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The FINITE potential well is a CONCEPT from QUANTUM mechanics. It is an EXTENSION ...

Hello Mate,Joule Law states that the rate of production of heat by a constant direct current is DIRECTLY proportional to the RESISTANCE of the circuit and to the square of the current. the PRINCIPLE that the INTERNAL energy of a given MASS of an ideal gas is solely a function of its temperature....Hope this helps you ☺️✌️❤️

helloExplanation:One-dimensional lattice For simplicity we consider, first, a one-dimensional crystal lattice and ASSUME that the forces between the atoms in this lattice are PROPORTIONAL to relative displacements from the EQUILIBRIUM positions. where M is the mass of the ATOM..hope this helps u ☺️❤️❤️❤️

tion:0.24 VELOCITY TRAVELLED by the trainacceleration does not CHANGE

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a BIG 80.94 HZ a BODY of MENS

The electric potential V is given as a FUNCTION of DISTANCE x by V=5x2+10x−9. The value of electric field at x=1 is. (All quantities are in SI units.)

14m/s......................

The RESULTANT of two vectors A and B SUBTENDS an angle of 45° with either of them. The magnitude of. the resultant is. (a) ZERO.

eeeeeeeeExplanation:STEADY State in Capacitors: When a capacitor is connected to a voltage SUPPLY in an RLC network, it starts out charging and then at some point the voltage across the capacitor remains CONSTANT at a maximum value CONSISTENT with the supply voltage. That state is called a steady-state.hope it is correct and helps u ☺️❤️❤️

tion:Their movement controls by defects.One of defects of usual metal isoscillations of atoms due totemperature. More temperature - moreoscillations - more collisions ofelectrons with atoms - LESS mobilitymore resistivity. ... That is why alloyshave no temperature dependence ofresistivity.Decreasing TemperatureIf you decrease the temperature of afixed amount of gas at constantpressure, the COMBINED gas lawreduces to Charles's law. In this CASE,VOLUME will also decrease.

tion:a SERIES circuit, the OUTPUT current of the first resistor FLOWS into the input of the SECOND resistor; therefore, the current is the same in each resistor. In a parallel circuit, all of the resistor leads on ONE side of the resistors are connected together and all the leads on the other side are connected together.

We know that a×B is VECTOR perpendicular to the plane of a and bTherefore unit vector perpendicular to the plane of a and b = ∣a×b∣a×b Now a×b=(2i−j+K)×(3i+4j−k)= ∣∣∣∣∣∣∣∣ i23 j−14 k1−1 ∣∣∣∣∣∣∣∣ =i(1−4)+j(3+2)+k(8+3)=−3i+5j+11k⇒ unit vector PARALLEL to a×b= ∣a×b∣a×b = (3 2 +5 2 +11 2 ) −3i+5j+11k = 155 −3i+5j+11k

73Explanation:I HOPE this can SOLVE your PROBLEM..The ANS is 73.

The ANSWER is 1/2, INDEPENDENT of MASS

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rk.Good work.Its CORRECTLY DRAWN.

27gExplanation:K. E=1/2mv squareBy rearrangingm=2K.E/vBy PUTTING valuesm=2(135)/10m=27g

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ာာိြနငသို့ခာနူတသသန၈၃ညမာာိာညိညိုျစ၂င၂ညိာျExplanation:ိြု်ုမုုမငါငင်ုတစသသန၈ငိကိပ်ြ်ညို၁သ ငြ်ု၁စ၉၃၈ငယ

how MUCH LONG is UR QUESTION

0Explanation:

Electric potential at a POINT is 1 VOLT SIMPLY means that if SOMEONE wants to move a "1 coloumb" +ve charge from ∞ to that point, we will have to PERFORM a work equal to 1 Joule.

Time taken by a hummingbird to fly 30 miles = 1 hourTime taken by a hummingbird to fly 500 miles to the GULF of MEXICO = = 500 ÷ 30 = 16.666 hours Therefore , a hummingbird TAKES 16.666 hours to fly 500 miles towards the Gulf of Mexico .Hey dear hope you find my answer useful!!

hope it helps... Explanation:Wave–PARTICLE duality is the CONCEPT in quantum mechanics that every particle or quantum entity may be described as either a particle or a wave. It expresses the INABILITY of the classical concepts "particle" or "wave" to fully describe the behaviour of quantum-scale objects.

