch the response is strictly decreasing.
  2. Endpoint interpolation gives phi_line = 123.075 + (25.4746 − 29.9508)(160.875 − 123.075)/(17.2492 − 29.9508) = 136.396 °. This estimates the inverse of the endpoint chord, rather than assuming that chord is the physical model.
  3. Use the actual equation, not the chord, and bracket its root. Evaluating the midpoint and retaining the sign-changing half-interval gives phi = 146.133 °; substituting back gives Y_out = 25.474639 °.
  4. The interpolation error in the input is |phi_line − phi| = 9.73684 °. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 24.803209 ° and 26.146069 °. Sort the roots even if the response decreases: 144.344 ° ≤ phi ≤ 147.768 °.
  6. The lower and upper input deviations are 1.7892 ° and 1.63492 °. They differ because the inverse response is nonlinear; a symmetric error bar would only be a local approximation. This interval includes reading uncertainty only, not model error or uncertainty in fixed inputs.

Answer phi ≈ 146.133 °; compatible interval [144.344, 147.768] °. Endpoint interpolation gives 136.396 °.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.

Extra challenging · 04

Conservation of angular momentum: infer an input with uncertainty

Angular momentum is conserved about a point when the net external torque about that point is zero: the system's total L⃗ then keeps its size and direction, however its parts rearrange, collide or grip one another. Use the supplied topic model Y_out = 3*m*d/(0.324+m*d^2), where Y_out is ω JUST AFTER IMPACT (rad s⁻¹). The output symbol Y_out is distinct from all input symbols. ^ denotes a power; π = 3.141592653589793. d is Impact distance d from pivot, measured in m. Keep m (Puck mass m) = 0.4 kg fixed. For this exercise use only 0.185 m ≤ d ≤ 0.815 m on this continuous branch. A grid of test settings is an input restriction for this exercise, not by itself a claim of physical quantisation. This calculation retains the topic model's stated assumptions; it does not extend them to a different physical setup. A reading gives Y_out = 1.5059485 rad s⁻¹, with a bounded reading uncertainty ±0.022883 rad s⁻¹. Treat the model and all fixed inputs as exact for this exercise; the bound is not a standard deviation. First estimate the unknown d by straight-line interpolation between the two endpoint predictions. Then solve the actual model on the stated branch to an absolute input tolerance of 0.000063 m, using a numerical bracket if required. Find the full input interval consistent with the bounded reading uncertainty and compare it with a symmetric input-error assumption. Do not assume that the supplied calibration points prove monotonicity outside this branch.

Explore the question data

ω JUST AFTER IMPACT against d

Predictions from the supplied Conservation of angular momentum model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law.

Vertical axis (y): ω JUST AFTER IMPACT / rad s⁻¹

ω JUST AFTER IMPACT against dPredictions from the supplied Conservation of angular momentum model, with all other inputs fixed as stated in the question. 5 calibration points support a trend comparison; they are not measured data or a straight-line law. Horizontal axis: d: Impact distance d from pivot / m. Vertical axis: ω JUST AFTER IMPACT / rad s⁻¹. Exact values are available in the data table below.0.61740.88771.1581.4281.6990.15980.32990.50.67010.8402xy

Horizontal axis (x): d: Impact distance d from pivot / m

Axes show the supplied calibration interval; the origin may lie outside the plot.

Reading 1d: Impact distance d from pivot / m: 0.185ω JUST AFTER IMPACT / rad s⁻¹: 0.6574
Read the exact data as a table
ω JUST AFTER IMPACT against d — supplied values
d: Impact distance d from pivot / mω JUST AFTER IMPACT / rad s⁻¹
0.1850.6574076816014689
0.342499999999999971.1080481771798691
0.499999999999999941.4150943396226414
0.65751.587772741222223
0.8151.6584985331275754

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

The model's endpoint predictions bracket the reading. Solve Y_out(d) = Y_measured and then solve again at Y_measured − u and Y_measured + u; a nonlinear inverse can give unequal input deviations.

Reveal the worked solution
  1. Endpoint predictions are Y_out(0.185) = 0.657408 rad s⁻¹ and Y_out(0.815) = 1.6585 rad s⁻¹. The target lies between them. On the selected branch the response is strictly increasing.
  2. Endpoint interpolation gives d_line = 0.185 + (1.50595 − 0.657408)(0.815 − 0.185)/(1.6585 − 0.657408) = 0.718998 m. This estimates the inverse of the endpoint chord, rather than assuming that chord is the physical model.
  3. Use the actual equation, not the chord, and bracket its root. Evaluating the midpoint and retaining the sign-changing half-interval gives d = 0.5693 m; substituting back gives Y_out = 1.5059485 rad s⁻¹.
  4. The interpolation error in the input is |d_line − d| = 0.149698 m. This is larger than the requested numerical tolerance.
  5. Invert both limits Y_out = 1.4830655 rad s⁻¹ and 1.5288315 rad s⁻¹. Sort the roots even if the response decreases: 0.549935 m ≤ d ≤ 0.590452 m.
  6. The lower and upper input deviations are 0.0193654 m and 0.0211516 m. They differ because the inverse response is nonlinear; a symmetric error bar would only be a local approximation. This interval includes reading uncertainty only, not model error or uncertainty in fixed inputs.

Answer d ≈ 0.5693 m; compatible interval [0.549935, 0.590452] m. Endpoint interpolation gives 0.718998 m.

Compare the assumptions, method and units with your attempt. Explain any correction before trying another question.

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