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Heat flux The heat flow
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Calculus: Early Transcendentals (2nd Edition)
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- 3. Find the flux of material as a function of r and t and show that at x = 1 the material is tranferred to the right and at x = -1 the material is tranferred to the left.arrow_forwardH1. Consider a point particle with position vector r = (x, y, z) in Cartesian coordinates, moving with a velocity v = (ß, az, -ay), where a and ß are positive constants. (a) What are the physical dimensions of a and B? (b) Find the general form of r(t), the position of the particle, as a function of time t, assuming the initial position of the particle is ro = (0,2,0). (hint: write v = (B, az, -ay) as a system of first order ODEs and note that the equation for x is decoupled from the others). Describe in words the motion of the particle and sketch its trajectory in R3 (you can use software packages for the plot). (c) Show that the speed of the particle is constant, but the acceleration vector a(t) is nonzero. Justify. (d) Assuming the particle has a constant mass m, use Newton's second law to show that the force acting on the particle is (as a function of the position r = = (x, y, z)) F(x, y, z) = ma² (0, -y, —z). H2. Suppose a particle of constant mass m with position x > 0, moves in…arrow_forwardAttached.arrow_forward
- Find the Jacobian for the change of variables defined by x = r cos θ and y = r sin θ.arrow_forwardH1. Consider a point particle with position vector r= (x, y, z) in Cartesian coordinates, moving with a velocity v = (B, az, -ay), where a and ẞ are positive constants. (a) What are the physical dimensions of a and B? (b) Find the general form of r(t), the position of the particle, as a function of time t, assuming the initial position of the particle is ro = (0,2,0). (hint: write v = (B, az, -ay) as a system of first order ODEs and note that the equation for x is decoupled from the others). Describe in words the motion of the particle and sketch its trajectory in R³ (you can use software packages for the plot). (c) Show that the speed of the particle is constant, but the acceleration vector a(t) is nonzero. Justify. (d) Assuming the particle has a constant mass m, use Newton's second law to show that force acting on the particle is (as a function of the position r = (x, y, z)) F(x, y, z) = ma² (0, -y, -z).arrow_forward1.11 please solve it on paperarrow_forward
- Compute the Jacobian for the substitutions x = ρsinφcosϴ, y = ρsinφsinϴ, z = ρcosϴ.arrow_forward+25y²,0, 10- through the surface 3 Find the outward flux of F = =1.arrow_forward1.1: The table below relates to straight conductors moving at constant speeds through uniform magnetic fields .The indicated directions follow a right hand Cartesian coordinate system (a screw turning form x to y advances with z) .Complete the table giving values, as well as directions where applicable. I Ii iii iv V vi Flux density, m T 80(+z) 80(+z) 300(-y) 150(+y) ? 120(+y) Active length, mM 300(y) 300(y) 150(x) 60(z) 250(x) 200(z) Resistance, m2 5 5 8 10 0.8 2.5 Velocity, m/s 1.6(+x) 1.6(-х) 2(-х) ? Current , A 2(-y) 2(-y) 0.5(+z) 12(-х) 4(-z) Induced emf, mV 90(-x) 40(-z) ? terminal voltage, mV ? 105 ? 60 ? Developed force, mN ? 750(+z) ? ? Conversion power, mW ? ? 450 ? 840 ? Copper loss, mW ? Input power .mW 22.5 ? Output power, mW ? ? Action ? ? mot mot Gen ?arrow_forward
- Algebra & Trigonometry with Analytic GeometryAlgebraISBN:9781133382119Author:SwokowskiPublisher:Cengage