Because, the FIELD lines spread out in all direction originating from the point in space where the single isolated charge has been KEPT, CLEARLY, since the electric field lines have to be normal to the equipotential surfaces, clearly in THREE DIMENSIONS, this equipotential surface will have a spherical shape.

The SHARPNESS of RESONANCE increases with an INCREASE in damping and decreases with a DECREASE in damping.

열 by the way WHATS this?Explanation:This is the equation for a (non-relativistic) particle of mass m moving along the x axis whileacted by the potential V (x,t) ∈ R. It is clear from this equation that the wavefunction mustbe complex: if it were real, the right-hand side of (1.2) would be real while the left-hand sidewould be imaginary, due to the explicit factor of i.Let us make two important remarks:1 1. The Schr¨odinger equation is a first order differential equation in time. This means that ifwe prescribe the wavefunction Ψ(x,t0) for all of space at an arbitrary initial time t0, thewavefunction is determined for all times.2. The Schr¨odinger equation is a linear equation for Ψ: if Ψ1 and Ψ2 are solutions so isa1Ψ1 + a2Ψ2 with a1 and a2 arbitrary complex numbers.Given a complex number z = a + IB, a, b ∈ R, its complex conjugate is z∗ = a − ib. Let|z| denote the NORM or length of the complex number z. The norm is a positive number (thus√ real!) and it is given by |z| = a2 + b2 . If the norm of a complex number is zero, the complexnumber is zero. You can quickly verify that∗ |z|2 = zz . (1.3)For a wavefunction Ψ(x,t) its complex conjugate (Ψ(x,t))∗ will be usually written as Ψ∗(x,t).We define the probability density P(x,t), also denoted as ρ(x,t), as the norm-squared ofthe wavefunction:P(x,t) = ρ(x,t) ≡ Ψ∗(x,t)Ψ(x,t) = |Ψ(x,t)|2 . (1.4)This probability density so defined is positive. The physical interpretation of the wavefunctionarises because we declare thatP(x,t) dx is the probability to find the particle in the interval [x, x + dx] at time t .(1.5)This interpretation requires a normalized wavefunction, namely, the wavefunction used abovemust satisfy, for all times, ∞dx |Ψ(x,t)|2 = 1 , ∀ t . (1.6) −∞By integrating over space, the left-hand adds up the probabilities that the particle be foundin all of the tiny intervals dx that comprise the real line. Since the particle must be foundsomewhere this sum must be equal to one.Suppose you are handed a wavefunction that is normalized at time t0: ∞dx |Ψ(x,t0)|2 = 1 , ∀ t . (1.7) −∞As mentioned above, knowledge of the wavefunction at one time implies, via the Schr¨odingerequation, knowledge for all times. The Schr¨odinger equation must guarantee that the wavefunction remains normalized for all times. Proving this is a good exercise:2 - - - - - - - - - - - - - - -Exercise 1. Show that the Schr¨odinger equation implies that the norm of the wavefunctiondoes not change in time:d ∞dx |Ψ(x,t)|2 = 0 . (1.8) dt −∞You will have to use both the Schr¨odinger equation and its complex-conjugate version. Moreoveryou will have to use Ψ(x,t) → 0 as |x| → ∞, which is true, as no normalizable wavefunctioncan take a non-zero value as |x| → ∞. While generally the derivative ∂ Ψ also goes to zero as ∂x|x| → ∞ you only need to assume that it remains bounded.Associated to the probability density ρ(x,t) = Ψ∗Ψ there is a probability current J(x,t)that characterizes the flow of probability and is given by∂ΨJ(x,t) = Im Ψ∗ . (1.9) m ∂xThe analogy in electromagnetism is useful. There we have the current density vector Ji and thecharge density ρ. The statement of charge conservation is the differential relation∇ · Ji + ∂ρ = 0 . (1.10) ∂tThis equation applied to a fixed volume V implies that the rate of change of the enclosed chargeQV (t) is only due to the flux of Ji across the surface S that bounds the volume:i dQV i (t) = − J · dia . (1.11) dt SMake sure you know how to get this equation from (1.10)! While the probability current inmore than one spatial dimension is also a vector, in our present one-dimensional case, it hasjust one component. The conservation equation is the analog of (1.10):∂J ∂ρ + = 0 . (1.12) ∂x ∂tYou can check that this equation holds using the above formula for J(x,t), the formula forρ(x,t), and the Schr¨odinger equation. The integral version is formulated by first defining theprobability Pab(t) of finding the particle in the interval x ∈ [a, b]b bPab(t) ≡ dx|Ψ(x,t)|2 = dx ρ(x,t). (1.13) a aYou can then quickly show thatdPab (t) = J(a,t) − J(b,t). (1.14) dt3Z~ Z ZHere J(a,t) denotes the rate at which probability flows in (in units of one over time) at the leftboundary of the interval, while J(b,t) denotes the rate at which probability flows out at theright boundary of the interval.It is SOMETIMES easier to work with wavefunctions that are not normalized. The normalization can be perfomed if needed. We will thus refer to wavefunctions in general without assumingnormalization, otherwise we will call them normalized wavefunction. In this spirit, two wavefunctions Ψ1 and Ψ2 solving the Schr¨odinger equation are DECLARED to be physically equivalentif they differ by multiplication by a complex number. Using the symbol ∼ for equivalence, wewriteΨ1 ∼ Ψ2 ←→ Ψ1(x,t) = α Ψ2(x,t), α ∈ C . (1.15)If the wavefunctions Ψ1 and Ψ2 are normalized they are equivalent if they differ by an overallconstant phase:Normalized wavefunctions: Ψ1 ∼ Ψ2 ←→ Ψ1(x,t) = eiθ Ψ2(x,t), θ ∈ R .

I THINK 2:1 is the ANSWER

: Ohm’s law states that the voltage or potential difference between two points is directly proportional to the current or electricity passing through the resistance, and directly proportional to the resistance of the CIRCUIT. The formula for Ohm’s law is V=IR. This RELATIONSHIP between current, voltage, and relationship was discovered by German scientist Georg Simon Ohm. Let us learn more about Ohms Law, Resistance, and its applications.Explanation: Ohm’s Law DefinitionMost basic components of electricity are voltage, current, and resistance. Ohm’s law shows a simple relation between these three QUANTITIES. Ohm’s law states that the current through a conductor between two points is directly proportional to the voltage across the two points. Ohm’s law states that the voltage or potential difference between two points is directly proportional to the current or electricity passing through the resistance, and directly proportional to the resistance of the circuit. The formula for Ohm’s law is V=IR. This relationship between current, voltage, and relationship was discovered by German scientist Georg Simon Ohm. Let us learn more about Ohms Law, Resistance, and its applications.Ohm’s Law DefinitionMost basic components of electricity are voltage, current, and resistance. Ohm’s law shows a simple relation between these three quantities. Ohm’s law states that the current through a conductor between two points is directly proportional to the voltage across the two points.Ohm’s Law FormulaVoltage= Current× ResistanceV= I×RV= voltage, I= current and R= resistanceThe SI unit of resistance is ohms and is denoted by ΩThis law is one of the most basic LAWS of electricity. It helps to calculate the power, efficiency, current, voltage, and resistance of an element of an electrical circuit.

tion:Step 1Given:mass of person (m) = 60 kg.height of jump (h) = 3.0 m.joints compressed (x) = 0.5 cm. = 0.005 m.Step 2Person stated at height contain potential energy. when he jumps, his potential energy converts into kinetic energy and at floor the kinetic energy becomes ZERO. The work done by floor on knee of person is equal to the kinetic energy.The work done by floor is,Physics homework QUESTION answer, step 2, image 1Angle will be 180 in between FORCE and DISPLACEMENT because force exerted on knee is in upward DIRECTION and direction of displacement is downward.Step 3Change in potential energy will be equal to kinetic energy.Physics homework question answer, step 3, image 1this change in potential energy will be equal to work done.Please mark it as the brainliest

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You can conclude from this that the incident ray the reflected ray and the normal at the point of INCIDENCE LIE in the same PLANE.

tion:lnitial velocity of the OBJECT (u) = 10 m / sMass of the object (m) =2 kg Final velocity (v) = 0 m /s lmpuse = CHANGE in momentum=> J = mv - MU => J = m(v-u)=> J = 2 ( 0 - 10) =>J = 20 Kg m / sSo, the impulse is 20 Kg m/ s.HOPE IT HELPS.

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D. PERFUME in ROOM DIFFUSES FASTEST

The Law of Orbits: All planets MOVE in ELLIPTICAL orbits, with the sun at one focus. 2. The Law of Areas: A line that connects a planet to the sun sweeps out equal areas in equal TIMES. ... The Law of Periods: The square of the period of any planet is proportional to the cube of the SEMIMAJOR axis of its orbit.